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class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Machine Learning">stat.ML</span> </div> </div> <p class="title is-5 mathjax"> Can a Single Tree Outperform an Entire Forest? </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Mao%2C+Q">Qiangqiang Mao</a>, <a href="/search/?searchtype=author&amp;query=Cao%2C+Y">Yankai Cao</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.17003v1-abstract-short" style="display: inline;"> The prevailing mindset is that a single decision tree underperforms classic random forests in testing accuracy, despite its advantages in interpretability and lightweight structure. This study challenges such a mindset by significantly improving the testing accuracy of an oblique regression tree through our gradient-based entire tree optimization framework, making its performance comparable to the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.17003v1-abstract-full').style.display = 'inline'; document.getElementById('2411.17003v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.17003v1-abstract-full" style="display: none;"> The prevailing mindset is that a single decision tree underperforms classic random forests in testing accuracy, despite its advantages in interpretability and lightweight structure. This study challenges such a mindset by significantly improving the testing accuracy of an oblique regression tree through our gradient-based entire tree optimization framework, making its performance comparable to the classic random forest. Our approach reformulates tree training as a differentiable unconstrained optimization task, employing a scaled sigmoid approximation strategy. To ameliorate numerical instability, we propose an algorithmic scheme that solves a sequence of increasingly accurate approximations. Additionally, a subtree polish strategy is implemented to reduce approximation errors accumulated across the tree. Extensive experiments on 16 datasets demonstrate that our optimized tree outperforms the classic random forest by an average of $2.03\%$ improvements in testing accuracy. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.17003v1-abstract-full').style.display = 'none'; document.getElementById('2411.17003v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 25 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.16191">arXiv:2411.16191</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.16191">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Optics">physics.optics</span> </div> </div> <p class="title is-5 mathjax"> Plasmonic Janus particles: A perspective on optical manipulation and biomedical applications </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Koya%2C+A+N">Alemayehu Nana Koya</a>, <a href="/search/?searchtype=author&amp;query=Sapunova%2C+A">Anastasiia Sapunova</a>, <a href="/search/?searchtype=author&amp;query=Sanamreddy%2C+N+R">Nageswar Reddy Sanamreddy</a>, <a href="/search/?searchtype=author&amp;query=Zou%2C+Y">Yanqiu Zou</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qifei Ma</a>, <a href="/search/?searchtype=author&amp;query=Kotsifak%2C+D">Domna Kotsifak</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+H">Huaizhou Jin</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+S">Shangzhong Jin</a>, <a href="/search/?searchtype=author&amp;query=Vavassori%2C+P">Paolo Vavassori</a>, <a href="/search/?searchtype=author&amp;query=Garoli%2C+D">Denis Garoli</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.16191v1-abstract-short" style="display: inline;"> The compositional asymmetry of Janus micro- and nanoparticles gives unprecedented opportunities to manipulate such composite particles with different stimuli to achieve enhanced optical, magnetic and photothermal responses, which can be exploited for sensing, phototherapy, and nanoscale robotic applications. This perspective overviews recent advances in optical manipulation of plasmonic Janus part&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.16191v1-abstract-full').style.display = 'inline'; document.getElementById('2411.16191v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.16191v1-abstract-full" style="display: none;"> The compositional asymmetry of Janus micro- and nanoparticles gives unprecedented opportunities to manipulate such composite particles with different stimuli to achieve enhanced optical, magnetic and photothermal responses, which can be exploited for sensing, phototherapy, and nanoscale robotic applications. This perspective overviews recent advances in optical manipulation of plasmonic Janus particles and their implications for biomedical applications. In particular, a brief summary of optical, plasmonic, and magnetic manipulation of Janus particles of various compositions are presented. Moreover, the potentials of plasmonic and magnetic Janus particles for targeted drug delivery, photothermal therapy, enhanced hyperthermia, and neuromodulation are briefly discussed. Finally, a perspective on the rational design and applications of this particular family of asymmetric particles is forwarded. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.16191v1-abstract-full').style.display = 'none'; document.getElementById('2411.16191v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 25 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.15752">arXiv:2411.15752</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.15752">pdf</a>, <a href="https://arxiv.org/format/2411.15752">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Measurement of cross sections of $e^+e^-\to K^0_S K^0_S 蠄(3686)$ from $\sqrt{s}=$ 4.682 to 4.951 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (642 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.15752v1-abstract-short" style="display: inline;"> The process $e^+e^-\to K^0_S K^0_S 蠄(3686)$ is studied by analyzing $e^+e^-$ collision data samples collected at eight center-of-mass energies ranging from 4.682 to 4.951 GeV with the BESIII detector operating at the BEPCII collider, corresponding to an integrated luminosity of $4.1~{\rm fb}^{-1}$. Observation of the $e^+e^-\to K^0_S K^0_S 蠄(3686)$ process is found for the first time with a statis&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.15752v1-abstract-full').style.display = 'inline'; document.getElementById('2411.15752v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.15752v1-abstract-full" style="display: none;"> The process $e^+e^-\to K^0_S K^0_S 蠄(3686)$ is studied by analyzing $e^+e^-$ collision data samples collected at eight center-of-mass energies ranging from 4.682 to 4.951 GeV with the BESIII detector operating at the BEPCII collider, corresponding to an integrated luminosity of $4.1~{\rm fb}^{-1}$. Observation of the $e^+e^-\to K^0_S K^0_S 蠄(3686)$ process is found for the first time with a statistical significance of $6.3蟽$, and the cross sections at each center-of-mass energy are measured. The ratio of cross sections of $e^+e^-\to K_S^0 K_S^0 蠄(3686)$ relative to $e^+e^-\to K^+ K^- 蠄(3686)$ is determined to be $\frac{蟽(e^+e^-\to K_S^0 K_S^0 蠄(3686))}{蟽(e^+e^-\to K^+ K^- 蠄(3686))}=0.45 \pm 0.25$, which is consistent with the prediction based on isospin symmetry. The uncertainty includes both statistical and systematic contributions. Additionally, the $K_S^0蠄(3686)$ invariant mass distribution is found to be consistent with three-body phase space. The significance of a contribution beyond three-body phase space is only $0.8蟽$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.15752v1-abstract-full').style.display = 'none'; document.getElementById('2411.15752v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.15737">arXiv:2411.15737</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.15737">pdf</a>, <a href="https://arxiv.org/format/2411.15737">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Artificial Intelligence">cs.AI</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Computation and Language">cs.CL</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Machine Learning">cs.LG</span> </div> </div> <p class="title is-5 mathjax"> TableTime: Reformulating Time Series Classification as Zero-Shot Table Understanding via Large Language Models </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Wang%2C+J">Jiahao Wang</a>, <a href="/search/?searchtype=author&amp;query=Cheng%2C+M">Mingyue Cheng</a>, <a href="/search/?searchtype=author&amp;query=Mao%2C+Q">Qingyang Mao</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+Q">Qi Liu</a>, <a href="/search/?searchtype=author&amp;query=Xu%2C+F">Feiyang Xu</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+X">Xin Li</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+E">Enhong Chen</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.15737v1-abstract-short" style="display: inline;"> Large language models (LLMs) have demonstrated their effectiveness in multivariate time series classification (MTSC). Effective adaptation of LLMs for MTSC necessitates informative data representations. Existing LLM-based methods directly encode embeddings for time series within the latent space of LLMs from scratch to align with semantic space of LLMs. Despite their effectiveness, we reveal that&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.15737v1-abstract-full').style.display = 'inline'; document.getElementById('2411.15737v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.15737v1-abstract-full" style="display: none;"> Large language models (LLMs) have demonstrated their effectiveness in multivariate time series classification (MTSC). Effective adaptation of LLMs for MTSC necessitates informative data representations. Existing LLM-based methods directly encode embeddings for time series within the latent space of LLMs from scratch to align with semantic space of LLMs. Despite their effectiveness, we reveal that these methods conceal three inherent bottlenecks: (1) they struggle to encode temporal and channel-specific information in a lossless manner, both of which are critical components of multivariate time series; (2) it is much difficult to align the learned representation space with the semantic space of the LLMs; (3) they require task-specific retraining, which is both computationally expensive and labor-intensive. To bridge these gaps, we propose TableTime, which reformulates MTSC as a table understanding task. Specifically, TableTime introduces the following strategies: (1) convert multivariate time series into a tabular form, thus minimizing information loss to the greatest extent; (2) represent tabular time series in text format to achieve natural alignment with the semantic space of LLMs; (3) design a reasoning framework that integrates contextual text information, neighborhood assistance, multi-path inference and problem decomposition to enhance the reasoning ability of LLMs and realize zero-shot classification. Extensive experiments performed on 10 publicly representative datasets from UEA archive verify the superiorities of the TableTime. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.15737v1-abstract-full').style.display = 'none'; document.getElementById('2411.15737v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.14718">arXiv:2411.14718</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.14718">pdf</a>, <a href="https://arxiv.org/format/2411.14718">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Cryptography and Security">cs.CR</span> </div> </div> <p class="title is-5 mathjax"> GraphTheft: Quantifying Privacy Risks in Graph Prompt Learning </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Zhu%2C+J">Jiani Zhu</a>, <a href="/search/?searchtype=author&amp;query=Lin%2C+X">Xi Lin</a>, <a href="/search/?searchtype=author&amp;query=Qi%2C+Y">Yuxin Qi</a>, <a href="/search/?searchtype=author&amp;query=Mao%2C+Q">Qinghua Mao</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.14718v1-abstract-short" style="display: inline;"> Graph Prompt Learning (GPL) represents an innovative approach in graph representation learning, enabling task-specific adaptations by fine-tuning prompts without altering the underlying pre-trained model. Despite its growing prominence, the privacy risks inherent in GPL remain unexplored. In this study, we provide the first evaluation of privacy leakage in GPL across three attacker capabilities: b&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.14718v1-abstract-full').style.display = 'inline'; document.getElementById('2411.14718v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.14718v1-abstract-full" style="display: none;"> Graph Prompt Learning (GPL) represents an innovative approach in graph representation learning, enabling task-specific adaptations by fine-tuning prompts without altering the underlying pre-trained model. Despite its growing prominence, the privacy risks inherent in GPL remain unexplored. In this study, we provide the first evaluation of privacy leakage in GPL across three attacker capabilities: black-box attacks when GPL as a service, and scenarios where node embeddings and prompt representations are accessible to third parties. We assess GPL&#39;s privacy vulnerabilities through Attribute Inference Attacks (AIAs) and Link Inference Attacks (LIAs), finding that under any capability, attackers can effectively infer the properties and relationships of sensitive nodes, and the success rate of inference on some data sets is as high as 98%. Importantly, while targeted inference attacks on specific prompts (e.g., GPF-plus) maintain high success rates, our analysis suggests that the prompt-tuning in GPL does not significantly elevate privacy risks compared to traditional GNNs. To mitigate these risks, we explored defense mechanisms, identifying that Laplacian noise perturbation can substantially reduce inference success, though balancing privacy protection with model performance remains challenging. This work highlights critical privacy risks in GPL, offering new insights and foundational directions for future privacy-preserving strategies in graph learning. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.14718v1-abstract-full').style.display = 'none'; document.getElementById('2411.14718v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 21 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.14205">arXiv:2411.14205</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.14205">pdf</a>, <a href="https://arxiv.org/format/2411.14205">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Artificial Intelligence">cs.AI</span> </div> </div> <p class="title is-5 mathjax"> Is this Generated Person Existed in Real-world? Fine-grained Detecting and Calibrating Abnormal Human-body </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Wang%2C+Z">Zeqing Wang</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qingyang Ma</a>, <a href="/search/?searchtype=author&amp;query=Wan%2C+W">Wentao Wan</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+H">Haojie Li</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+K">Keze Wang</a>, <a href="/search/?searchtype=author&amp;query=Tian%2C+Y">Yonghong Tian</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.14205v1-abstract-short" style="display: inline;"> Recent improvements in visual synthesis have significantly enhanced the depiction of generated human photos, which are pivotal due to their wide applicability and demand. Nonetheless, the existing text-to-image or text-to-video models often generate low-quality human photos that might differ considerably from real-world body structures, referred to as &#34;abnormal human bodies&#34;. Such abnormalities, t&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.14205v1-abstract-full').style.display = 'inline'; document.getElementById('2411.14205v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.14205v1-abstract-full" style="display: none;"> Recent improvements in visual synthesis have significantly enhanced the depiction of generated human photos, which are pivotal due to their wide applicability and demand. Nonetheless, the existing text-to-image or text-to-video models often generate low-quality human photos that might differ considerably from real-world body structures, referred to as &#34;abnormal human bodies&#34;. Such abnormalities, typically deemed unacceptable, pose considerable challenges in the detection and repair of them within human photos. These challenges require precise abnormality recognition capabilities, which entail pinpointing both the location and the abnormality type. Intuitively, Visual Language Models (VLMs) that have obtained remarkable performance on various visual tasks are quite suitable for this task. However, their performance on abnormality detection in human photos is quite poor. Hence, it is quite important to highlight this task for the research community. In this paper, we first introduce a simple yet challenging task, i.e., \textbf{F}ine-grained \textbf{H}uman-body \textbf{A}bnormality \textbf{D}etection \textbf{(FHAD)}, and construct two high-quality datasets for evaluation. Then, we propose a meticulous framework, named HumanCalibrator, which identifies and repairs abnormalities in human body structures while preserving the other content. Experiments indicate that our HumanCalibrator achieves high accuracy in abnormality detection and accomplishes an increase in visual comparisons while preserving the other visual content. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.14205v1-abstract-full').style.display = 'none'; document.getElementById('2411.14205v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 21 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">16 pages, 14 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.13865">arXiv:2411.13865</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.13865">pdf</a>, <a href="https://arxiv.org/format/2411.13865">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Information Retrieval">cs.IR</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Artificial Intelligence">cs.AI</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Computation and Language">cs.CL</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Machine Learning">cs.LG</span> </div> </div> <p class="title is-5 mathjax"> HARec: Hyperbolic Graph-LLM Alignment for Exploration and Exploitation in Recommender Systems </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qiyao Ma</a>, <a href="/search/?searchtype=author&amp;query=Yang%2C+M">Menglin Yang</a>, <a href="/search/?searchtype=author&amp;query=Ju%2C+M">Mingxuan Ju</a>, <a href="/search/?searchtype=author&amp;query=Zhao%2C+T">Tong Zhao</a>, <a href="/search/?searchtype=author&amp;query=Shah%2C+N">Neil Shah</a>, <a href="/search/?searchtype=author&amp;query=Ying%2C+R">Rex Ying</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.13865v1-abstract-short" style="display: inline;"> Modern recommendation systems often create information cocoons, limiting users&#39; exposure to diverse content. To enhance user experience, a crucial challenge is developing systems that can balance content exploration and exploitation, allowing users to adjust their recommendation preferences. Intuitively, this balance can be achieved through a tree-structured representation, where depth search faci&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.13865v1-abstract-full').style.display = 'inline'; document.getElementById('2411.13865v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.13865v1-abstract-full" style="display: none;"> Modern recommendation systems often create information cocoons, limiting users&#39; exposure to diverse content. To enhance user experience, a crucial challenge is developing systems that can balance content exploration and exploitation, allowing users to adjust their recommendation preferences. Intuitively, this balance can be achieved through a tree-structured representation, where depth search facilitates exploitation and breadth search enables exploration. However, current works face two challenges to achieve this target: (1) Euclidean methods fail to fully capture hierarchical structures and lack flexibility in balancing exploration-exploitation, while (2) hyperbolic approaches, despite better hierarchical modeling, suffer from insufficient semantic alignment due to their reliance on Euclidean text encoders. To address these challenges, we propose HARec, a hyperbolic representation learning framework that jointly aligns user-item collaborative information with textual descriptions in hyperbolic space. Our framework introduces two key technique novelty: (1) a hierarchical-aware graph-llm alignment mechanism that enables better hierarchical representation, and (2) a hyperbolic hierarchical tree structure that facilitates user-adjustable exploration-exploitation trade-offs. Extensive experiments demonstrate that HARec consistently outperforms both Euclidean and hyperbolic baselines, achieving up to 5.49% improvement in utility metrics and 11.39% increase in diversity metrics. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.13865v1-abstract-full').style.display = 'none'; document.getElementById('2411.13865v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 21 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.13503">arXiv:2411.13503</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.13503">pdf</a>, <a href="https://arxiv.org/format/2411.13503">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> </div> </div> <p class="title is-5 mathjax"> VBench++: Comprehensive and Versatile Benchmark Suite for Video Generative Models </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Huang%2C+Z">Ziqi Huang</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+F">Fan Zhang</a>, <a href="/search/?searchtype=author&amp;query=Xu%2C+X">Xiaojie Xu</a>, <a href="/search/?searchtype=author&amp;query=He%2C+Y">Yinan He</a>, <a href="/search/?searchtype=author&amp;query=Yu%2C+J">Jiashuo Yu</a>, <a href="/search/?searchtype=author&amp;query=Dong%2C+Z">Ziyue Dong</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qianli Ma</a>, <a href="/search/?searchtype=author&amp;query=Chanpaisit%2C+N">Nattapol Chanpaisit</a>, <a href="/search/?searchtype=author&amp;query=Si%2C+C">Chenyang Si</a>, <a href="/search/?searchtype=author&amp;query=Jiang%2C+Y">Yuming Jiang</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+Y">Yaohui Wang</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+X">Xinyuan Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+Y">Ying-Cong Chen</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+L">Limin Wang</a>, <a href="/search/?searchtype=author&amp;query=Lin%2C+D">Dahua Lin</a>, <a href="/search/?searchtype=author&amp;query=Qiao%2C+Y">Yu Qiao</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+Z">Ziwei Liu</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.13503v1-abstract-short" style="display: inline;"> Video generation has witnessed significant advancements, yet evaluating these models remains a challenge. A comprehensive evaluation benchmark for video generation is indispensable for two reasons: 1) Existing metrics do not fully align with human perceptions; 2) An ideal evaluation system should provide insights to inform future developments of video generation. To this end, we present VBench, a&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.13503v1-abstract-full').style.display = 'inline'; document.getElementById('2411.13503v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.13503v1-abstract-full" style="display: none;"> Video generation has witnessed significant advancements, yet evaluating these models remains a challenge. A comprehensive evaluation benchmark for video generation is indispensable for two reasons: 1) Existing metrics do not fully align with human perceptions; 2) An ideal evaluation system should provide insights to inform future developments of video generation. To this end, we present VBench, a comprehensive benchmark suite that dissects &#34;video generation quality&#34; into specific, hierarchical, and disentangled dimensions, each with tailored prompts and evaluation methods. VBench has several appealing properties: 1) Comprehensive Dimensions: VBench comprises 16 dimensions in video generation (e.g., subject identity inconsistency, motion smoothness, temporal flickering, and spatial relationship, etc). The evaluation metrics with fine-grained levels reveal individual models&#39; strengths and weaknesses. 2) Human Alignment: We also provide a dataset of human preference annotations to validate our benchmarks&#39; alignment with human perception, for each evaluation dimension respectively. 3) Valuable Insights: We look into current models&#39; ability across various evaluation dimensions, and various content types. We also investigate the gaps between video and image generation models. 4) Versatile Benchmarking: VBench++ supports evaluating text-to-video and image-to-video. We introduce a high-quality Image Suite with an adaptive aspect ratio to enable fair evaluations across different image-to-video generation settings. Beyond assessing technical quality, VBench++ evaluates the trustworthiness of video generative models, providing a more holistic view of model performance. 5) Full Open-Sourcing: We fully open-source VBench++ and continually add new video generation models to our leaderboard to drive forward the field of video generation. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.13503v1-abstract-full').style.display = 'none'; document.getElementById('2411.13503v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 20 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Leaderboard: https://huggingface.co/spaces/Vchitect/VBench_Leaderboard Code: https://github.com/Vchitect/VBench Project page: https://vchitect.github.io/VBench-project/ extension of arXiv:2311.17982. arXiv admin note: substantial text overlap with arXiv:2311.17982</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.12302">arXiv:2411.12302</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.12302">pdf</a>, <a href="https://arxiv.org/ps/2411.12302">ps</a>, <a href="https://arxiv.org/format/2411.12302">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Dynamical Systems">math.DS</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Number Theory">math.NT</span> </div> </div> <p class="title is-5 mathjax"> Arithmetic unique ergodicity for infinite dimensional flat bundles </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qiaochu Ma</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.12302v1-abstract-short" style="display: inline;"> In this paper, we prove a uniform version of quantum unique ergodicity for high-frequency eigensections of a certain series of unitary flat bundles over arithmetic surfaces. </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.12302v1-abstract-full" style="display: none;"> In this paper, we prove a uniform version of quantum unique ergodicity for high-frequency eigensections of a certain series of unitary flat bundles over arithmetic surfaces. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.12302v1-abstract-full').style.display = 'none'; document.getElementById('2411.12302v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">17 pages, Comments are welcome!</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.11648">arXiv:2411.11648</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.11648">pdf</a>, <a href="https://arxiv.org/ps/2411.11648">ps</a>, <a href="https://arxiv.org/format/2411.11648">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> </div> </div> <p class="title is-5 mathjax"> Evidence for Two Excited $惟^{-}$ Hyperons </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (650 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.11648v1-abstract-short" style="display: inline;"> Using $e^+e^-$ collision data corresponding to an integrated luminosity of 19 fb$^{-1}$ collected by the BESIII detector at center-of-mass energies ranging from 4.13 to 4.70 GeV, we report the first evidence for a new excited $惟^{-}$ hyperon, the $惟^*(2109)^{-}$, through the process $e^+ e^- \to 惟^*(2109)^{-} \bar惟^{+} +c.c.$ with a significance of 3.7 $蟽$. The mass and width of $惟^*(2109)^{-}$ ar&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.11648v1-abstract-full').style.display = 'inline'; document.getElementById('2411.11648v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.11648v1-abstract-full" style="display: none;"> Using $e^+e^-$ collision data corresponding to an integrated luminosity of 19 fb$^{-1}$ collected by the BESIII detector at center-of-mass energies ranging from 4.13 to 4.70 GeV, we report the first evidence for a new excited $惟^{-}$ hyperon, the $惟^*(2109)^{-}$, through the process $e^+ e^- \to 惟^*(2109)^{-} \bar惟^{+} +c.c.$ with a significance of 3.7 $蟽$. The mass and width of $惟^*(2109)^{-}$ are measured to be $2108.8 \pm 5.5_{\rm stat} \pm 1.5_{\rm syst} {\rm MeV}/c^{2}$ and $21.6 \pm 17.7_{\rm stat} \pm 9.4_{\rm syst} {\rm MeV}$, respectively. We also present evidence for production of the $惟^*(2012)^{-}$ in the process $e^+ e^- \to 惟^*(2012)^{-} \bar惟^{+} +c.c.$ with a significance of 3.7 $蟽$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.11648v1-abstract-full').style.display = 'none'; document.getElementById('2411.11648v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 18 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">8 pages, 2 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.10321">arXiv:2411.10321</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.10321">pdf</a>, <a href="https://arxiv.org/format/2411.10321">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> </div> </div> <p class="title is-5 mathjax"> Probabilistic Prior Driven Attention Mechanism Based on Diffusion Model for Imaging Through Atmospheric Turbulence </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Sun%2C+G">Guodong Sun</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qixiang Ma</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+L">Liqiang Zhang</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+H">Hongwei Wang</a>, <a href="/search/?searchtype=author&amp;query=Gao%2C+Z">Zixuan Gao</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+H">Haotian Zhang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.10321v1-abstract-short" style="display: inline;"> Atmospheric turbulence introduces severe spatial and geometric distortions, challenging traditional image restoration methods. We propose the Probabilistic Prior Turbulence Removal Network (PPTRN), which combines probabilistic diffusion-based prior modeling with Transformer-driven feature extraction to address this issue. PPTRN employs a two-stage approach: first, a latent encoder and Transformer&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.10321v1-abstract-full').style.display = 'inline'; document.getElementById('2411.10321v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.10321v1-abstract-full" style="display: none;"> Atmospheric turbulence introduces severe spatial and geometric distortions, challenging traditional image restoration methods. We propose the Probabilistic Prior Turbulence Removal Network (PPTRN), which combines probabilistic diffusion-based prior modeling with Transformer-driven feature extraction to address this issue. PPTRN employs a two-stage approach: first, a latent encoder and Transformer are jointly trained on clear images to establish robust feature representations. Then, a Denoising Diffusion Probabilistic Model (DDPM) models prior distributions over latent vectors, guiding the Transformer in capturing diverse feature variations essential for restoration. A key innovation in PPTRN is the Probabilistic Prior Driven Cross Attention mechanism, which integrates the DDPM-generated prior with feature embeddings to reduce artifacts and enhance spatial coherence. Extensive experiments validate that PPTRN significantly improves restoration quality on turbulence-degraded images, setting a new benchmark in clarity and structural fidelity. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.10321v1-abstract-full').style.display = 'none'; document.getElementById('2411.10321v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 15 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.09245">arXiv:2411.09245</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.09245">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Optics">physics.optics</span> </div> </div> <p class="title is-5 mathjax"> Application of Optical Tweezers in the Study of Emulsions for Multiple Applications </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qifei Ma</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+H">Huaizhou Jin</a>, <a href="/search/?searchtype=author&amp;query=Shang%2C+X">Xiaoxiao Shang</a>, <a href="/search/?searchtype=author&amp;query=Pardy%2C+T">Tamas Pardy</a>, <a href="/search/?searchtype=author&amp;query=Scheler%2C+O">Ott Scheler</a>, <a href="/search/?searchtype=author&amp;query=Bartkova%2C+S">Simona Bartkova</a>, <a href="/search/?searchtype=author&amp;query=Cojoc%2C+D">Dan Cojoc</a>, <a href="/search/?searchtype=author&amp;query=Garoli%2C+D">Denis Garoli</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+S">Shangzhong Jin</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.09245v1-abstract-short" style="display: inline;"> Emulsions are ubiquitous in everyday life and find applications in various industries. Optical tweezers (OTs) have emerged as the preferred method for studying emulsion dynamics. In this review, we first introduce the theory of optical trapping and emulsion stability. We then survey applications in the manipulation of emulsions, stability mechanism, the processes of aggregation and coalescence, an&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.09245v1-abstract-full').style.display = 'inline'; document.getElementById('2411.09245v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.09245v1-abstract-full" style="display: none;"> Emulsions are ubiquitous in everyday life and find applications in various industries. Optical tweezers (OTs) have emerged as the preferred method for studying emulsion dynamics. In this review, we first introduce the theory of optical trapping and emulsion stability. We then survey applications in the manipulation of emulsions, stability mechanism, the processes of aggregation and coalescence, and important responsive and switchable behaviors. And we overview the instrumentation framework of various OT setups, and evaluate their complexity and cost with a view towards the democratization of this technology. Following this, we delve into basic experimentation methods, the challenges associated with using OTs in emulsion applications. Additionally, we present a promising research outlook, including studies on stability mechanism of emulsions stabilized by compound or mixed emulsifiers or rigid or soft particles, as well as dynamic processes of responsive or functional emulsions. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.09245v1-abstract-full').style.display = 'none'; document.getElementById('2411.09245v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.07730">arXiv:2411.07730</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.07730">pdf</a>, <a href="https://arxiv.org/ps/2411.07730">ps</a>, <a href="https://arxiv.org/format/2411.07730">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Study of the light scalar $a_{0}(980)$ through the decay $D^{0} \to a_{0}(980)^-e^{+} 谓_{e}$ with $a_{0}(980)^- \to 畏蟺^-$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (649 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.07730v1-abstract-short" style="display: inline;"> Using 7.93 ${\rm fb^{-1}}$ of $e^+e^-$ collision data collected at a center-of-mass energy of 3.773 ${\rm GeV}$ with the BESIII detector, we present an analysis of the decay $D^{0} \to 畏蟺^- e^+ 谓_{e}$. The branching fraction of the decay $D^{0} \to a_{0}(980)^{-} e^+ 谓_{e}$ with $a_{0}(980)^{-} \to 畏蟺^{-}$ is measured to be $(0.86\pm0.17_{\text{stat}}\pm0.05_{\text{syst}})\times 10^{-4}$. The deca&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.07730v1-abstract-full').style.display = 'inline'; document.getElementById('2411.07730v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.07730v1-abstract-full" style="display: none;"> Using 7.93 ${\rm fb^{-1}}$ of $e^+e^-$ collision data collected at a center-of-mass energy of 3.773 ${\rm GeV}$ with the BESIII detector, we present an analysis of the decay $D^{0} \to 畏蟺^- e^+ 谓_{e}$. The branching fraction of the decay $D^{0} \to a_{0}(980)^{-} e^+ 谓_{e}$ with $a_{0}(980)^{-} \to 畏蟺^{-}$ is measured to be $(0.86\pm0.17_{\text{stat}}\pm0.05_{\text{syst}})\times 10^{-4}$. The decay dynamics of this process is studied with a single-pole parameterization of the hadronic form factor and the Flatt茅 formula describing the $a_0(980)$ line shape in the differential decay rate. The product of the form factor $f^{ a_0}_{+}(0)$ and the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cd}|$ is determined for the first time with the result $f^{ a_0}_+(0)|V_{cd}|=0.126\pm0.013_{\rm stat}\pm0.003_{\rm syst}$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.07730v1-abstract-full').style.display = 'none'; document.getElementById('2411.07730v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 12 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.07135">arXiv:2411.07135</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.07135">pdf</a>, <a href="https://arxiv.org/format/2411.07135">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Artificial Intelligence">cs.AI</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Graphics">cs.GR</span> </div> </div> <p class="title is-5 mathjax"> Edify 3D: Scalable High-Quality 3D Asset Generation </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=NVIDIA"> NVIDIA</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Bala%2C+M">Maciej Bala</a>, <a href="/search/?searchtype=author&amp;query=Cui%2C+Y">Yin Cui</a>, <a href="/search/?searchtype=author&amp;query=Ding%2C+Y">Yifan Ding</a>, <a href="/search/?searchtype=author&amp;query=Ge%2C+Y">Yunhao Ge</a>, <a href="/search/?searchtype=author&amp;query=Hao%2C+Z">Zekun Hao</a>, <a href="/search/?searchtype=author&amp;query=Hasselgren%2C+J">Jon Hasselgren</a>, <a href="/search/?searchtype=author&amp;query=Huffman%2C+J">Jacob Huffman</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+J">Jingyi Jin</a>, <a href="/search/?searchtype=author&amp;query=Lewis%2C+J+P">J. P. Lewis</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+Z">Zhaoshuo Li</a>, <a href="/search/?searchtype=author&amp;query=Lin%2C+C">Chen-Hsuan Lin</a>, <a href="/search/?searchtype=author&amp;query=Lin%2C+Y">Yen-Chen Lin</a>, <a href="/search/?searchtype=author&amp;query=Lin%2C+T">Tsung-Yi Lin</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+M">Ming-Yu Liu</a>, <a href="/search/?searchtype=author&amp;query=Luo%2C+A">Alice Luo</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qianli Ma</a>, <a href="/search/?searchtype=author&amp;query=Munkberg%2C+J">Jacob Munkberg</a>, <a href="/search/?searchtype=author&amp;query=Shi%2C+S">Stella Shi</a>, <a href="/search/?searchtype=author&amp;query=Wei%2C+F">Fangyin Wei</a>, <a href="/search/?searchtype=author&amp;query=Xiang%2C+D">Donglai Xiang</a>, <a href="/search/?searchtype=author&amp;query=Xu%2C+J">Jiashu Xu</a>, <a href="/search/?searchtype=author&amp;query=Zeng%2C+X">Xiaohui Zeng</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+Q">Qinsheng Zhang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.07135v1-abstract-short" style="display: inline;"> We introduce Edify 3D, an advanced solution designed for high-quality 3D asset generation. Our method first synthesizes RGB and surface normal images of the described object at multiple viewpoints using a diffusion model. The multi-view observations are then used to reconstruct the shape, texture, and PBR materials of the object. Our method can generate high-quality 3D assets with detailed geometr&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.07135v1-abstract-full').style.display = 'inline'; document.getElementById('2411.07135v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.07135v1-abstract-full" style="display: none;"> We introduce Edify 3D, an advanced solution designed for high-quality 3D asset generation. Our method first synthesizes RGB and surface normal images of the described object at multiple viewpoints using a diffusion model. The multi-view observations are then used to reconstruct the shape, texture, and PBR materials of the object. Our method can generate high-quality 3D assets with detailed geometry, clean shape topologies, high-resolution textures, and materials within 2 minutes of runtime. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.07135v1-abstract-full').style.display = 'none'; document.getElementById('2411.07135v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 11 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Project website: https://research.nvidia.com/labs/dir/edify-3d</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.07126">arXiv:2411.07126</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.07126">pdf</a>, <a href="https://arxiv.org/format/2411.07126">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Machine Learning">cs.LG</span> </div> </div> <p class="title is-5 mathjax"> Edify Image: High-Quality Image Generation with Pixel Space Laplacian Diffusion Models </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=NVIDIA"> NVIDIA</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Atzmon%2C+Y">Yuval Atzmon</a>, <a href="/search/?searchtype=author&amp;query=Bala%2C+M">Maciej Bala</a>, <a href="/search/?searchtype=author&amp;query=Balaji%2C+Y">Yogesh Balaji</a>, <a href="/search/?searchtype=author&amp;query=Cai%2C+T">Tiffany Cai</a>, <a href="/search/?searchtype=author&amp;query=Cui%2C+Y">Yin Cui</a>, <a href="/search/?searchtype=author&amp;query=Fan%2C+J">Jiaojiao Fan</a>, <a href="/search/?searchtype=author&amp;query=Ge%2C+Y">Yunhao Ge</a>, <a href="/search/?searchtype=author&amp;query=Gururani%2C+S">Siddharth Gururani</a>, <a href="/search/?searchtype=author&amp;query=Huffman%2C+J">Jacob Huffman</a>, <a href="/search/?searchtype=author&amp;query=Isaac%2C+R">Ronald Isaac</a>, <a href="/search/?searchtype=author&amp;query=Jannaty%2C+P">Pooya Jannaty</a>, <a href="/search/?searchtype=author&amp;query=Karras%2C+T">Tero Karras</a>, <a href="/search/?searchtype=author&amp;query=Lam%2C+G">Grace Lam</a>, <a href="/search/?searchtype=author&amp;query=Lewis%2C+J+P">J. P. Lewis</a>, <a href="/search/?searchtype=author&amp;query=Licata%2C+A">Aaron Licata</a>, <a href="/search/?searchtype=author&amp;query=Lin%2C+Y">Yen-Chen Lin</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+M">Ming-Yu Liu</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qianli Ma</a>, <a href="/search/?searchtype=author&amp;query=Mallya%2C+A">Arun Mallya</a>, <a href="/search/?searchtype=author&amp;query=Martino-Tarr%2C+A">Ashlee Martino-Tarr</a>, <a href="/search/?searchtype=author&amp;query=Mendez%2C+D">Doug Mendez</a>, <a href="/search/?searchtype=author&amp;query=Nah%2C+S">Seungjun Nah</a>, <a href="/search/?searchtype=author&amp;query=Pruett%2C+C">Chris Pruett</a> , et al. (7 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.07126v1-abstract-short" style="display: inline;"> We introduce Edify Image, a family of diffusion models capable of generating photorealistic image content with pixel-perfect accuracy. Edify Image utilizes cascaded pixel-space diffusion models trained using a novel Laplacian diffusion process, in which image signals at different frequency bands are attenuated at varying rates. Edify Image supports a wide range of applications, including text-to-i&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.07126v1-abstract-full').style.display = 'inline'; document.getElementById('2411.07126v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.07126v1-abstract-full" style="display: none;"> We introduce Edify Image, a family of diffusion models capable of generating photorealistic image content with pixel-perfect accuracy. Edify Image utilizes cascaded pixel-space diffusion models trained using a novel Laplacian diffusion process, in which image signals at different frequency bands are attenuated at varying rates. Edify Image supports a wide range of applications, including text-to-image synthesis, 4K upsampling, ControlNets, 360 HDR panorama generation, and finetuning for image customization. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.07126v1-abstract-full').style.display = 'none'; document.getElementById('2411.07126v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 11 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.06978">arXiv:2411.06978</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.06978">pdf</a>, <a href="https://arxiv.org/ps/2411.06978">ps</a>, <a href="https://arxiv.org/format/2411.06978">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Number Theory">math.NT</span> </div> </div> <p class="title is-5 mathjax"> Cancellation in sums over special sequences on $\mathbf{\rm{GL}_{m}}$ and their applications </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qiang Ma</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+R">Rui Zhang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.06978v2-abstract-short" style="display: inline;"> Let $a(n)$ be the $n$-th Dirichlet coefficient of the automorphic $L$-function or the Rankin--Selberg $L$-function. We investigate the cancellation of $a(n)$ over specific sequences linked to the Waring--Goldbach problem, by establishing a nontrivial bound for the additive twisted sums over primes on ${\mathrm{GL}}_m$ and ${\mathrm{GL}}_m\times{\mathrm{GL}}_m .$ The bound does not depend on the ge&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.06978v2-abstract-full').style.display = 'inline'; document.getElementById('2411.06978v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.06978v2-abstract-full" style="display: none;"> Let $a(n)$ be the $n$-th Dirichlet coefficient of the automorphic $L$-function or the Rankin--Selberg $L$-function. We investigate the cancellation of $a(n)$ over specific sequences linked to the Waring--Goldbach problem, by establishing a nontrivial bound for the additive twisted sums over primes on ${\mathrm{GL}}_m$ and ${\mathrm{GL}}_m\times{\mathrm{GL}}_m .$ The bound does not depend on the generalized Ramanujan conjecture or the nonexistence of Landau--Siegel zeros. Furthermore, we present an application associated with the Sato--Tate conjecture and propose a conjecture about Goldbach&#39;s conjecture on average bound. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.06978v2-abstract-full').style.display = 'none'; document.getElementById('2411.06978v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 13 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 11 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">33 pages. Comments welcome</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">MSC Class:</span> 11L07; 11F66; 11P55 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.03664">arXiv:2411.03664</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.03664">pdf</a>, <a href="https://arxiv.org/format/2411.03664">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Materials Science">cond-mat.mtrl-sci</span> </div> </div> <p class="title is-5 mathjax"> A Predictive First-Principles Framework of Chiral Charge Density Waves </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Shao%2C+S">Sen Shao</a>, <a href="/search/?searchtype=author&amp;query=Chiu%2C+W">Wei-Chi Chiu</a>, <a href="/search/?searchtype=author&amp;query=Hossain%2C+M+S">Md Shafayat Hossain</a>, <a href="/search/?searchtype=author&amp;query=Hou%2C+T">Tao Hou</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+N">Naizhou Wang</a>, <a href="/search/?searchtype=author&amp;query=Belopolski%2C+I">Ilya Belopolski</a>, <a href="/search/?searchtype=author&amp;query=Zhao%2C+Y">Yilin Zhao</a>, <a href="/search/?searchtype=author&amp;query=Ni%2C+J">Jinyang Ni</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+Q">Qi Zhang</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+Y">Yongkai Li</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+J">Jinjin Liu</a>, <a href="/search/?searchtype=author&amp;query=Yahyavi%2C+M">Mohammad Yahyavi</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Yuanjun Jin</a>, <a href="/search/?searchtype=author&amp;query=Feng%2C+Q">Qiange Feng</a>, <a href="/search/?searchtype=author&amp;query=Cui%2C+P">Peiyuan Cui</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+C">Cheng-Long Zhang</a>, <a href="/search/?searchtype=author&amp;query=Yao%2C+Y">Yugui Yao</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+Z">Zhiwei Wang</a>, <a href="/search/?searchtype=author&amp;query=Yin%2C+J">Jia-Xin Yin</a>, <a href="/search/?searchtype=author&amp;query=Xu%2C+S">Su-Yang Xu</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qiong Ma</a>, <a href="/search/?searchtype=author&amp;query=Gao%2C+W">Wei-bo Gao</a>, <a href="/search/?searchtype=author&amp;query=Bansil%2C+A">Arun Bansil</a>, <a href="/search/?searchtype=author&amp;query=Hasan%2C+M+Z">M. Zahid Hasan</a>, <a href="/search/?searchtype=author&amp;query=Chang%2C+G">Guoqing Chang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.03664v1-abstract-short" style="display: inline;"> Implementing and tuning chirality is fundamental in physics, chemistry, and material science. Chiral charge density waves (CDWs), where chirality arises from correlated charge orders, are attracting intense interest due to their exotic transport and optical properties. However, a general framework for predicting chiral CDW materials is lacking, primarily because the underlying mechanisms remain el&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.03664v1-abstract-full').style.display = 'inline'; document.getElementById('2411.03664v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.03664v1-abstract-full" style="display: none;"> Implementing and tuning chirality is fundamental in physics, chemistry, and material science. Chiral charge density waves (CDWs), where chirality arises from correlated charge orders, are attracting intense interest due to their exotic transport and optical properties. However, a general framework for predicting chiral CDW materials is lacking, primarily because the underlying mechanisms remain elusive. Here, we address this challenge by developing the first comprehensive predictive framework, systematically identifying chiral CDW materials via first-principles calculations. The key lies in the previously overlooked phase difference of the CDW Q-vectors between layers, which is linked to opposite collective atomic displacements across different layers. This phase difference induces a spiral arrangement of the Q-vectors, ultimately giving rise to a chiral structure in real space. We validate our framework by applying it to the kagome lattice AV$_{3}$Sb$_{5}$ (A = K, Rb, Cs), successfully predicting emergent structural chirality. To demonstrate the generality of our approach, we extend it to predict chiral CDWs in the triangular-lattice NbSe$_{2}$. Beyond material predictions, our theory uncovers a universal and unprecedented Hall effect in chiral CDW materials, occurring without external magnetic fields or intrinsic magnetization. Our experiments on CsV$_{3}$Sb$_{5}$ confirm this prediction, observing a unique signature where the Hall conductivity&#39;s sign reverses when the input current is reversed, a phenomenon distinct from known Hall effects. Our findings elucidate the mechanisms behind chiral CDWs and open new avenues for discovering materials with unconventional quantum properties, with potential applications in next-generation electronic and spintronic devices. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.03664v1-abstract-full').style.display = 'none'; document.getElementById('2411.03664v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.01215">arXiv:2411.01215</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.01215">pdf</a>, <a href="https://arxiv.org/format/2411.01215">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Astrophysical Phenomena">astro-ph.HE</span> </div> </div> <p class="title is-5 mathjax"> Detection of two TeV gamma-ray outbursts from NGC 1275 by LHAASO </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Cao%2C+Z">Zhen Cao</a>, <a href="/search/?searchtype=author&amp;query=Aharonian%2C+F">F. Aharonian</a>, <a href="/search/?searchtype=author&amp;query=Axikegu"> Axikegu</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y+X">Y. X. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+Y+W">Y. W. Bao</a>, <a href="/search/?searchtype=author&amp;query=Bastieri%2C+D">D. Bastieri</a>, <a href="/search/?searchtype=author&amp;query=Bi%2C+X+J">X. J. Bi</a>, <a href="/search/?searchtype=author&amp;query=Bi%2C+Y+J">Y. J. Bi</a>, <a href="/search/?searchtype=author&amp;query=Cai%2C+J+T">J. T. Cai</a>, <a href="/search/?searchtype=author&amp;query=Cao%2C+Q">Q. Cao</a>, <a href="/search/?searchtype=author&amp;query=Cao%2C+W+Y">W. Y. Cao</a>, <a href="/search/?searchtype=author&amp;query=Cao%2C+Z">Zhe Cao</a>, <a href="/search/?searchtype=author&amp;query=Chang%2C+J">J. Chang</a>, <a href="/search/?searchtype=author&amp;query=Chang%2C+J+F">J. F. Chang</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+A+M">A. M. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+E+S">E. S. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+L">Liang Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+L">Lin Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+L">Long Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+M+J">M. J. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+M+L">M. L. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+Q+H">Q. H. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+S+H">S. H. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+S+Z">S. Z. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+T+L">T. L. Chen</a> , et al. (254 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.01215v2-abstract-short" style="display: inline;"> The Water Cherenkov Detector Array (WCDA) is one of the components of Large High Altitude Air Shower Observatory (LHAASO) and can monitor any sources over two-thirds of the sky for up to 7 hours per day with &gt;98\% duty cycle. In this work, we report the detection of two outbursts of the Fanaroff-Riley I radio galaxy NGC 1275 that were detected by LHAASO-WCDA between November 2022 and January 2023&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.01215v2-abstract-full').style.display = 'inline'; document.getElementById('2411.01215v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.01215v2-abstract-full" style="display: none;"> The Water Cherenkov Detector Array (WCDA) is one of the components of Large High Altitude Air Shower Observatory (LHAASO) and can monitor any sources over two-thirds of the sky for up to 7 hours per day with &gt;98\% duty cycle. In this work, we report the detection of two outbursts of the Fanaroff-Riley I radio galaxy NGC 1275 that were detected by LHAASO-WCDA between November 2022 and January 2023 with statistical significance of 5.2~$蟽$ and 8.3~$蟽$. The observed spectral energy distribution in the range from 500 GeV to 3 TeV is fitted by a power-law with a best-fit spectral index of $伪=-3.37\pm0.52$ and $-3.35\pm0.29$, respectively. The outburst flux above 0.5~TeV was ($4.55\pm 4.21)\times~10^{-11}~\rm cm^{-2}~s^{-1}$ and ($3.45\pm 1.78)\times~10^{-11}~\rm cm^{-2}~s^{-1}$, corresponding to 60\%, 45\% of Crab Nebula flux. Variation analysis reveals the variability time-scale of days at the TeV energy band. A simple test by one-zone synchrotron self-Compton model reproduces the data in the gamma-ray band well. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.01215v2-abstract-full').style.display = 'none'; document.getElementById('2411.01215v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 2 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">11 pages, 8 figures, 3 tables</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.22981">arXiv:2410.22981</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.22981">pdf</a>, <a href="https://arxiv.org/format/2410.22981">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Machine Learning">cs.LG</span> </div> </div> <p class="title is-5 mathjax"> DisenTS: Disentangled Channel Evolving Pattern Modeling for Multivariate Time Series Forecasting </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Liu%2C+Z">Zhiding Liu</a>, <a href="/search/?searchtype=author&amp;query=Yang%2C+J">Jiqian Yang</a>, <a href="/search/?searchtype=author&amp;query=Mao%2C+Q">Qingyang Mao</a>, <a href="/search/?searchtype=author&amp;query=Zhao%2C+Y">Yuze Zhao</a>, <a href="/search/?searchtype=author&amp;query=Cheng%2C+M">Mingyue Cheng</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+Z">Zhi Li</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+Q">Qi Liu</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+E">Enhong Chen</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.22981v1-abstract-short" style="display: inline;"> Multivariate time series forecasting plays a crucial role in various real-world applications. Significant efforts have been made to integrate advanced network architectures and training strategies that enhance the capture of temporal dependencies, thereby improving forecasting accuracy. On the other hand, mainstream approaches typically utilize a single unified model with simplistic channel-mixing&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.22981v1-abstract-full').style.display = 'inline'; document.getElementById('2410.22981v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.22981v1-abstract-full" style="display: none;"> Multivariate time series forecasting plays a crucial role in various real-world applications. Significant efforts have been made to integrate advanced network architectures and training strategies that enhance the capture of temporal dependencies, thereby improving forecasting accuracy. On the other hand, mainstream approaches typically utilize a single unified model with simplistic channel-mixing embedding or cross-channel attention operations to account for the critical intricate inter-channel dependencies. Moreover, some methods even trade capacity for robust prediction based on the channel-independent assumption. Nonetheless, as time series data may display distinct evolving patterns due to the unique characteristics of each channel (including multiple strong seasonalities and trend changes), the unified modeling methods could yield suboptimal results. To this end, we propose DisenTS, a tailored framework for modeling disentangled channel evolving patterns in general multivariate time series forecasting. The central idea of DisenTS is to model the potential diverse patterns within the multivariate time series data in a decoupled manner. Technically, the framework employs multiple distinct forecasting models, each tasked with uncovering a unique evolving pattern. To guide the learning process without supervision of pattern partition, we introduce a novel Forecaster Aware Gate (FAG) module that generates the routing signals adaptively according to both the forecasters&#39; states and input series&#39; characteristics. The forecasters&#39; states are derived from the Linear Weight Approximation (LWA) strategy, which quantizes the complex deep neural networks into compact matrices. Additionally, the Similarity Constraint (SC) is further proposed to guide each model to specialize in an underlying pattern by minimizing the mutual information between the representations. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.22981v1-abstract-full').style.display = 'none'; document.getElementById('2410.22981v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 30 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.21841">arXiv:2410.21841</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.21841">pdf</a>, <a href="https://arxiv.org/ps/2410.21841">ps</a>, <a href="https://arxiv.org/format/2410.21841">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Search for $螞$-$\bar螞 $ oscillation in $J/蠄\rightarrow螞\bar螞$ decay </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (638 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.21841v2-abstract-short" style="display: inline;"> Using $(10087\pm44)\times 10^{6}$ $J/蠄$ decays collected by the BESIII detector at the BEPCII collider, we search for baryon number violation via $螞-\bar螞$ oscillation in the decay $J/蠄\to 螞\bar螞$. No evidence for $螞-\bar螞$ oscillation is observed. The upper limit on the time-integrated probability of $螞-\bar螞$ oscillation is estimated to be $1.4\times 10^{-6}$, corresponding to an oscillation par&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.21841v2-abstract-full').style.display = 'inline'; document.getElementById('2410.21841v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.21841v2-abstract-full" style="display: none;"> Using $(10087\pm44)\times 10^{6}$ $J/蠄$ decays collected by the BESIII detector at the BEPCII collider, we search for baryon number violation via $螞-\bar螞$ oscillation in the decay $J/蠄\to 螞\bar螞$. No evidence for $螞-\bar螞$ oscillation is observed. The upper limit on the time-integrated probability of $螞-\bar螞$ oscillation is estimated to be $1.4\times 10^{-6}$, corresponding to an oscillation parameter less than $2.1\times 10^{-18}~\mathrm{GeV}$ at $90\%$ confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.21841v2-abstract-full').style.display = 'none'; document.getElementById('2410.21841v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 29 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 29 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">8 pages, 2 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.20063">arXiv:2410.20063</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.20063">pdf</a>, <a href="https://arxiv.org/format/2410.20063">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Measurement of the branching fraction of $D^+ \to 蟿^+谓_蟿$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (650 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.20063v2-abstract-short" style="display: inline;"> By analyzing $e^{+}e^{-}$ collision data with an integrated luminosity of 7.9~fb$^{-1}$ collected with the BESIII detector at the center-of-mass energy of 3.773~GeV, the branching fraction of $D^+\to蟿^+谓_蟿$ is determined as $\mathcal{B}=(9.9\pm 1.1_\mathrm{stat}\pm 0.5_\mathrm{syst})\times10^{-4}$. Taking the most precise result&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.20063v2-abstract-full').style.display = 'inline'; document.getElementById('2410.20063v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.20063v2-abstract-full" style="display: none;"> By analyzing $e^{+}e^{-}$ collision data with an integrated luminosity of 7.9~fb$^{-1}$ collected with the BESIII detector at the center-of-mass energy of 3.773~GeV, the branching fraction of $D^+\to蟿^+谓_蟿$ is determined as $\mathcal{B}=(9.9\pm 1.1_\mathrm{stat}\pm 0.5_\mathrm{syst})\times10^{-4}$. Taking the most precise result $\mathcal{B}(D^+\to渭^+谓_渭)=(3.981\pm 0.079_\mathrm{stat}\pm0.040_\mathrm{syst})\times10^{-4}$, we determine $R_{蟿/渭} = 螕(D^+\to蟿^+谓_蟿)/螕(D^+\to渭^+谓_渭)= 2.49\pm0.31$, achieving a factor of two improvement in precision compared to the previous BESIII result. This measurement is in agreement with the standard model prediction of lepton flavor universality within one standard deviation. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.20063v2-abstract-full').style.display = 'none'; document.getElementById('2410.20063v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 25 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 26 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.18505">arXiv:2410.18505</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.18505">pdf</a>, <a href="https://arxiv.org/format/2410.18505">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computation and Language">cs.CL</span> </div> </div> <p class="title is-5 mathjax"> CCI3.0-HQ: a large-scale Chinese dataset of high quality designed for pre-training large language models </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Wang%2C+L">Liangdong Wang</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+B">Bo-Wen Zhang</a>, <a href="/search/?searchtype=author&amp;query=Wu%2C+C">Chengwei Wu</a>, <a href="/search/?searchtype=author&amp;query=Zhao%2C+H">Hanyu Zhao</a>, <a href="/search/?searchtype=author&amp;query=Shi%2C+X">Xiaofeng Shi</a>, <a href="/search/?searchtype=author&amp;query=Gu%2C+S">Shuhao Gu</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+J">Jijie Li</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Quanyue Ma</a>, <a href="/search/?searchtype=author&amp;query=Pan%2C+T">TengFei Pan</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+G">Guang Liu</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.18505v2-abstract-short" style="display: inline;"> We present CCI3.0-HQ (https://huggingface.co/datasets/BAAI/CCI3-HQ), a high-quality 500GB subset of the Chinese Corpora Internet 3.0 (CCI3.0)(https://huggingface.co/datasets/BAAI/CCI3-Data), developed using a novel two-stage hybrid filtering pipeline that significantly enhances data quality. To evaluate its effectiveness, we trained a 0.5B parameter model from scratch on 100B tokens across various&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.18505v2-abstract-full').style.display = 'inline'; document.getElementById('2410.18505v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.18505v2-abstract-full" style="display: none;"> We present CCI3.0-HQ (https://huggingface.co/datasets/BAAI/CCI3-HQ), a high-quality 500GB subset of the Chinese Corpora Internet 3.0 (CCI3.0)(https://huggingface.co/datasets/BAAI/CCI3-Data), developed using a novel two-stage hybrid filtering pipeline that significantly enhances data quality. To evaluate its effectiveness, we trained a 0.5B parameter model from scratch on 100B tokens across various datasets, achieving superior performance on 10 benchmarks in a zero-shot setting compared to CCI3.0, SkyPile, and WanjuanV1. The high-quality filtering process effectively distills the capabilities of the Qwen2-72B-instruct model into a compact 0.5B model, attaining optimal F1 scores for Chinese web data classification. We believe this open-access dataset will facilitate broader access to high-quality language models. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.18505v2-abstract-full').style.display = 'none'; document.getElementById('2410.18505v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 25 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 24 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.18464">arXiv:2410.18464</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.18464">pdf</a>, <a href="https://arxiv.org/ps/2410.18464">ps</a>, <a href="https://arxiv.org/format/2410.18464">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Search for $畏_c(2S)\to p\bar{p}$ and branching fraction measurements of $蠂_{cJ} \to p\bar{p}$ via $蠄(2S)$ radiative decays </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (640 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.18464v1-abstract-short" style="display: inline;"> Using $(27.12\pm0.14) \times 10^{8}$ $蠄(2S)$ events collected by the BESIII detector operating at BEPCII, we search for the decay $畏_c(2S)\to p\bar{p}$ via the process $蠄(2S)\to 纬畏_c(2S)$, and only find a signal with a significance of $1.7\,蟽$. The upper limit of the product branching fraction at the 90% confidence level is determined to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.18464v1-abstract-full').style.display = 'inline'; document.getElementById('2410.18464v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.18464v1-abstract-full" style="display: none;"> Using $(27.12\pm0.14) \times 10^{8}$ $蠄(2S)$ events collected by the BESIII detector operating at BEPCII, we search for the decay $畏_c(2S)\to p\bar{p}$ via the process $蠄(2S)\to 纬畏_c(2S)$, and only find a signal with a significance of $1.7\,蟽$. The upper limit of the product branching fraction at the 90% confidence level is determined to be $\mathcal{B}(蠄(2S)\to 纬畏_c(2S))\times \mathcal{B}(畏_c(2S)\to p\bar{p})&lt;2.4\times 10^{-7}$. The branching fractions of $蠂_{cJ}\to p\bar{p}~(J=0,1,2)$ are also measured to be $\mathcal{B}(蠂_{c0}\to p\bar{p})=(2.51\pm0.02\pm0.08)\times 10^{-4}$, $\mathcal{B}(蠂_{c1}\to p\bar{p})=(8.16\pm0.09\pm0.25)\times 10^{-4}$, and $\mathcal{B}(蠂_{c2}\to p\bar{p})=(8.33\pm0.09\pm0.22)\times 10^{-4}$, where the first uncertainty is statistical and the second systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.18464v1-abstract-full').style.display = 'none'; document.getElementById('2410.18464v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.17871">arXiv:2410.17871</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.17871">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Applied Physics">physics.app-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Optics">physics.optics</span> </div> </div> <p class="title is-5 mathjax"> Advances and Applications of Dynamic Surface-Enhanced Raman Spectroscopy (SERS) for Single Molecule Studies </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Zou%2C+Y">Yanqiu Zou</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+H">Huaizhou Jin</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qifei Ma</a>, <a href="/search/?searchtype=author&amp;query=Zheng%2C+Z">Zhenrong Zheng</a>, <a href="/search/?searchtype=author&amp;query=Weng%2C+S">Shukun Weng</a>, <a href="/search/?searchtype=author&amp;query=Kolataj%2C+K">Karol Kolataj</a>, <a href="/search/?searchtype=author&amp;query=Acuna%2C+G">Guillermo Acuna</a>, <a href="/search/?searchtype=author&amp;query=Bald%2C+I">Ilko Bald</a>, <a href="/search/?searchtype=author&amp;query=Garoli%2C+D">Denis Garoli</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.17871v1-abstract-short" style="display: inline;"> Dynamic surface-enhanced Raman spectroscopy (SERS) is nowadays one of the most interesting applications of SERS, in particular for single molecule studies. In fact, it enables the study of real-time processes at the molecular level. This review summarizes the latest developments in dynamic SERS techniques and their applications, focusing on new instrumentation, data analysis methods, temporal reso&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.17871v1-abstract-full').style.display = 'inline'; document.getElementById('2410.17871v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.17871v1-abstract-full" style="display: none;"> Dynamic surface-enhanced Raman spectroscopy (SERS) is nowadays one of the most interesting applications of SERS, in particular for single molecule studies. In fact, it enables the study of real-time processes at the molecular level. This review summarizes the latest developments in dynamic SERS techniques and their applications, focusing on new instrumentation, data analysis methods, temporal resolution and sensitivity improvements, and novel substrates. We highlight the progress and applications of single-molecule dynamic SERS in monitoring chemical reactions, catalysis, biomolecular interactions, conformational dynamics, and real-time sensing and detection. We aim to provide a comprehensive review on its advancements, applications as well as its current challenges and development frontiers. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.17871v1-abstract-full').style.display = 'none'; document.getElementById('2410.17871v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 23 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.16912">arXiv:2410.16912</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.16912">pdf</a>, <a href="https://arxiv.org/ps/2410.16912">ps</a>, <a href="https://arxiv.org/format/2410.16912">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Measurement of the branching fractions of the decays $螞_{c}^{+}\rightarrow螞K_{S}^{0}K^{+}$, $螞_{c}^{+}\rightarrow螞K_{S}^{0}蟺^{+}$ and $螞_{c}^{+}\rightarrow螞K^{*+}$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (639 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.16912v1-abstract-short" style="display: inline;"> Studies are performed of the Cabibbo-favored decay $螞_{c}^{+}\to螞K_{S}^{0}K^+$ and the singly Cabibbo-suppressed decay $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$, based on a sample of $e^{+}e^{-}$ collision data, corresponding to an integrated luminosity of 4.5 fb$^{-1}$, accumulated at center-of-mass energies between $4599.53$ MeV and $4698.82$ MeV with the BESIII detector. The decay&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.16912v1-abstract-full').style.display = 'inline'; document.getElementById('2410.16912v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.16912v1-abstract-full" style="display: none;"> Studies are performed of the Cabibbo-favored decay $螞_{c}^{+}\to螞K_{S}^{0}K^+$ and the singly Cabibbo-suppressed decay $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$, based on a sample of $e^{+}e^{-}$ collision data, corresponding to an integrated luminosity of 4.5 fb$^{-1}$, accumulated at center-of-mass energies between $4599.53$ MeV and $4698.82$ MeV with the BESIII detector. The decay $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$ is observed for the first time. The branching fractions of $螞_{c}^{+}\to螞K_{S}^{0}K^+$ and $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$ are measured to be $(3.04\pm0.30\pm0.16)\times 10^{-3}$ and $(1.73\pm0.27\pm0.10)\times 10^{-3}$, respectively, where the first uncertainties are statistical and the second are systematic. These results correspond to the most precise measurement of these quantities for both decays. Evidence of a $K^{*+}$ contribution in the $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$ decay is found with a statistical significance of $4.7蟽$. The branching fraction of $螞_{c}^{+}\to螞K^{*+}$ is calculated under three possible interference scenarios. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.16912v1-abstract-full').style.display = 'none'; document.getElementById('2410.16912v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 22 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.13515">arXiv:2410.13515</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.13515">pdf</a>, <a href="https://arxiv.org/format/2410.13515">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Observation of a rare beta decay of the charmed baryon with a Graph Neural Network </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (637 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.13515v1-abstract-short" style="display: inline;"> The study of beta decay of the charmed baryon provides unique insights into the fundamental mechanism of the strong and electro-weak interactions. The $螞_c^+$, being the lightest charmed baryon, undergoes disintegration solely through the charm quark weak decay. Its beta decay provides an ideal laboratory for investigating non-perturbative effects in quantum chromodynamics and for constraining the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13515v1-abstract-full').style.display = 'inline'; document.getElementById('2410.13515v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.13515v1-abstract-full" style="display: none;"> The study of beta decay of the charmed baryon provides unique insights into the fundamental mechanism of the strong and electro-weak interactions. The $螞_c^+$, being the lightest charmed baryon, undergoes disintegration solely through the charm quark weak decay. Its beta decay provides an ideal laboratory for investigating non-perturbative effects in quantum chromodynamics and for constraining the fundamental parameters of the Cabibbo-Kobayashi-Maskawa matrix in weak interaction theory. This article presents the first observation of the Cabibbo-suppressed $螞_c^+$ beta decay into a neutron $螞_c^+ \rightarrow n e^+ 谓_{e}$, based on $4.5~\mathrm{fb}^{-1}$ of electron-positron annihilation data collected with the BESIII detector in the energy region above the $螞^+_c\bar螞^-_c$ threshold. A novel machine learning technique, leveraging Graph Neural Networks, has been utilized to effectively separate signals from dominant backgrounds, particularly $螞_c^+ \rightarrow 螞e^+ 谓_{e}$. This approach has yielded a statistical significance of more than $10蟽$. The absolute branching fraction of $螞_c^+ \rightarrow n e^+ 谓_{e}$ is measured to be $(3.57\pm0.34_{\mathrm{stat}}\pm0.14_{\mathrm{syst}})\times 10^{-3}$. For the first time, the CKM matrix element $\left|V_{cd}\right|$ is extracted via a charmed baryon decay to be $0.208\pm0.011_{\rm exp.}\pm0.007_{\rm LQCD}\pm0.001_{蟿_{螞_c^+}}$. This study provides a new probe to further understand fundamental interactions in the charmed baryon sector, and demonstrates the power of modern machine learning techniques in enhancing experimental capability in high energy physics research. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13515v1-abstract-full').style.display = 'none'; document.getElementById('2410.13515v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 17 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">28 pages, 6 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.13478">arXiv:2410.13478</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.13478">pdf</a>, <a href="https://arxiv.org/format/2410.13478">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Observation of $蠂_{c0}\to危^{+}\bar危^{-}畏$ and evidence for $蠂_{c1,2}\to危^{+}\bar危^{-}畏$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (634 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.13478v1-abstract-short" style="display: inline;"> Using $(27.12\pm 0.14)\times10^{8}$ $蠄(3686)$ events collected with the BESIII detector, the decay $蠂_{c0}\to危^{+}\bar危^{-}畏$ is observed for the first time with a statistical significance of $7.0蟽$, and evidence for $蠂_{c1}\to危^{+}\bar危^{-}畏$ and $蠂_{c2}\to危^{+}\bar危^{-}畏$ is found with statistical significances of $4.3蟽$ and $4.6蟽$, respectively. The branching fractions are determined to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13478v1-abstract-full').style.display = 'inline'; document.getElementById('2410.13478v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.13478v1-abstract-full" style="display: none;"> Using $(27.12\pm 0.14)\times10^{8}$ $蠄(3686)$ events collected with the BESIII detector, the decay $蠂_{c0}\to危^{+}\bar危^{-}畏$ is observed for the first time with a statistical significance of $7.0蟽$, and evidence for $蠂_{c1}\to危^{+}\bar危^{-}畏$ and $蠂_{c2}\to危^{+}\bar危^{-}畏$ is found with statistical significances of $4.3蟽$ and $4.6蟽$, respectively. The branching fractions are determined to be $\mathcal{B}(蠂_{c0}\to危^{+}\bar危^{-}畏)=({1.26 \pm 0.20 \pm 0.13}) \times 10^{-4}, ~\mathcal{B}(蠂_{c1}\to危^{+}\bar危^{-}畏)=({5.10 \pm 1.21 \pm 0.67}) \times 10^{-5}$, and $\mathcal{B}(蠂_{c2}\to危^{+}\bar危^{-}畏)=({5.46 \pm 1.18 \pm 0.50}) \times 10^{-5}$, where the first uncertainties are statistical, and the second ones are systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13478v1-abstract-full').style.display = 'none'; document.getElementById('2410.13478v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 17 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.13368">arXiv:2410.13368</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.13368">pdf</a>, <a href="https://arxiv.org/format/2410.13368">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> </div> </div> <p class="title is-5 mathjax"> Observation of the Singly Cabibbo-Suppressed Decay $螞_c^{+}\to p蟺^0$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (638 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.13368v1-abstract-short" style="display: inline;"> Utilizing 4.5${~\rm{fb}}^{-1}$ of $e^+e^-$ annihilation data collected with the BESIII detector at the BEPCII collider at center-of-mass energies between 4.600 and 4.699 GeV, the first observation of the singly Cabibbo-suppressed decay $螞_c^{+}\to p蟺^0$ is presented, with a statistical significance of $5.4蟽$. The ratio of the branching fractions of $螞_c^{+}\to p蟺^0$ and $螞_c^{+}\to p畏$ is measured&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13368v1-abstract-full').style.display = 'inline'; document.getElementById('2410.13368v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.13368v1-abstract-full" style="display: none;"> Utilizing 4.5${~\rm{fb}}^{-1}$ of $e^+e^-$ annihilation data collected with the BESIII detector at the BEPCII collider at center-of-mass energies between 4.600 and 4.699 GeV, the first observation of the singly Cabibbo-suppressed decay $螞_c^{+}\to p蟺^0$ is presented, with a statistical significance of $5.4蟽$. The ratio of the branching fractions of $螞_c^{+}\to p蟺^0$ and $螞_c^{+}\to p畏$ is measured as $\mathcal{B}(螞_c^{+}\to p蟺^0)/\mathcal{B}(螞_c^{+}\to p畏)=(0.120\pm0.026_{\rm stat.}\pm0.007_{\rm syst.})$. This result resolves the longstanding discrepancy between earlier experimental searches, providing both a decisive conclusion and valuable input for QCD-inspired theoretical models. A sophisticated deep learning approach using a Transformer-based architecture is employed to distinguish the signal from the prevalent hadronic backgrounds, complemented by thorough validation and systematic uncertainty quantification. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13368v1-abstract-full').style.display = 'none'; document.getElementById('2410.13368v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 17 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">9 pages, 4 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.12620">arXiv:2410.12620</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.12620">pdf</a>, <a href="https://arxiv.org/format/2410.12620">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Search for $e^{+}e^{-} \to 蠁蠂_{c0}$ and $蠁畏_{c2}(1D)$ at center-of-mass energies from 4.47 to 4.95 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (644 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.12620v1-abstract-short" style="display: inline;"> Utilizing a data set of $6.7$ fb$^{-1}$ from electron-positron collisions recorded by the BESIII detector at the BEPCII storage ring, a search is conducted for the processes $e^{+}e^{-} \to 蠁蠂_{c0}$ and $蠁畏_{c2}(1D)$ across center-of-mass energies from 4.47 to 4.95 GeV. In the absence of any significant signals, upper limits are set. These include limits on the Born cross sections for&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.12620v1-abstract-full').style.display = 'inline'; document.getElementById('2410.12620v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.12620v1-abstract-full" style="display: none;"> Utilizing a data set of $6.7$ fb$^{-1}$ from electron-positron collisions recorded by the BESIII detector at the BEPCII storage ring, a search is conducted for the processes $e^{+}e^{-} \to 蠁蠂_{c0}$ and $蠁畏_{c2}(1D)$ across center-of-mass energies from 4.47 to 4.95 GeV. In the absence of any significant signals, upper limits are set. These include limits on the Born cross sections for $e^{+}e^{-} \to 蠁蠂_{c0}$, as well as the product of the Born cross section for $e^{+}e^{-} \to 蠁畏_{c2}(1D)$ and a sum of five branching fractions. Furthermore, the product of the electronic width of $Y(4660)$ and the branching fraction of the $Y(4660) \to 蠁蠂_{c0}$, denoted as $螕^{Y(4660)}_{e^{+}e^{-}} \mathcal{B}_{Y(4660) \to 蠁蠂_{c0}}$, is determined to be $&lt; 0.40$ eV at the 90\% confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.12620v1-abstract-full').style.display = 'none'; document.getElementById('2410.12620v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 16 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">14 pages, 6 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.12346">arXiv:2410.12346</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.12346">pdf</a>, <a href="https://arxiv.org/format/2410.12346">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> </div> </div> <p class="title is-5 mathjax"> Efficient Diffusion as Low Light Enhancer </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Lan%2C+G">Guanzhou Lan</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qianli Ma</a>, <a href="/search/?searchtype=author&amp;query=Yang%2C+Y">Yuqi Yang</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+Z">Zhigang Wang</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+D">Dong Wang</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+X">Xuelong Li</a>, <a href="/search/?searchtype=author&amp;query=Zhao%2C+B">Bin Zhao</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.12346v2-abstract-short" style="display: inline;"> The computational burden of the iterative sampling process remains a major challenge in diffusion-based Low-Light Image Enhancement (LLIE). Current acceleration methods, whether training-based or training-free, often lead to significant performance degradation, highlighting the trade-off between performance and efficiency. In this paper, we identify two primary factors contributing to performance&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.12346v2-abstract-full').style.display = 'inline'; document.getElementById('2410.12346v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.12346v2-abstract-full" style="display: none;"> The computational burden of the iterative sampling process remains a major challenge in diffusion-based Low-Light Image Enhancement (LLIE). Current acceleration methods, whether training-based or training-free, often lead to significant performance degradation, highlighting the trade-off between performance and efficiency. In this paper, we identify two primary factors contributing to performance degradation: fitting errors and the inference gap. Our key insight is that fitting errors can be mitigated by linearly extrapolating the incorrect score functions, while the inference gap can be reduced by shifting the Gaussian flow to a reflectance-aware residual space. Based on the above insights, we design Reflectance-Aware Trajectory Refinement (RATR) module, a simple yet effective module to refine the teacher trajectory using the reflectance component of images. Following this, we introduce \textbf{Re}flectance-aware \textbf{D}iffusion with \textbf{Di}stilled \textbf{T}rajectory (\textbf{ReDDiT}), an efficient and flexible distillation framework tailored for LLIE. Our framework achieves comparable performance to previous diffusion-based methods with redundant steps in just 2 steps while establishing new state-of-the-art (SOTA) results with 8 or 4 steps. Comprehensive experimental evaluations on 10 benchmark datasets validate the effectiveness of our method, consistently outperforming existing SOTA methods. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.12346v2-abstract-full').style.display = 'none'; document.getElementById('2410.12346v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 21 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">8 pages</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.12274">arXiv:2410.12274</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.12274">pdf</a>, <a href="https://arxiv.org/format/2410.12274">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> </div> </div> <p class="title is-5 mathjax"> Fusion from Decomposition: A Self-Supervised Approach for Image Fusion and Beyond </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Liang%2C+P">Pengwei Liang</a>, <a href="/search/?searchtype=author&amp;query=Jiang%2C+J">Junjun Jiang</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qing Ma</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+X">Xianming Liu</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+J">Jiayi Ma</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.12274v1-abstract-short" style="display: inline;"> Image fusion is famous as an alternative solution to generate one high-quality image from multiple images in addition to image restoration from a single degraded image. The essence of image fusion is to integrate complementary information from source images. Existing fusion methods struggle with generalization across various tasks and often require labor-intensive designs, in which it is difficult&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.12274v1-abstract-full').style.display = 'inline'; document.getElementById('2410.12274v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.12274v1-abstract-full" style="display: none;"> Image fusion is famous as an alternative solution to generate one high-quality image from multiple images in addition to image restoration from a single degraded image. The essence of image fusion is to integrate complementary information from source images. Existing fusion methods struggle with generalization across various tasks and often require labor-intensive designs, in which it is difficult to identify and extract useful information from source images due to the diverse requirements of each fusion task. Additionally, these methods develop highly specialized features for different downstream applications, hindering the adaptation to new and diverse downstream tasks. To address these limitations, we introduce DeFusion++, a novel framework that leverages self-supervised learning (SSL) to enhance the versatility of feature representation for different image fusion tasks. DeFusion++ captures the image fusion task-friendly representations from large-scale data in a self-supervised way, overcoming the constraints of limited fusion datasets. Specifically, we introduce two innovative pretext tasks: common and unique decomposition (CUD) and masked feature modeling (MFM). CUD decomposes source images into abstract common and unique components, while MFM refines these components into robust fused features. Jointly training of these tasks enables DeFusion++ to produce adaptable representations that can effectively extract useful information from various source images, regardless of the fusion task. The resulting fused representations are also highly adaptable for a wide range of downstream tasks, including image segmentation and object detection. DeFusion++ stands out by producing versatile fused representations that can enhance both the quality of image fusion and the effectiveness of downstream high-level vision tasks, simplifying the process with the elegant fusion framework. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.12274v1-abstract-full').style.display = 'none'; document.getElementById('2410.12274v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 16 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">18page</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.11620">arXiv:2410.11620</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.11620">pdf</a>, <a href="https://arxiv.org/format/2410.11620">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Cosmology and Nongalactic Astrophysics">astro-ph.CO</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Astrophysics of Galaxies">astro-ph.GA</span> </div> </div> <p class="title is-5 mathjax"> Exploring the effect of different cosmologies on the Epoch of Reionization 21-cm signal with POLAR </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+A">Anshuman Acharya</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qing-bo Ma</a>, <a href="/search/?searchtype=author&amp;query=Giri%2C+S+K">Sambit K. Giri</a>, <a href="/search/?searchtype=author&amp;query=Ciardi%2C+B">Benedetta Ciardi</a>, <a href="/search/?searchtype=author&amp;query=Ghara%2C+R">Raghunath Ghara</a>, <a href="/search/?searchtype=author&amp;query=Mellema%2C+G">Garrelt Mellema</a>, <a href="/search/?searchtype=author&amp;query=Zaroubi%2C+S">Saleem Zaroubi</a>, <a href="/search/?searchtype=author&amp;query=Hothi%2C+I">Ian Hothi</a>, <a href="/search/?searchtype=author&amp;query=Iliev%2C+I+T">Ilian T. Iliev</a>, <a href="/search/?searchtype=author&amp;query=Koopmans%2C+L+V+E">L茅on V. E. Koopmans</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+M">Michele Bianco</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.11620v1-abstract-short" style="display: inline;"> A detection of the 21-cm signal power spectrum from the Epoch of Reionization is imminent, thanks to consistent advancements from telescopes such as LOFAR, MWA, and HERA, along with the development of SKA. In light of this progress, it is crucial to expand the parameter space of simulations used to infer astrophysical properties from this signal. In this work, we explore the role of cosmological p&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.11620v1-abstract-full').style.display = 'inline'; document.getElementById('2410.11620v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.11620v1-abstract-full" style="display: none;"> A detection of the 21-cm signal power spectrum from the Epoch of Reionization is imminent, thanks to consistent advancements from telescopes such as LOFAR, MWA, and HERA, along with the development of SKA. In light of this progress, it is crucial to expand the parameter space of simulations used to infer astrophysical properties from this signal. In this work, we explore the role of cosmological parameters such as the Hubble constant $H_0$ and the matter clustering amplitude $蟽_8$, whose values as provided by measurements at different redshifts are in tension. We run $N$-body simulations using GADGET-4, and post-process them with the reionization simulation code POLAR, that uses L-GALAXIES to include galaxy formation and evolution properties and GRIZZLY to execute 1-D radiative transfer of ionizing photons in the intergalactic medium (IGM). We compare our results with the latest JWST observations and explore which astrophysical properties for different cosmologies are necessary to match the observed UV luminosity functions at redshifts $z = 10$ and 9. Additionally, we explore the impact of these parameters on the observed 21-cm signal power spectrum, focusing on the redshifts within the range of LOFAR 21-cm signal observations ($z \approx 8.5-10$). Despite differences in cosmological and astrophysical parameters, the 21-cm power spectrum at these redshifts agrees with presently observed upper limits. This suggests the need for broader physical parameter spaces for inference modeling to account for all models that agree with observations. However, we also propose stronger constraining power by using a combination of galactic and IGM observables. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.11620v1-abstract-full').style.display = 'none'; document.getElementById('2410.11620v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 15 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">16 pages, 8 figures, 2 tables. Submitted to the Monthly Notices of the Royal Astronomical Society (MNRAS)</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> NORDITA-2024-035 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.11607">arXiv:2410.11607</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.11607">pdf</a>, <a href="https://arxiv.org/format/2410.11607">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Observation of $蠂_{cJ}\to p \bar p K^0_S K^- 蟺^+ + c.c.$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (648 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.11607v1-abstract-short" style="display: inline;"> By analyzing $(27.12\pm0.14)\times10^8$ $蠄(3686)$ events collected with the BESIII detector operating at the BEPCII collider, the decays of $蠂_{cJ} \to p \bar{p} K^0_S K^- 蟺^+ +c.c.(J=0, 1, 2)$ are observed for the first time with statistical significances greater than $10蟽$. The branching fractions of these decays are determined to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.11607v1-abstract-full').style.display = 'inline'; document.getElementById('2410.11607v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.11607v1-abstract-full" style="display: none;"> By analyzing $(27.12\pm0.14)\times10^8$ $蠄(3686)$ events collected with the BESIII detector operating at the BEPCII collider, the decays of $蠂_{cJ} \to p \bar{p} K^0_S K^- 蟺^+ +c.c.(J=0, 1, 2)$ are observed for the first time with statistical significances greater than $10蟽$. The branching fractions of these decays are determined to be $\mathcal{B}(蠂_{c0}\to p \bar p K^{0}_{S} K^- 蟺^+ + c.c.)=(2.61\pm0.27\pm0.32)\times10^{-5},$ $\mathcal{B}(蠂_{c1}\to p \bar p K^{0}_{S} K^- 蟺^+ + c.c.)=(4.16\pm0.24\pm0.46)\times10^{-5},$ and $\mathcal{B}(蠂_{c2}\to p \bar p K^{0}_{S} K^- 蟺^+ + c.c.)=(5.63\pm0.28\pm0.46)\times10^{-5}$, respectively. The processes $蠂_{c1,2} \to \bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.$ are also observed, with statistical significances of 5.7$蟽$ and 7.0$蟽$, respectively. Evidence for $蠂_{c0} \to\bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.$ is found with statistical significances of 3.3$蟽$ each. The corresponding branching fractions are determined to be $\mathcal{B}(蠂_{c0}\to \bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.) =(1.61^{+0.68}_{-0.64}\pm0.23)\times10^{-5}$, $\mathcal{B}(蠂_{c1}\to \bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.)=(4.06^{+0.80}_{-0.76}\pm0.52)\times10^{-5}$, and $\mathcal{B}(蠂_{c2}\to \bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.)=(4.09^{+0.87}_{-0.84}\pm0.42)\times10^{-5}$. Here, the first uncertainties are statistical and the second ones are systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.11607v1-abstract-full').style.display = 'none'; document.getElementById('2410.11607v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 15 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">12 pages, 5 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.11337">arXiv:2410.11337</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.11337">pdf</a>, <a href="https://arxiv.org/format/2410.11337">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Fluid Dynamics">physics.flu-dyn</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Medical Physics">physics.med-ph</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1017/jfm.2024.600">10.1017/jfm.2024.600 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Hydrodynamic coupling of a cilia--mucus system in Herschel--Bulkley flows </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Mao%2C+Q">Q. Mao</a>, <a href="/search/?searchtype=author&amp;query=d%27Ortona%2C+U">Umberto d&#39;Ortona</a>, <a href="/search/?searchtype=author&amp;query=Favier%2C+J">J. Favier</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.11337v1-abstract-short" style="display: inline;"> The yield stress and shear thinning properties of mucus are identified as critical for ciliary coordination and mucus transport in human airways. We use here numerical simulations to explore the hydrodynamic coupling of cilia and mucus with these two properties using the Herschel--Bulkley model, in a lattice Boltzmann solver for the fluid flow. Three mucus flow regimes, i.e. a poorly organized reg&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.11337v1-abstract-full').style.display = 'inline'; document.getElementById('2410.11337v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.11337v1-abstract-full" style="display: none;"> The yield stress and shear thinning properties of mucus are identified as critical for ciliary coordination and mucus transport in human airways. We use here numerical simulations to explore the hydrodynamic coupling of cilia and mucus with these two properties using the Herschel--Bulkley model, in a lattice Boltzmann solver for the fluid flow. Three mucus flow regimes, i.e. a poorly organized regime, a swirly regime, and a fully unidirectional regime, are observed and analysed by parametric studies. We systematically investigate the effects of ciliary density, interaction length, Bingham number and flow index on the mucus flow regime formation. The underlying mechanism of the regime formation is analysed in detail by examining the variation of two physical quantities (polarization and integral length) and the evolution of the flow velocity, viscosity and shear-rate fields. Mucus viscosity is found to be the dominant parameter influencing the regime formation when enhancing the yield stress and shear thinning properties. The present model is able to reproduce the solid body rotation observed in experiments (Loiseau et al. , Nat. Phys. , vol. 16, 2020, pp. 1158--1164). A more precise prediction can be achieved by incorporating non-Newtonian properties into the modelling of mucus as proposed by Gsell et al. ( Sci. Rep. , vol. 10, 2020, 8405). <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.11337v1-abstract-full').style.display = 'none'; document.getElementById('2410.11337v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 15 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Journal of Fluid Mechanics, 2024, 994, pp.A8 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.08889">arXiv:2410.08889</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.08889">pdf</a>, <a href="https://arxiv.org/format/2410.08889">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> </div> </div> <p class="title is-5 mathjax"> Exploiting Memory-aware Q-distribution Prediction for Nuclear Fusion via Modern Hopfield Network </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qingchuan Ma</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+S">Shiao Wang</a>, <a href="/search/?searchtype=author&amp;query=Zheng%2C+T">Tong Zheng</a>, <a href="/search/?searchtype=author&amp;query=Dai%2C+X">Xiaodong Dai</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+Y">Yifeng Wang</a>, <a href="/search/?searchtype=author&amp;query=Yang%2C+Q">Qingquan Yang</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+X">Xiao Wang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.08889v1-abstract-short" style="display: inline;"> This study addresses the critical challenge of predicting the Q-distribution in long-term stable nuclear fusion task, a key component for advancing clean energy solutions. We introduce an innovative deep learning framework that employs Modern Hopfield Networks to incorporate associative memory from historical shots. Utilizing a newly compiled dataset, we demonstrate the effectiveness of our approa&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08889v1-abstract-full').style.display = 'inline'; document.getElementById('2410.08889v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.08889v1-abstract-full" style="display: none;"> This study addresses the critical challenge of predicting the Q-distribution in long-term stable nuclear fusion task, a key component for advancing clean energy solutions. We introduce an innovative deep learning framework that employs Modern Hopfield Networks to incorporate associative memory from historical shots. Utilizing a newly compiled dataset, we demonstrate the effectiveness of our approach in enhancing Q-distribution prediction. The proposed method represents a significant advancement by leveraging historical memory information for the first time in this context, showcasing improved prediction accuracy and contributing to the optimization of nuclear fusion research. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08889v1-abstract-full').style.display = 'none'; document.getElementById('2410.08889v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 11 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.08879">arXiv:2410.08879</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.08879">pdf</a>, <a href="https://arxiv.org/format/2410.08879">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> </div> </div> <p class="title is-5 mathjax"> Multi-modal Fusion based Q-distribution Prediction for Controlled Nuclear Fusion </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Wang%2C+S">Shiao Wang</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+Y">Yifeng Wang</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qingchuan Ma</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+X">Xiao Wang</a>, <a href="/search/?searchtype=author&amp;query=Yan%2C+N">Ning Yan</a>, <a href="/search/?searchtype=author&amp;query=Yang%2C+Q">Qingquan Yang</a>, <a href="/search/?searchtype=author&amp;query=Xu%2C+G">Guosheng Xu</a>, <a href="/search/?searchtype=author&amp;query=Tang%2C+J">Jin Tang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.08879v1-abstract-short" style="display: inline;"> Q-distribution prediction is a crucial research direction in controlled nuclear fusion, with deep learning emerging as a key approach to solving prediction challenges. In this paper, we leverage deep learning techniques to tackle the complexities of Q-distribution prediction. Specifically, we explore multimodal fusion methods in computer vision, integrating 2D line image data with the original 1D&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08879v1-abstract-full').style.display = 'inline'; document.getElementById('2410.08879v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.08879v1-abstract-full" style="display: none;"> Q-distribution prediction is a crucial research direction in controlled nuclear fusion, with deep learning emerging as a key approach to solving prediction challenges. In this paper, we leverage deep learning techniques to tackle the complexities of Q-distribution prediction. Specifically, we explore multimodal fusion methods in computer vision, integrating 2D line image data with the original 1D data to form a bimodal input. Additionally, we employ the Transformer&#39;s attention mechanism for feature extraction and the interactive fusion of bimodal information. Extensive experiments validate the effectiveness of our approach, significantly reducing prediction errors in Q-distribution. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08879v1-abstract-full').style.display = 'none'; document.getElementById('2410.08879v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 11 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.08866">arXiv:2410.08866</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.08866">pdf</a>, <a href="https://arxiv.org/ps/2410.08866">ps</a>, <a href="https://arxiv.org/format/2410.08866">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Differential Geometry">math.DG</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Analysis of PDEs">math.AP</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Algebraic Topology">math.AT</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="K-Theory and Homology">math.KT</span> </div> </div> <p class="title is-5 mathjax"> Bounding the A-hat genus using scalar curvature lower bounds and isoperimetric constants </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qiaochu Ma</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+J">Jinmin Wang</a>, <a href="/search/?searchtype=author&amp;query=Yu%2C+G">Guoliang Yu</a>, <a href="/search/?searchtype=author&amp;query=Zhu%2C+B">Bo Zhu</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.08866v1-abstract-short" style="display: inline;"> In this paper, we prove an upper bound on the $\widehat{A}$ genus of a smooth, closed, spin Riemannian manifold using its scalar curvature lower bound, Neumann isoperimetric constant, and volume. The proof of this result relies on spectral analysis of the Dirac operator. We also construct an example to show that the Neumann isoperimetric constant in this bound is necessary. Our result partially an&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08866v1-abstract-full').style.display = 'inline'; document.getElementById('2410.08866v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.08866v1-abstract-full" style="display: none;"> In this paper, we prove an upper bound on the $\widehat{A}$ genus of a smooth, closed, spin Riemannian manifold using its scalar curvature lower bound, Neumann isoperimetric constant, and volume. The proof of this result relies on spectral analysis of the Dirac operator. We also construct an example to show that the Neumann isoperimetric constant in this bound is necessary. Our result partially answers a question of Gromov on bounding characteristic numbers using scalar curvature lower bound. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08866v1-abstract-full').style.display = 'none'; document.getElementById('2410.08866v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 11 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Comments are welcome!</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.08603">arXiv:2410.08603</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.08603">pdf</a>, <a href="https://arxiv.org/format/2410.08603">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Observation of $D^+\to畏^\prime渭^+谓_渭$ and First Study of $D^+\to 畏^\prime \ell^+谓_\ell$ Decay Dynamics </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (643 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.08603v1-abstract-short" style="display: inline;"> Using $20.3\,\rm fb^{-1}$ of $e^+e^-$ collision data collected at the center-of-mass energy 3.773\,GeV with the BESIII detector, we report the first observation of the semileptonic decay $D^+\to 畏^\prime 渭^+谓_渭$ with significance of $8.6蟽$ including systematic uncertainties, and an improved measurement of $D^+\to 畏^\prime e^+谓_e$. The branching fractions of $D^+\to 畏^\prime 渭^+谓_渭$ and&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08603v1-abstract-full').style.display = 'inline'; document.getElementById('2410.08603v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.08603v1-abstract-full" style="display: none;"> Using $20.3\,\rm fb^{-1}$ of $e^+e^-$ collision data collected at the center-of-mass energy 3.773\,GeV with the BESIII detector, we report the first observation of the semileptonic decay $D^+\to 畏^\prime 渭^+谓_渭$ with significance of $8.6蟽$ including systematic uncertainties, and an improved measurement of $D^+\to 畏^\prime e^+谓_e$. The branching fractions of $D^+\to 畏^\prime 渭^+谓_渭$ and $D^+\to 畏^\prime e^+谓_e$ are determined to be $(1.92\pm0.28_{\rm stat}\pm 0.08_{\rm syst})\times 10^{-4}$ and $(1.79\pm0.19_{\rm stat}\pm 0.07_{\rm syst})\times 10^{-4}$, respectively. From an analysis of the $D^+\to 畏^\prime \ell^+谓_\ell$ decay dynamics, the product of the hadronic form factor $f_+^{畏^{\prime}}(0)$ and the CKM matrix element $|V_{cd}|$ is measured for the first time, giving $f^{畏^\prime}_+(0)|V_{cd}| = (5.92\pm0.56_{\rm stat}\pm0.13_{\rm syst})\times 10^{-2}$. No evidence for violation of $渭-e$ lepton-flavor universality is found in both the full range and several bins of $\ell^+谓_\ell$ four-momentum transfer. The $畏-畏^\prime$ mixing angle in the quark flavor basis is determined to be $蠁_{\rm P} =(39.8\pm0.8_{\rm stat}\pm0.3_{\rm syst})^\circ$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08603v1-abstract-full').style.display = 'none'; document.getElementById('2410.08603v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 11 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.07626">arXiv:2410.07626</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.07626">pdf</a>, <a href="https://arxiv.org/format/2410.07626">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Precision Measurement of the Branching Fraction of $D^{+}\to 渭^{+}谓_渭$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (643 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.07626v1-abstract-short" style="display: inline;"> Using $20.3~\mathrm{fb}^{-1}$ of $e^+e^-$ collision data collected at a center-of-mass energy of $E_{\rm cm}=3.773$ GeV with the BESIII detector operating at the BEPCII collider, we determine the branching fraction of the leptonic decay $D^+\to渭^+谓_渭$ to be $(3.981\pm0.079_{\rm stat}\pm0.040_{\rm syst})\times10^{-4}$. Interpreting our measurement with knowledge of the Fermi coupling constant&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.07626v1-abstract-full').style.display = 'inline'; document.getElementById('2410.07626v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.07626v1-abstract-full" style="display: none;"> Using $20.3~\mathrm{fb}^{-1}$ of $e^+e^-$ collision data collected at a center-of-mass energy of $E_{\rm cm}=3.773$ GeV with the BESIII detector operating at the BEPCII collider, we determine the branching fraction of the leptonic decay $D^+\to渭^+谓_渭$ to be $(3.981\pm0.079_{\rm stat}\pm0.040_{\rm syst})\times10^{-4}$. Interpreting our measurement with knowledge of the Fermi coupling constant $G_F$, the masses of the $D^+$ and $渭^+$ as well as the lifetime of the $D^+$, we determine $f_{D^+}|V_{cd}|=(47.53\pm0.48_{\rm stat}\pm0.24_{\rm syst}\pm0.12_{\rm input})~\mathrm{MeV}$. This result is a factor of 2.3 more precise than the previous best measurement. Using the value of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cd}|$ given by the global standard model fit, we obtain the $D^+$ decay constant $f_{D^+}=(211.5\pm2.3_{\rm stat}\pm1.1_{\rm syst}\pm0.8_{\rm input})$ MeV. Alternatively, using the value of $f_{D^+}$ from a precise lattice quantum chromodynamics calculation, we extract $|V_{cd}|=0.2242\pm0.0023_{\rm stat}\pm0.0011_{\rm syst}\pm0.0009_{\rm input}$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.07626v1-abstract-full').style.display = 'none'; document.getElementById('2410.07626v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 10 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">9 pages, 2 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.07386">arXiv:2410.07386</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.07386">pdf</a>, <a href="https://arxiv.org/format/2410.07386">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Space Physics">physics.space-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Plasma Physics">physics.plasm-ph</span> </div> </div> <p class="title is-5 mathjax"> Nonlinear resonant interactions of radiation belt electrons with intense whistler-mode waves </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Artemyev%2C+A+V">A. V. Artemyev</a>, <a href="/search/?searchtype=author&amp;query=Mourenas%2C+D">D. Mourenas</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+X+-">X. -J. Zhang</a>, <a href="/search/?searchtype=author&amp;query=Agapitov%2C+O">O. Agapitov</a>, <a href="/search/?searchtype=author&amp;query=Neishtadt%2C+A+I">A. I. Neishtadt</a>, <a href="/search/?searchtype=author&amp;query=Vainchtein%2C+D+L">D. L. Vainchtein</a>, <a href="/search/?searchtype=author&amp;query=Vasiliev%2C+A+A">A. A. Vasiliev</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+X">X. Zhang</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Q. Ma</a>, <a href="/search/?searchtype=author&amp;query=Bortnik%2C+J">J. Bortnik</a>, <a href="/search/?searchtype=author&amp;query=Krasnoselskikh%2C+V+V">V. V. Krasnoselskikh</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.07386v1-abstract-short" style="display: inline;"> The dynamics of the Earth&#39;s outer radiation belt, filled by energetic electron fluxes, is largely controlled by electron resonant interactions with electromagnetic whistler-mode waves. The most coherent and intense waves resonantly interact with electrons nonlinearly, and the observable effects of such nonlinear interactions cannot be described within the frame of classical quasi-linear models. Th&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.07386v1-abstract-full').style.display = 'inline'; document.getElementById('2410.07386v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.07386v1-abstract-full" style="display: none;"> The dynamics of the Earth&#39;s outer radiation belt, filled by energetic electron fluxes, is largely controlled by electron resonant interactions with electromagnetic whistler-mode waves. The most coherent and intense waves resonantly interact with electrons nonlinearly, and the observable effects of such nonlinear interactions cannot be described within the frame of classical quasi-linear models. This paper provides an overview of the current stage of the theory of nonlinear resonant interactions and discusses different possible approaches for incorporating these nonlinear interactions into global radiation belt simulations. We focused on observational properties of whistler-mode waves and theoretical aspects of electron nonlinear resonant interactions between such waves and energetic electrons. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.07386v1-abstract-full').style.display = 'none'; document.getElementById('2410.07386v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.06664">arXiv:2410.06664</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.06664">pdf</a>, <a href="https://arxiv.org/format/2410.06664">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Artificial Intelligence">cs.AI</span> </div> </div> <p class="title is-5 mathjax"> Decouple-Then-Merge: Towards Better Training for Diffusion Models </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qianli Ma</a>, <a href="/search/?searchtype=author&amp;query=Ning%2C+X">Xuefei Ning</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+D">Dongrui Liu</a>, <a href="/search/?searchtype=author&amp;query=Niu%2C+L">Li Niu</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+L">Linfeng Zhang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.06664v1-abstract-short" style="display: inline;"> Diffusion models are trained by learning a sequence of models that reverse each step of noise corruption. Typically, the model parameters are fully shared across multiple timesteps to enhance training efficiency. However, since the denoising tasks differ at each timestep, the gradients computed at different timesteps may conflict, potentially degrading the overall performance of image generation.&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.06664v1-abstract-full').style.display = 'inline'; document.getElementById('2410.06664v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.06664v1-abstract-full" style="display: none;"> Diffusion models are trained by learning a sequence of models that reverse each step of noise corruption. Typically, the model parameters are fully shared across multiple timesteps to enhance training efficiency. However, since the denoising tasks differ at each timestep, the gradients computed at different timesteps may conflict, potentially degrading the overall performance of image generation. To solve this issue, this work proposes a Decouple-then-Merge (DeMe) framework, which begins with a pretrained model and finetunes separate models tailored to specific timesteps. We introduce several improved techniques during the finetuning stage to promote effective knowledge sharing while minimizing training interference across timesteps. Finally, after finetuning, these separate models can be merged into a single model in the parameter space, ensuring efficient and practical inference. Experimental results show significant generation quality improvements upon 6 benchmarks including Stable Diffusion on COCO30K, ImageNet1K, PartiPrompts, and DDPM on LSUN Church, LSUN Bedroom, and CIFAR10. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.06664v1-abstract-full').style.display = 'none'; document.getElementById('2410.06664v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.06515">arXiv:2410.06515</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.06515">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Software Engineering">cs.SE</span> </div> </div> <p class="title is-5 mathjax"> Studying Practitioners&#39; Expectations on Clear Code Review Comments </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Li%2C+Z">Zhenhao Li</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+J">Junkai Chen</a>, <a href="/search/?searchtype=author&amp;query=Mao%2C+Q">Qiheng Mao</a>, <a href="/search/?searchtype=author&amp;query=Hu%2C+X">Xing Hu</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+K">Kui Liu</a>, <a href="/search/?searchtype=author&amp;query=Xia%2C+X">Xin Xia</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.06515v1-abstract-short" style="display: inline;"> The code review comment (CRC) is pivotal in the process of modern code review. It provides reviewers with the opportunity to identify potential bugs, offer constructive feedback, and suggest improvements. Clear and concise code review comments (CRCs) facilitate the communication between developers and is crucial to the correct understanding of the issues identified and proposed solutions. Despite&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.06515v1-abstract-full').style.display = 'inline'; document.getElementById('2410.06515v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.06515v1-abstract-full" style="display: none;"> The code review comment (CRC) is pivotal in the process of modern code review. It provides reviewers with the opportunity to identify potential bugs, offer constructive feedback, and suggest improvements. Clear and concise code review comments (CRCs) facilitate the communication between developers and is crucial to the correct understanding of the issues identified and proposed solutions. Despite the importance of CRCs&#39; clarity, there is still a lack of guidelines on what constitutes a good clarity and how to evaluate it. In this paper, we conduct a comprehensive study on understanding and evaluating the clarity of CRCs. We first derive a set of attributes related to the clarity of CRCs, namely RIE attributes (i.e., Relevance, Informativeness, and Expression), as well as their corresponding evaluation criteria based on our literature review and survey with practitioners. We then investigate the clarity of CRCs in open-source projects written in nine programming languages and find that a large portion (i.e., 28.8%) of the CRCs lack the clarity in at least one of the attributes. Finally, we propose ClearCRC, an automated framework that evaluates the clarity of CRCs. Experimental results show that ClearCRC can effectively evaluate the clarity of CRCs and outperform the baselines. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.06515v1-abstract-full').style.display = 'none'; document.getElementById('2410.06515v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.06500">arXiv:2410.06500</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.06500">pdf</a>, <a href="https://arxiv.org/format/2410.06500">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Search for the radiative decays $D^+\to纬蟻^+$ and $D^+\to纬K^{*+}$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (648 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.06500v1-abstract-short" style="display: inline;"> We search for the radiative decays $D^{+} \to 纬蟻^+$ and $D^{+} \to 纬K^{*+}$ using 20.3~fb$^{-1}$ of $e^+e^-$ annihilation data collected at the center-of-mass energy $\sqrt{s}=3.773$ GeV by the BESIII detector operating at the BEPCII collider. No significant signals are observed, and the upper limits on the branching fractions of $D^{+} \to 纬蟻^+$ and $D^{+} \to 纬K^{*+}$ at 90\% confidence level ar&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.06500v1-abstract-full').style.display = 'inline'; document.getElementById('2410.06500v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.06500v1-abstract-full" style="display: none;"> We search for the radiative decays $D^{+} \to 纬蟻^+$ and $D^{+} \to 纬K^{*+}$ using 20.3~fb$^{-1}$ of $e^+e^-$ annihilation data collected at the center-of-mass energy $\sqrt{s}=3.773$ GeV by the BESIII detector operating at the BEPCII collider. No significant signals are observed, and the upper limits on the branching fractions of $D^{+} \to 纬蟻^+$ and $D^{+} \to 纬K^{*+}$ at 90\% confidence level are set to be $1.3\times10^{-5}$ and $1.8\times10^{-5}$, respectively. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.06500v1-abstract-full').style.display = 'none'; document.getElementById('2410.06500v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.05736">arXiv:2410.05736</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.05736">pdf</a>, <a href="https://arxiv.org/ps/2410.05736">ps</a>, <a href="https://arxiv.org/format/2410.05736">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Observation of an axial-vector state in the study of $蠄(3686) \to 蠁畏畏&#39;$ decay </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (625 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.05736v1-abstract-short" style="display: inline;"> Using (2712.4 $\pm$ 14.3)$\times 10^{6}$ $蠄(3686)$ events collected with the BESIII detector at BEPCII, a partial wave analysis of the decay $蠄(3686) \to 蠁畏畏&#39; $ is performed with the covariant tensor approach. An axial-vector state with a mass near 2.3 $\rm GeV/c^2$ is observed for the first time. Its mass and width are measured to be 2316&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.05736v1-abstract-full').style.display = 'inline'; document.getElementById('2410.05736v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.05736v1-abstract-full" style="display: none;"> Using (2712.4 $\pm$ 14.3)$\times 10^{6}$ $蠄(3686)$ events collected with the BESIII detector at BEPCII, a partial wave analysis of the decay $蠄(3686) \to 蠁畏畏&#39; $ is performed with the covariant tensor approach. An axial-vector state with a mass near 2.3 $\rm GeV/c^2$ is observed for the first time. Its mass and width are measured to be 2316 $\pm 9_{\mathrm{stat}} \pm 30_{\mathrm{syst}}\,\rm MeV/c^2$ and 89 $\pm 15_{\mathrm{stat}} \pm 26_{\mathrm{syst}}\,\rm MeV$, respectively. The product branching fractions of $\mathcal{B}(蠄(3686) \to X(2300) 畏&#39;) \mathcal{B}(X(2300)\to 蠁畏)$ and $\mathcal{B}(蠄(3686) \to X(2300) 畏)\mathcal{B}(X(2300)\to 蠁畏&#39;)$ are determined to be (4.8 $\pm 1.3_{\mathrm{stat}} \pm 0.7_{\mathrm{syst}})\times 10^{-6}$ and (2.2 $\pm 0.7_{\mathrm{stat}} \pm 0.7_{\mathrm{syst}})\times 10^{-6}$, respectively. The branching fraction $\mathcal{B}(蠄(3686) \to 蠁畏畏&#39;)$ is measured for the first time to be (3.14$\pm0.17_{\mathrm{stat}}\pm0.24_{\mathrm{syst}})\times10^{-5}$. The first uncertainties are statistical and the second are systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.05736v1-abstract-full').style.display = 'none'; document.getElementById('2410.05736v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.04454">arXiv:2410.04454</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.04454">pdf</a>, <a href="https://arxiv.org/format/2410.04454">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computation and Language">cs.CL</span> </div> </div> <p class="title is-5 mathjax"> CopyLens: Dynamically Flagging Copyrighted Sub-Dataset Contributions to LLM Outputs </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qichao Ma</a>, <a href="/search/?searchtype=author&amp;query=Zhu%2C+R">Rui-Jie Zhu</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+P">Peiye Liu</a>, <a href="/search/?searchtype=author&amp;query=Yan%2C+R">Renye Yan</a>, <a href="/search/?searchtype=author&amp;query=Zhang%2C+F">Fahong Zhang</a>, <a href="/search/?searchtype=author&amp;query=Liang%2C+L">Ling Liang</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+M">Meng Li</a>, <a href="/search/?searchtype=author&amp;query=Yu%2C+Z">Zhaofei Yu</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+Z">Zongwei Wang</a>, <a href="/search/?searchtype=author&amp;query=Cai%2C+Y">Yimao Cai</a>, <a href="/search/?searchtype=author&amp;query=Huang%2C+T">Tiejun Huang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.04454v1-abstract-short" style="display: inline;"> Large Language Models (LLMs) have become pervasive due to their knowledge absorption and text-generation capabilities. Concurrently, the copyright issue for pretraining datasets has been a pressing concern, particularly when generation includes specific styles. Previous methods either focus on the defense of identical copyrighted outputs or find interpretability by individual tokens with computati&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.04454v1-abstract-full').style.display = 'inline'; document.getElementById('2410.04454v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.04454v1-abstract-full" style="display: none;"> Large Language Models (LLMs) have become pervasive due to their knowledge absorption and text-generation capabilities. Concurrently, the copyright issue for pretraining datasets has been a pressing concern, particularly when generation includes specific styles. Previous methods either focus on the defense of identical copyrighted outputs or find interpretability by individual tokens with computational burdens. However, the gap between them exists, where direct assessments of how dataset contributions impact LLM outputs are missing. Once the model providers ensure copyright protection for data holders, a more mature LLM community can be established. To address these limitations, we introduce CopyLens, a new framework to analyze how copyrighted datasets may influence LLM responses. Specifically, a two-stage approach is employed: First, based on the uniqueness of pretraining data in the embedding space, token representations are initially fused for potential copyrighted texts, followed by a lightweight LSTM-based network to analyze dataset contributions. With such a prior, a contrastive-learning-based non-copyright OOD detector is designed. Our framework can dynamically face different situations and bridge the gap between current copyright detection methods. Experiments show that CopyLens improves efficiency and accuracy by 15.2% over our proposed baseline, 58.7% over prompt engineering methods, and 0.21 AUC over OOD detection baselines. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.04454v1-abstract-full').style.display = 'none'; document.getElementById('2410.04454v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 6 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.04425">arXiv:2410.04425</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.04425">pdf</a>, <a href="https://arxiv.org/format/2410.04425">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Astrophysical Phenomena">astro-ph.HE</span> </div> </div> <p class="title is-5 mathjax"> LHAASO detection of very-high-energy gamma-ray emission surrounding PSR J0248+6021 </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Cao%2C+Z">Zhen Cao</a>, <a href="/search/?searchtype=author&amp;query=Aharonian%2C+F">F. Aharonian</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Axikegu"> Axikegu</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y+X">Y. X. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+Y+W">Y. W. Bao</a>, <a href="/search/?searchtype=author&amp;query=Bastieri%2C+D">D. Bastieri</a>, <a href="/search/?searchtype=author&amp;query=Bi%2C+X+J">X. J. Bi</a>, <a href="/search/?searchtype=author&amp;query=Bi%2C+Y+J">Y. J. Bi</a>, <a href="/search/?searchtype=author&amp;query=Cai%2C+J+T">J. T. Cai</a>, <a href="/search/?searchtype=author&amp;query=Cao%2C+Q">Q. Cao</a>, <a href="/search/?searchtype=author&amp;query=Cao%2C+W+Y">W. Y. Cao</a>, <a href="/search/?searchtype=author&amp;query=Cao%2C+Z">Zhe Cao</a>, <a href="/search/?searchtype=author&amp;query=Chang%2C+J">J. Chang</a>, <a href="/search/?searchtype=author&amp;query=Chang%2C+J+F">J. F. Chang</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+A+M">A. M. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+E+S">E. S. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+L">Liang Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+L">Lin Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+L">Long Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+M+J">M. J. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+M+L">M. L. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+Q+H">Q. H. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+S+H">S. H. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+S+Z">S. Z. Chen</a> , et al. (255 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.04425v1-abstract-short" style="display: inline;"> We report the detection of an extended very-high-energy (VHE) gamma-ray source coincident with the locations of middle-aged (62.4~\rm kyr) pulsar PSR J0248+6021, by using the LHAASO-WCDA data of live 796 days and LHAASO-KM2A data of live 1216 days. A significant excess of \gray induced showers is observed both by WCDA in energy bands of 1-25~\rm TeV and KM2A in energy bands of $&gt;$ 25~\rm TeV with&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.04425v1-abstract-full').style.display = 'inline'; document.getElementById('2410.04425v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.04425v1-abstract-full" style="display: none;"> We report the detection of an extended very-high-energy (VHE) gamma-ray source coincident with the locations of middle-aged (62.4~\rm kyr) pulsar PSR J0248+6021, by using the LHAASO-WCDA data of live 796 days and LHAASO-KM2A data of live 1216 days. A significant excess of \gray induced showers is observed both by WCDA in energy bands of 1-25~\rm TeV and KM2A in energy bands of $&gt;$ 25~\rm TeV with 7.3 $蟽$ and 13.5 $蟽$, respectively. The best-fit position derived through WCDA data is R.A. = 42.06$^\circ \pm$ 0.12$^\circ$ and Dec. = 60.24$^\circ \pm $ 0.13$^\circ$ with an extension of 0.69$^\circ\pm$0.15$^\circ$ and that of the KM2A data is R.A.= 42.29$^\circ \pm $ 0.13$^\circ$ and Dec. = 60.38$^\circ \pm$ 0.07$^\circ$ with an extension of 0.37$^\circ\pm$0.07$^\circ$. No clear extended multiwavelength counterpart of this LHAASO source has been found from the radio band to the GeV band. The most plausible explanation of the VHE \gray emission is the inverse Compton process of highly relativistic electrons and positrons injected by the pulsar. These electrons/positrons are hypothesized to be either confined within the pulsar wind nebula or to have already escaped into the interstellar medium, forming a pulsar halo. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.04425v1-abstract-full').style.display = 'none'; document.getElementById('2410.04425v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 6 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">12 pages, 10 figures, Accepted by Sci. China-Phys. Mech. Astron</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.02421">arXiv:2410.02421</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.02421">pdf</a>, <a href="https://arxiv.org/format/2410.02421">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Search for lepton number violating decays of $D_s^+\to h^-h^0e^+e^+$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (650 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.02421v2-abstract-short" style="display: inline;"> Based on 7.33 fb$^{-1}$ of $e^+e^-$ collision data collected by the BESIII detector operating at the BEPCII collider at center-of-mass energies from 4.128 to 4.226 GeV, a search for the Majorana neutrino $谓_m$ is conducted in the lepton-number-violating decays of $D_s^+\to h^-h^0e^+e^+$. Here, $h^-$ represents a $K^-$ or $蟺^-$, and $h^0$ represents a $蟺^0$, $K_S^0$ or $蠁$. No significant signal is&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.02421v2-abstract-full').style.display = 'inline'; document.getElementById('2410.02421v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.02421v2-abstract-full" style="display: none;"> Based on 7.33 fb$^{-1}$ of $e^+e^-$ collision data collected by the BESIII detector operating at the BEPCII collider at center-of-mass energies from 4.128 to 4.226 GeV, a search for the Majorana neutrino $谓_m$ is conducted in the lepton-number-violating decays of $D_s^+\to h^-h^0e^+e^+$. Here, $h^-$ represents a $K^-$ or $蟺^-$, and $h^0$ represents a $蟺^0$, $K_S^0$ or $蠁$. No significant signal is observed, and the upper limits of their branching fractions at the 90\% confidence level are determined to be $\mathcal{B}(D_s^+\to 蠁蟺^-e^+e^+) &lt; 6.9 \times 10^{-5}$, $\mathcal{B}(D_s^+\to 蠁K^-e^+e^+) &lt; 9.9 \times 10^{-5}$, $\mathcal{B}(D_s^+\to K_S^0蟺^-e^+e^+) &lt; 1.3 \times 10^{-5}$, $\mathcal{B}(D_s^+\to K_S^0K^-e^+e^+) &lt; 2.9 \times 10^{-5}$, $\mathcal{B}(D_s^+\to 蟺^-蟺^0e^+e^+) &lt; 2.9 \times 10^{-5}$ and $\mathcal{B}(D_s^+\to K^-蟺^0e^+e^+) &lt; 3.4 \times 10^{-5}$. The Majorana neutrino is searched for with different mass assumptions within the range [0.20, 0.80] GeV$/c^2$ in the decay of $D_s^+\to蠁e^+谓_m$ with $谓_m\to蟺^-e^+$, and the upper limits of the branching fractions at the 90\% confidence level are at the level of $10^{-5}-10^{-2}$, depending on the mass of the Majorana neutrino. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.02421v2-abstract-full').style.display = 'none'; document.getElementById('2410.02421v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 20 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 3 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.00379">arXiv:2410.00379</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.00379">pdf</a>, <a href="https://arxiv.org/format/2410.00379">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Artificial Intelligence">cs.AI</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Machine Learning">cs.LG</span> </div> </div> <p class="title is-5 mathjax"> CXPMRG-Bench: Pre-training and Benchmarking for X-ray Medical Report Generation on CheXpert Plus Dataset </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Wang%2C+X">Xiao Wang</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+F">Fuling Wang</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+Y">Yuehang Li</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qingchuan Ma</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+S">Shiao Wang</a>, <a href="/search/?searchtype=author&amp;query=Jiang%2C+B">Bo Jiang</a>, <a href="/search/?searchtype=author&amp;query=Li%2C+C">Chuanfu Li</a>, <a href="/search/?searchtype=author&amp;query=Tang%2C+J">Jin Tang</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2410.00379v1-abstract-short" style="display: inline;"> X-ray image-based medical report generation (MRG) is a pivotal area in artificial intelligence which can significantly reduce diagnostic burdens and patient wait times. Despite significant progress, we believe that the task has reached a bottleneck due to the limited benchmark datasets and the existing large models&#39; insufficient capability enhancements in this specialized domain. Specifically, the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.00379v1-abstract-full').style.display = 'inline'; document.getElementById('2410.00379v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.00379v1-abstract-full" style="display: none;"> X-ray image-based medical report generation (MRG) is a pivotal area in artificial intelligence which can significantly reduce diagnostic burdens and patient wait times. Despite significant progress, we believe that the task has reached a bottleneck due to the limited benchmark datasets and the existing large models&#39; insufficient capability enhancements in this specialized domain. Specifically, the recently released CheXpert Plus dataset lacks comparative evaluation algorithms and their results, providing only the dataset itself. This situation makes the training, evaluation, and comparison of subsequent algorithms challenging. Thus, we conduct a comprehensive benchmarking of existing mainstream X-ray report generation models and large language models (LLMs), on the CheXpert Plus dataset. We believe that the proposed benchmark can provide a solid comparative basis for subsequent algorithms and serve as a guide for researchers to quickly grasp the state-of-the-art models in this field. More importantly, we propose a large model for the X-ray image report generation using a multi-stage pre-training strategy, including self-supervised autoregressive generation and Xray-report contrastive learning, and supervised fine-tuning. Extensive experimental results indicate that the autoregressive pre-training based on Mamba effectively encodes X-ray images, and the image-text contrastive pre-training further aligns the feature spaces, achieving better experimental results. Source code can be found on \url{https://github.com/Event-AHU/Medical_Image_Analysis}. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.00379v1-abstract-full').style.display = 'none'; document.getElementById('2410.00379v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 1 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">In Peer Review</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2409.19976">arXiv:2409.19976</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.19976">pdf</a>, <a href="https://arxiv.org/format/2409.19976">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Machine Learning">cs.LG</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Numerical Analysis">math.NA</span> </div> </div> <p class="title is-5 mathjax"> Learning Partial Differential Equations with Deep Parallel Neural Operator </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qinglong Ma</a>, <a href="/search/?searchtype=author&amp;query=Zhao%2C+P">Peizhi Zhao</a>, <a href="/search/?searchtype=author&amp;query=Wang%2C+S">Sen Wang</a>, <a href="/search/?searchtype=author&amp;query=Song%2C+T">Tao Song</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2409.19976v2-abstract-short" style="display: inline;"> In recent years, Solving partial differential equations has shifted the focus of traditional neural network studies from finite-dimensional Euclidean spaces to generalized functional spaces in research. A novel methodology is to learn an operator as a means of approximating the mapping between outputs. Currently, researchers have proposed a variety of operator architectures. Nevertheless, the majo&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.19976v2-abstract-full').style.display = 'inline'; document.getElementById('2409.19976v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.19976v2-abstract-full" style="display: none;"> In recent years, Solving partial differential equations has shifted the focus of traditional neural network studies from finite-dimensional Euclidean spaces to generalized functional spaces in research. A novel methodology is to learn an operator as a means of approximating the mapping between outputs. Currently, researchers have proposed a variety of operator architectures. Nevertheless, the majority of these architectures adopt an iterative update architecture, whereby a single operator is learned from the same function space. In practical physical science problems, the numerical solutions of partial differential equations are complex, and a serial single operator is unable to accurately approximate the intricate mapping between input and output. So, We propose a deep parallel operator model (DPNO) for efficiently and accurately solving partial differential equations. DPNO employs convolutional neural networks to extract local features and map data into distinct latent spaces. Designing a parallel block of double Fourier neural operators to solve the iterative error problem. DPNO approximates complex mappings between inputs and outputs by learning multiple operators in different potential spaces in parallel blocks. DPNO achieved the best performance on five of them, with an average improvement of 10.5\%, and ranked second on one dataset. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.19976v2-abstract-full').style.display = 'none'; document.getElementById('2409.19976v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 7 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 30 September, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2409.17752">arXiv:2409.17752</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.17752">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Mesoscale and Nanoscale Physics">cond-mat.mes-hall</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Materials Science">cond-mat.mtrl-sci</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Optics">physics.optics</span> </div> </div> <p class="title is-5 mathjax"> Observation of Transient Trion Induced by Ultrafast Charge Transfer in Graphene/MoS2 Heterostructure </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Wang%2C+C">Chen Wang</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+Y">Yu Chen</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+Q">Qiushi Ma</a>, <a href="/search/?searchtype=author&amp;query=Suo%2C+P">Peng Suo</a>, <a href="/search/?searchtype=author&amp;query=Sun%2C+K">Kaiwen Sun</a>, <a href="/search/?searchtype=author&amp;query=Cheng%2C+Y">Yifan Cheng</a>, <a href="/search/?searchtype=author&amp;query=Lin%2C+X">Xian Lin</a>, <a href="/search/?searchtype=author&amp;query=Liu%2C+W">Weimin Liu</a>, <a href="/search/?searchtype=author&amp;query=Ma%2C+G">Guohong Ma</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2409.17752v1-abstract-short" style="display: inline;"> Van der Waals (Vdw) heterostructures constructed from TMDCs provide an ideal platform for exploring various quasiparticle behaviors, with trion-composed of neutral exciton and charged carrier-being a notable example. There are typically three methods to generate trion: electrical doping, chemical doping, and direct optical doping. The first two methods generate static trion, while the last gives r&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.17752v1-abstract-full').style.display = 'inline'; document.getElementById('2409.17752v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.17752v1-abstract-full" style="display: none;"> Van der Waals (Vdw) heterostructures constructed from TMDCs provide an ideal platform for exploring various quasiparticle behaviors, with trion-composed of neutral exciton and charged carrier-being a notable example. There are typically three methods to generate trion: electrical doping, chemical doping, and direct optical doping. The first two methods generate static trion, while the last gives rise to transient trion. Here, we present an indirect optical doping approach to generate transient trion via ultrafast charge transfer (CT) and achieve control over the trion-to-exciton ratio by adjusting CT in Gr/MoS2 heterostructure. Furthermore, we demonstrated that dynamics of the transient trion generated with this method, which shows slightly longer lifetime than that of exciton accounted for the Coulomb interactions between trion and charged defect. This study provides fresh perspectives on the construction of new quasiparticles, dynamical characterization and the control of the many-body interaction in two-dimensional structure. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.17752v1-abstract-full').style.display = 'none'; document.getElementById('2409.17752v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 26 September, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">16 pages, 4 figures</span> </p> </li> </ol> <nav class="pagination is-small is-centered breathe-horizontal" role="navigation" aria-label="pagination"> <a href="" class="pagination-previous 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