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name="order"><option selected value="-announced_date_first">Announcement date (newest first)</option><option value="announced_date_first">Announcement date (oldest first)</option><option value="-submitted_date">Submission date (newest first)</option><option value="submitted_date">Submission date (oldest first)</option><option value="">Relevance</option></select> </span> </div> <div class="control"> <button class="button is-small is-link">Go</button> </div> </div> </form> </div> </div> <ol class="breathe-horizontal" start="1"> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.12554">arXiv:2411.12554</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.12554">pdf</a>, <a href="https://arxiv.org/format/2411.12554">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 - Lattice">hep-lat</span> </div> </div> <p class="title is-5 mathjax"> Light Cone Distribution Amplitude for the $螞$ Baryon from Lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Chu%2C+M">Min-Huan Chu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bai%2C+H">Haoyang Bai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Liang%2C+J">Jian Liang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Schafer%2C+A">Andreas Schafer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Su%2C+Y">Yushan Su</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zeng%2C+J">Jun Zeng</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jian-Hui Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An 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="2411.12554v1-abstract-short" style="display: inline;"> We calculate the leading-twist light-cone distribution amplitudes of the light $螞$ baryon using lattice methods within the framework of large momentum effective theory. Our numerical computations are conducted employing $N_f=2+1$ stout smeared clover fermions and a Symanzik gauge action on a lattice with spacing $a=0.077\;\rm{fm}$, and a pion mass of 303 MeV. To approach the large momentum regime,&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.12554v1-abstract-full').style.display = 'inline'; document.getElementById('2411.12554v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.12554v1-abstract-full" style="display: none;"> We calculate the leading-twist light-cone distribution amplitudes of the light $螞$ baryon using lattice methods within the framework of large momentum effective theory. Our numerical computations are conducted employing $N_f=2+1$ stout smeared clover fermions and a Symanzik gauge action on a lattice with spacing $a=0.077\;\rm{fm}$, and a pion mass of 303 MeV. To approach the large momentum regime, we simulate the equal-time correlations with the hadron momentum $P^z = \{2.52, 3.02, 3.52\}$ GeV. By investigating the potential analytic characteristics of the baryon quasi-distribution amplitude in coordinate space, we validate these findings through our lattice calculations. After renormalization and extrapolation, we present results for the three-dimensional distribution of momentum fractions for the two light quarks. Based on these findings the paper briefly discusses the phenomenological impact on weak decays of $螞_b$, and outlines potential systematic uncertainties that can be improved in the future. This work lays the theoretical foundation for accessing baryon LCDAs from lattice QCD. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.12554v1-abstract-full').style.display = 'none'; document.getElementById('2411.12554v1-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> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.18654">arXiv:2410.18654</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.18654">pdf</a>, <a href="https://arxiv.org/format/2410.18654">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 - Lattice">hep-lat</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"> Calculation of heavy meson light-cone distribution amplitudes from lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Han%2C+X">Xue-Ying Han</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=L%C3%BC%2C+C">Cai-Dian L眉</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sch%C3%A4fer%2C+A">Andreas Sch盲fer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Su%2C+Y">Yushan Su</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Xu%2C+J">Ji Xu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yibo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jian-Hui Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhao%2C+S">Shuai 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="2410.18654v1-abstract-short" style="display: inline;"> We develop an approach for calculating heavy quark effective theory (HQET) light-cone distribution amplitudes (LCDAs) by employing a sequential effective theory methodology. The theoretical foundation of the framework is established, elucidating how the quasi distribution amplitudes (quasi DAs) with three scales can be utilized to compute HQET LCDAs. We provide theoretical support for this approac&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.18654v1-abstract-full').style.display = 'inline'; document.getElementById('2410.18654v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.18654v1-abstract-full" style="display: none;"> We develop an approach for calculating heavy quark effective theory (HQET) light-cone distribution amplitudes (LCDAs) by employing a sequential effective theory methodology. The theoretical foundation of the framework is established, elucidating how the quasi distribution amplitudes (quasi DAs) with three scales can be utilized to compute HQET LCDAs. We provide theoretical support for this approach by demonstrating the rationale behind devising a hierarchical ordering for the three involved scales, discussing the factorization at each step, clarifying the underlying reason for obtaining HQET LCDAs in the final phase, and addressing potential theoretical challenges. The lattice QCD simulation aspect is explored in detail, and the computations of quasi DAs are presented. We employ three fitting strategies to handle contributions from excited states and extract the bare matrix elements. For renormalization purposes, we apply hybrid renormalization schemes at short and long distance separations. To mitigate long-distance perturbations, we perform an extrapolation in $位= z\cdot P^z$ and assess the stability against various parameters. After two-step matching, our results for HQET LCDAs are found in agreement with existing model parametrizations. The potential phenomenological implications of the results are discussed, shedding light on how these findings could impact our understanding of the strong interaction dynamics and physics beyond the standard model. It should be noted, however, that systematic uncertainties have not been accounted for yet. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.18654v1-abstract-full').style.display = 'none'; document.getElementById('2410.18654v1-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> <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">27 pages, 23 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/2403.17492">arXiv:2403.17492</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2403.17492">pdf</a>, <a href="https://arxiv.org/format/2403.17492">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 - Phenomenology">hep-ph</span> <span class="tag is-small is-grey 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> </div> </div> <p class="title is-5 mathjax"> A new method to access heavy meson lightcone distribution amplitudes from first-principle </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Han%2C+X">Xue-Ying Han</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=L%C3%BC%2C+C">Cai-Dian L眉</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Xu%2C+J">Ji Xu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhao%2C+S">Shuai 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="2403.17492v1-abstract-short" style="display: inline;"> We present a method to compute lightcone distribution amplitudes (LCDAs) of heavy meson within heavy quark effective theory (HQET). Our method utilizes quasi distribution amplitudes (quasi-DAs) with a large momentum component $P^z$. We point out that by sequentially integrating out $P^z$ and $m_H$, one can disentangle different dynamical scales. Integrating out $P^z$ allows to connect quasi-DAs to&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2403.17492v1-abstract-full').style.display = 'inline'; document.getElementById('2403.17492v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2403.17492v1-abstract-full" style="display: none;"> We present a method to compute lightcone distribution amplitudes (LCDAs) of heavy meson within heavy quark effective theory (HQET). Our method utilizes quasi distribution amplitudes (quasi-DAs) with a large momentum component $P^z$. We point out that by sequentially integrating out $P^z$ and $m_H$, one can disentangle different dynamical scales. Integrating out $P^z$ allows to connect quasi-DAs to QCD LCDAs, and then integrating out $m_H$ enables to relate QCD LCDAs to HQET LCDAs. To verify this proposal, we make use of lattice QCD simulation on a lattice ensemble with spacing $a = 0.05187$\,fm. The preliminary findings for HQET LCDAs qualitatively align with phenomenological models. Using a recent model for HQET LCDAs, we also fit the first inverse moment $位_B^{-1}$ and the result is consistent with the experimentally constrain from $B \to 纬\ell谓_\ell$. This agreement demonstrates the promise of our method in providing first-principle predictions for heavy meson LCDAs. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2403.17492v1-abstract-full').style.display = 'none'; document.getElementById('2403.17492v1-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 March, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 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">6.5 +1.5 pages, 4 +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/2310.02179">arXiv:2310.02179</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2310.02179">pdf</a>, <a href="https://arxiv.org/format/2310.02179">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 - Lattice">hep-lat</span> </div> </div> <p class="title is-5 mathjax"> Fast Fermion Smearing Scheme with Gaussian-like Profile </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Li%2C+C">ChuanYang Li</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Draper%2C+T">Terrence Draper</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Liang%2C+J">Jian Liang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Liu%2C+K">Keh-Fei Liu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Shi%2C+J">Jun Shi</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+N">Nan Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-bo Yang</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="2310.02179v3-abstract-short" style="display: inline;"> We propose a novel smearing scheme which gives a Gaussian-like profile and is more efficient than the traditional Gaussian smearing in terms of computer time consumption. We also carry out a detailed analysis of the profiles, smearing sizes, and the behaviors of hadron effective masses of different smearing schemes, and point out that having a sufficient number of gauge paths in a smearing scheme&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2310.02179v3-abstract-full').style.display = 'inline'; document.getElementById('2310.02179v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2310.02179v3-abstract-full" style="display: none;"> We propose a novel smearing scheme which gives a Gaussian-like profile and is more efficient than the traditional Gaussian smearing in terms of computer time consumption. We also carry out a detailed analysis of the profiles, smearing sizes, and the behaviors of hadron effective masses of different smearing schemes, and point out that having a sufficient number of gauge paths in a smearing scheme is essential to produce strong smearing effects. For a moderate smearing size $\bar{r}\sim 10a$, the time cost for the novel smearing is less than $1/8$ of that for the traditional Gaussian smearing. In practical lattice calculations with larger smearing sizes or finer lattice spacings the improvement will be more substantial. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2310.02179v3-abstract-full').style.display = 'none'; document.getElementById('2310.02179v3-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> 27 February, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 3 October, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2023. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2306.06488">arXiv:2306.06488</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2306.06488">pdf</a>, <a href="https://arxiv.org/format/2306.06488">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 - Lattice">hep-lat</span> <span class="tag is-small is-grey 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 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/10.1007/JHEP08(2023)172">10.1007/JHEP08(2023)172 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Lattice Calculation of the Intrinsic Soft Function and the Collins-Soper Kernel </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Lattice+Parton+Collaboration"> Lattice Parton Collaboration</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Chu%2C+M">Min-Huan Chu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=He%2C+J">Jin-Chen He</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Liang%2C+J">Jian Liang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sch%C3%A4fer%2C+A">Andreas Sch盲fer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Shu%2C+H">Hai-Tao Shu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Su%2C+Y">Yushan Su</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Walter%2C+L">Lisa Walter</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+J">Ji-Hao Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zeng%2C+J">Jun Zeng</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An 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="2306.06488v3-abstract-short" style="display: inline;"> We calculate the soft function using lattice QCD in the framework of large momentum effective theory incorporating the one-loop perturbative contributions. The soft function is a crucial ingredient in the lattice determination of light cone objects using transverse-momentum-dependent (TMD) factorization. It consists of a rapidity-independent part called intrinsic soft function and a rapidity-depen&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2306.06488v3-abstract-full').style.display = 'inline'; document.getElementById('2306.06488v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2306.06488v3-abstract-full" style="display: none;"> We calculate the soft function using lattice QCD in the framework of large momentum effective theory incorporating the one-loop perturbative contributions. The soft function is a crucial ingredient in the lattice determination of light cone objects using transverse-momentum-dependent (TMD) factorization. It consists of a rapidity-independent part called intrinsic soft function and a rapidity-dependent part called Collins-Soper kernel. We have adopted appropriate normalization when constructing the pseudo-scalar meson form factor that is needed in the determination of the intrinsic part and applied Fierz rearrangement to suppress the higher-twist effects. In the calculation of CS kernel we consider a CLS ensemble other than the MILC ensemble used in a previous study. We have also compared the applicability of determining the CS kernel using quasi TMDWFs and quasi TMDPDFs. As an example, the determined soft function is used to obtain the physical TMD wave functions (WFs) of pion and unpolarized iso-vector TMD parton distribution functions (PDFs) of proton. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2306.06488v3-abstract-full').style.display = 'none'; document.getElementById('2306.06488v3-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> 28 August, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 10 June, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 2023. </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">24 pages, 19 figures, published version</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JHEP08(2023)172 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2302.09961">arXiv:2302.09961</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2302.09961">pdf</a>, <a href="https://arxiv.org/format/2302.09961">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 - Lattice">hep-lat</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"> Transverse-Momentum-Dependent Wave Functions of Pion from Lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Chu%2C+M">Min-Huan Chu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=He%2C+J">Jin-Chen He</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Liang%2C+J">Jian Liang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Schafer%2C+A">Andreas Schafer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Shu%2C+H">Hai-Tao Shu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Su%2C+Y">Yushan Su</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+J">Ji-Hao Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zeng%2C+J">Jun Zeng</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jian-Hui Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An 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="2302.09961v1-abstract-short" style="display: inline;"> We present a first lattice QCD calculation of the transverse-momentum-dependent wave functions (TMDWFs) of the pion using large-momentum effective theory. Numerical simulations are based on one ensemble with 2+1+1 flavors of highly improved staggered quarks action with lattice spacing $a=0.121$~fm from the MILC Collaboration, and one with 2 +1 flavor clover fermions and tree-level Symanzik gauge a&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2302.09961v1-abstract-full').style.display = 'inline'; document.getElementById('2302.09961v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2302.09961v1-abstract-full" style="display: none;"> We present a first lattice QCD calculation of the transverse-momentum-dependent wave functions (TMDWFs) of the pion using large-momentum effective theory. Numerical simulations are based on one ensemble with 2+1+1 flavors of highly improved staggered quarks action with lattice spacing $a=0.121$~fm from the MILC Collaboration, and one with 2 +1 flavor clover fermions and tree-level Symanzik gauge action generated by the CLS Collaboration with $a=0.098$~fm. As a key ingredient, the soft function is first obtained by incorporating the one-loop perturbative contributions and a proper normalization. Based on this and the equal-time quasi-TMDWFs simulated on the lattice, we extract the light-cone TMDWFs. The results are comparable between the two lattice ensembles and a comparison with phenomenological parametrization is made. Our studies provide a first attempt of $ab$ $initio$ calculation of TMDWFs which will eventually lead to crucial theory inputs for making predictions for exclusive processes under QCD factorization. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2302.09961v1-abstract-full').style.display = 'none'; document.getElementById('2302.09961v1-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 February, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2023. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2211.02340">arXiv:2211.02340</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2211.02340">pdf</a>, <a href="https://arxiv.org/format/2211.02340">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 - Lattice">hep-lat</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"> Unpolarized Transverse-Momentum-Dependent Parton Distributions of the Nucleon from Lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Lattice+Parton+Collaboration"> Lattice Parton Collaboration</a>, <a href="/search/hep-lat?searchtype=author&amp;query=He%2C+J">Jin-Chen He</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Chu%2C+M">Min-Huan Chu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sch%C3%A4fer%2C+A">Andreas Sch盲fer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Su%2C+Y">Yushan Su</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yibo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jian-Hui Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An 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="2211.02340v3-abstract-short" style="display: inline;"> We present a first lattice QCD calculation of the unpolarized nucleon&#39;s isovector transverse-momentum-dependent parton distribution functions (TMDPDFs), which are essential to predict observables of multi-scale, semi-inclusive processes in the standard model. We use a $N_f=2+1+1$ MILC ensemble with valence clover fermions on a highly improved staggered quark (HISQ) sea to compute the quark momentu&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2211.02340v3-abstract-full').style.display = 'inline'; document.getElementById('2211.02340v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2211.02340v3-abstract-full" style="display: none;"> We present a first lattice QCD calculation of the unpolarized nucleon&#39;s isovector transverse-momentum-dependent parton distribution functions (TMDPDFs), which are essential to predict observables of multi-scale, semi-inclusive processes in the standard model. We use a $N_f=2+1+1$ MILC ensemble with valence clover fermions on a highly improved staggered quark (HISQ) sea to compute the quark momentum distributions in a large-momentum nucleon on the lattice. The state-of-the-art techniques in renormalization and extrapolation in the correlation distance on the lattice are adopted. {The perturbative kernel up to next-to-next-to-leading order is taken into account}, and the dependence on the pion mass and the hadron momentum is explored. Our results are qualitatively comparable with phenomenological TMDPDFs, which provide an opportunity to predict high energy scatterings from first principles. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2211.02340v3-abstract-full').style.display = 'none'; document.getElementById('2211.02340v3-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 May, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 4 November, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2022. </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, 20 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/2208.08008">arXiv:2208.08008</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2208.08008">pdf</a>, <a href="https://arxiv.org/format/2208.08008">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 - Lattice">hep-lat</span> </div> </div> <p class="title is-5 mathjax"> Nucleon Transversity Distribution in the Continuum and Physical Mass Limit from Lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Yao%2C+F">Fei Yao</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Walter%2C+L">Lisa Walter</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Chen%2C+J">Jiunn-Wei Chen</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Jin%2C+L">Luchang Jin</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Lahrtz%2C+S">Sebastian Lahrtz</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ma%2C+L">Lingquan Ma</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Mohanta%2C+P">Protick Mohanta</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sch%C3%A4fer%2C+A">Andreas Sch盲fer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Shu%2C+H">Hai-Tao Shu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Su%2C+Y">Yushan Su</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sun%2C+P">Peng Sun</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Xiong%2C+X">Xiaonu Xiong</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jian-Hui 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="2208.08008v2-abstract-short" style="display: inline;"> We report a state-of-the-art lattice QCD calculation of the isovector quark transversity distribution of the proton in the continuum and physical mass limit using large-momentum effective theory. The calculation is done at four lattice spacings $a=\{0.098,0.085,0.064,0.049\}$~fm and various pion masses ranging between $220$ and $350$ MeV, with proton momenta up to $2.8$ GeV. The result is non-pert&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2208.08008v2-abstract-full').style.display = 'inline'; document.getElementById('2208.08008v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2208.08008v2-abstract-full" style="display: none;"> We report a state-of-the-art lattice QCD calculation of the isovector quark transversity distribution of the proton in the continuum and physical mass limit using large-momentum effective theory. The calculation is done at four lattice spacings $a=\{0.098,0.085,0.064,0.049\}$~fm and various pion masses ranging between $220$ and $350$ MeV, with proton momenta up to $2.8$ GeV. The result is non-perturbatively renormalized in the hybrid scheme with self renormalization which treats the infrared physics at large correlation distance properly, and extrapolated to the continuum, physical mass and infinite momentum limit. We also compare with recent global analyses for the nucleon isovector quark transversity distribution. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2208.08008v2-abstract-full').style.display = 'none'; document.getElementById('2208.08008v2-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 February, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 August, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2022. </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, 18 figures, 2 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/2204.00200">arXiv:2204.00200</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2204.00200">pdf</a>, <a href="https://arxiv.org/ps/2204.00200">ps</a>, <a href="https://arxiv.org/format/2204.00200">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 - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-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/10.1103/PhysRevD.106.034509">10.1103/PhysRevD.106.034509 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Nonperturbative Determination of Collins-Soper Kernel from Quasi Transverse-Momentum Dependent Wave Functions </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Chu%2C+M">Min-Huan Chu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Deng%2C+Z">Zhi-Fu Deng</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sch%C3%A4fer%2C+A">Andreas Sch盲fer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Su%2C+Y">Yushan Su</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sun%2C+P">Peng Sun</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zeng%2C+J">Jun Zeng</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jialu Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jian-Hui Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An 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="2204.00200v1-abstract-short" style="display: inline;"> In the framework of large-momentum effective theory at one-loop matching accuracy, we perform a lattice calculation of the Collins-Soper kernel which governs the rapidity evolution of transverse-momentum-dependent (TMD) distributions. We first obtain the quasi TMD wave functions at three different meson momenta on a lattice with valence clover quarks on a dynamical HISQ sea and lattice spacing&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2204.00200v1-abstract-full').style.display = 'inline'; document.getElementById('2204.00200v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2204.00200v1-abstract-full" style="display: none;"> In the framework of large-momentum effective theory at one-loop matching accuracy, we perform a lattice calculation of the Collins-Soper kernel which governs the rapidity evolution of transverse-momentum-dependent (TMD) distributions. We first obtain the quasi TMD wave functions at three different meson momenta on a lattice with valence clover quarks on a dynamical HISQ sea and lattice spacing $a=0.12$~fm from MILC, and renormalize the pertinent linear divergences using Wilson loops. Through one-loop matching to the light-cone wave functions, we determine the Collins-Soper kernel with transverse separation up to 0.6~fm. We study the systematic uncertainties from operator mixing and scale dependence, as well as the impact from higher power corrections. Our results potentially allow for a determination of the soft function and other transverse-momentum dependent quantities at one-loop accuracy. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2204.00200v1-abstract-full').style.display = 'none'; document.getElementById('2204.00200v1-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 April, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2022. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2201.09173">arXiv:2201.09173</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2201.09173">pdf</a>, <a href="https://arxiv.org/format/2201.09173">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 - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-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/10.1103/PhysRevLett.129.132001">10.1103/PhysRevLett.129.132001 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Pion and Kaon Distribution Amplitudes from Lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Chu%2C+M">Min-Huan Chu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=He%2C+J">Jin-Chen He</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sch%C3%A4fer%2C+A">Andreas Sch盲fer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Su%2C+Y">Yushan Su</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sun%2C+P">Peng Sun</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Xu%2C+J">Ji Xu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yao%2C+F">Fei Yao</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jian-Hui Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An 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="2201.09173v1-abstract-short" style="display: inline;"> We present the state-of-the-art lattice QCD calculation of the pion and kaon light-cone distribution amplitudes (DAs) using large-momentum effective theory. The calculation is done at three lattice spacings $a\approx\{0.06,0.09,0.12\}$ fm and physical pion and kaon masses, with the meson momenta $P_z = \{1.29,1.72,2.15\}$ GeV. The result is non-perturbatively renormalized in a recently proposed hy&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2201.09173v1-abstract-full').style.display = 'inline'; document.getElementById('2201.09173v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2201.09173v1-abstract-full" style="display: none;"> We present the state-of-the-art lattice QCD calculation of the pion and kaon light-cone distribution amplitudes (DAs) using large-momentum effective theory. The calculation is done at three lattice spacings $a\approx\{0.06,0.09,0.12\}$ fm and physical pion and kaon masses, with the meson momenta $P_z = \{1.29,1.72,2.15\}$ GeV. The result is non-perturbatively renormalized in a recently proposed hybrid scheme with self renormalization, and extrapolated to the continuum as well as the infinite momentum limit. We find a significant deviation of the pion and kaon DAs from the asymptotic form, and a large $SU(3)$ flavor breaking effect in the kaon DA. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2201.09173v1-abstract-full').style.display = 'none'; document.getElementById('2201.09173v1-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 January, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2022. </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,18 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/2103.07064">arXiv:2103.07064</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2103.07064">pdf</a>, <a href="https://arxiv.org/ps/2103.07064">ps</a>, <a href="https://arxiv.org/format/2103.07064">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 - Lattice">hep-lat</span> <span class="tag is-small is-grey 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 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/10.1088/1674-1137/ac2b12">10.1088/1674-1137/ac2b12 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> First Lattice QCD determination of semileptonic decays of charmed-strange baryons $螢_c$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Huang%2C+F">Fei Huang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Li%2C+R">Renbo Li</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Li%2C+Y">Yuanyuan Li</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Lu%2C+C">Cai-Dian Lu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sun%2C+P">Peng Sun</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sun%2C+W">Wei Sun</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</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="2103.07064v2-abstract-short" style="display: inline;"> While the standard model is the most successfully theory to describe all interactions and constituents in elementary particle physics, it has been constantly examined for over four decades. Weak decays of charm quarks can measure the coupling strength of quarks in different families and serve as an ideal probe for CP violation. As the lowest charm-strange baryons with three different flavors,&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2103.07064v2-abstract-full').style.display = 'inline'; document.getElementById('2103.07064v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2103.07064v2-abstract-full" style="display: none;"> While the standard model is the most successfully theory to describe all interactions and constituents in elementary particle physics, it has been constantly examined for over four decades. Weak decays of charm quarks can measure the coupling strength of quarks in different families and serve as an ideal probe for CP violation. As the lowest charm-strange baryons with three different flavors, $螢_c$ baryons (made of $csu$ or $csd$) have been extensively studied in experiments at the large hadron collider and in electron-positron collision. However the lack of reliable knowledge in theory becomes the unavoidable obstacle in the way. In this work, we use the state-of-the-art Lattice QCD techniques, and generate 2+1 clover fermion ensembles with two lattice spacings, $a=(0.108{\rm fm},0.080{\rm fm})$. We then present the first {\it ab-initio} lattice QCD determination of form factors governing $螢_{c}\to 螢\ell^+谓_{\ell}$, analogous with the notable $尾$-decay of nuclei. Our theoretical results for decay widths are consistent with and about two times more precise than the latest measurements by ALICE and Belle collaborations. Together with experimental measurements, we independently determine the quark-mixing matrix element $|V_{cs}|$, which is found in good agreement with other determinations. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2103.07064v2-abstract-full').style.display = 'none'; document.getElementById('2103.07064v2-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 January, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 11 March, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2021. </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">6+1 pages, 4 figures; v2: 7 pages, corrected typos</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Chinese Physics C 46, 011002(2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.09788">arXiv:2011.09788</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.09788">pdf</a>, <a href="https://arxiv.org/format/2011.09788">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 - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-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/10.1103/PhysRevLett.127.062002">10.1103/PhysRevLett.127.062002 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Distribution Amplitudes of $K^*$ and $蠁$ at Physical Pion Mass from Lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Chu%2C+M">Min-Huan Chu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sun%2C+P">Peng Sun</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Xu%2C+J">Ji Xu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+J">Jian-Hui Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An 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="2011.09788v2-abstract-short" style="display: inline;"> We present the first lattice QCD calculation of the distribution amplitudes of longitudinally and transversely polarized vector mesons $K^*$ and $蠁$ using large momentum effective theory. We use the clover fermion action on three ensembles with 2+1+1 flavors of highly improved staggered quarks (HISQ) action, generated by MILC collaboration, at physical pion mass and \{0.06, 0.09, 0.12\} fm lattice&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.09788v2-abstract-full').style.display = 'inline'; document.getElementById('2011.09788v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.09788v2-abstract-full" style="display: none;"> We present the first lattice QCD calculation of the distribution amplitudes of longitudinally and transversely polarized vector mesons $K^*$ and $蠁$ using large momentum effective theory. We use the clover fermion action on three ensembles with 2+1+1 flavors of highly improved staggered quarks (HISQ) action, generated by MILC collaboration, at physical pion mass and \{0.06, 0.09, 0.12\} fm lattice spacings, and choose three different hadron momenta $P_z=\{1.29, 1.72, 2.15\}$ GeV. The resulting lattice matrix elements are nonperturbatively renormalized in a hybrid scheme proposed recently. An extrapolation to the continuum and infinite momentum limit is carried out. We find that while the longitudinal distribution amplitudes tend to be close to the asymptotic form, the transverse ones deviate rather significantly from the asymptotic form. Our final results provide crucial {\it ab initio} theory inputs for analyzing pertinent exclusive processes. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.09788v2-abstract-full').style.display = 'none'; document.getElementById('2011.09788v2-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 January, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 19 November, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2020. </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">6+3 pages; 5 + 6 figures; v2: 7+6 pages, expanded discussions</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 127, 062002 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2005.14572">arXiv:2005.14572</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2005.14572">pdf</a>, <a href="https://arxiv.org/format/2005.14572">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 - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-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/10.1103/PhysRevLett.125.192001">10.1103/PhysRevLett.125.192001 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Lattice-QCD Calculations of TMD Soft Function Through Large-Momentum Effective Theory </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Zhang%2C+Q">Qi-An Zhang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jun Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Huo%2C+Y">Yikai Huo</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ji%2C+X">Xiangdong Ji</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Liu%2C+Y">Yizhuang Liu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Liu%2C+Y">Yu-Sheng Liu</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Schlemmer%2C+M">Maximilian Schlemmer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sch%C3%A4fer%2C+A">Andreas Sch盲fer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sun%2C+P">Peng Sun</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wang%2C+W">Wei Wang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Yang%2C+Y">Yi-Bo Yang</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="2005.14572v2-abstract-short" style="display: inline;"> The transverse-momentum-dependent (TMD) soft function is a key ingredient in QCD factorization of Drell-Yan and other processes with relatively small transverse momentum. We present a lattice QCD study of this function at moderately large rapidity on a 2+1 flavor CLS dynamic ensemble with $a=0.098$ fm. We extract the rapidity-independent (or intrinsic) part of the soft function through a large-mom&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14572v2-abstract-full').style.display = 'inline'; document.getElementById('2005.14572v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2005.14572v2-abstract-full" style="display: none;"> The transverse-momentum-dependent (TMD) soft function is a key ingredient in QCD factorization of Drell-Yan and other processes with relatively small transverse momentum. We present a lattice QCD study of this function at moderately large rapidity on a 2+1 flavor CLS dynamic ensemble with $a=0.098$ fm. We extract the rapidity-independent (or intrinsic) part of the soft function through a large-momentum-transfer pseudo-scalar meson form factor and its quasi-TMD wave function using leading-order factorization in large-momentum effective theory. We also investigate the rapidity-dependent part of the soft function---the Collins-Soper evolution kernel---based on the large-momentum evolution of the quasi-TMD wave function. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14572v2-abstract-full').style.display = 'none'; document.getElementById('2005.14572v2-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 October, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 29 May, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2020. </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">6 +4 pages, 5 + 7 figures; v2: 7 + 6 pages, 5 + 9 figures, accepted for publication by Physical Review Letters</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 125, 192001 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1705.06186">arXiv:1705.06186</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1705.06186">pdf</a>, <a href="https://arxiv.org/format/1705.06186">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 - 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 Theory">nucl-th</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/10.1142/S0217751X1950009X">10.1142/S0217751X1950009X <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Iso-vector axial form factors of the nucleon in two-flavour lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Capitani%2C+S">Stefano Capitani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Della+Morte%2C+M">Michele Della Morte</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Djukanovic%2C+D">Dalibor Djukanovic</a>, <a href="/search/hep-lat?searchtype=author&amp;query=von+Hippel%2C+G+M">Georg M. von Hippel</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">Jiayu Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=J%C3%A4ger%2C+B">Benjamin J盲ger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Junnarkar%2C+P+M">Parikshit M. Junnarkar</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Meyer%2C+H+B">Harvey B. Meyer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Rae%2C+T+D">Thomas D. Rae</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wittig%2C+H">Hartmut Wittig</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="1705.06186v4-abstract-short" style="display: inline;"> We present a lattice calculation of the nucleon iso-vector axial and induced pseudoscalar form factors on the CLS ensembles using $N_{\rm f}=2$ dynamical flavours of non-perturbatively $\mathcal{O}(a)$-improved Wilson fermions and an $\mathcal{O}(a)$-improved axial current together with the pseudoscalar density. Excited-state effects in the extraction of the form factors are treated using a variet&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1705.06186v4-abstract-full').style.display = 'inline'; document.getElementById('1705.06186v4-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1705.06186v4-abstract-full" style="display: none;"> We present a lattice calculation of the nucleon iso-vector axial and induced pseudoscalar form factors on the CLS ensembles using $N_{\rm f}=2$ dynamical flavours of non-perturbatively $\mathcal{O}(a)$-improved Wilson fermions and an $\mathcal{O}(a)$-improved axial current together with the pseudoscalar density. Excited-state effects in the extraction of the form factors are treated using a variety of methods, with a detailed discussion of their respective merits. The chiral and continuum extrapolation of the results is performed both using formulae inspired by Heavy Baryon Chiral Perturbation Theory (HBChPT) and a global approach to the form factors based on a chiral effective theory (EFT) including axial vector mesons. Our results indicate that careful treatment of excited-state effects is important in order to obtain reliable results for the axial form factors of the nucleon, and that the main remaining error stems from the systematic uncertainties of the chiral extrapolation. As final results, we quote $g_{\rm A} = 1.278 \pm 0.068\genfrac{}{}{0pt}{1}{+0.000}{-0.087}$, $\langle r_{\rm A}^2\rangle = 0.360 \pm 0.036\genfrac{}{}{0pt}{1}{+0.080}{-0.088}~\mathrm{fm}^2$, and $g_{\rm P} = 7.7 \pm 1.8 \genfrac{}{}{0pt}{1}{+0.8}{-2.0}$ for the axial charge, axial charge radius and induced pseudoscalar charge, respectively, where the first error is statistical and the second is systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1705.06186v4-abstract-full').style.display = 'none'; document.getElementById('1705.06186v4-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 January, 2019; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 17 May, 2017; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2017. </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">27 pages, 13 figures (23 PDF files); uses revtex4-1.cls; v4: corrections to affiliation addresses, matches published version</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> CP3-Origins-2017-018, HIM-2017-03, MITP/17-029, TIFR/TH/17-21 </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Int.J.Mod.Phys. A 34 (2019) 1950009 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1504.04628">arXiv:1504.04628</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1504.04628">pdf</a>, <a href="https://arxiv.org/format/1504.04628">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 - 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 Theory">nucl-th</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/10.1103/PhysRevD.92.054511">10.1103/PhysRevD.92.054511 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Nucleon electromagnetic form factors in two-flavour QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Capitani%2C+S">S. Capitani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Della+Morte%2C+M">M. Della Morte</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Djukanovic%2C+D">D. Djukanovic</a>, <a href="/search/hep-lat?searchtype=author&amp;query=von+Hippel%2C+G">G. von Hippel</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">J. Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=J%C3%A4ger%2C+B">B. J盲ger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Knippschild%2C+B">B. Knippschild</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Meyer%2C+H+B">H. B. Meyer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Rae%2C+T+D">T. D. Rae</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wittig%2C+H">H. Wittig</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="1504.04628v2-abstract-short" style="display: inline;"> We present results for the nucleon electromagnetic form factors, including the momentum transfer dependence and derived quantities (charge radii and magnetic moment). The analysis is performed using O(a) improved Wilson fermions in Nf=2 QCD measured on the CLS ensembles. Particular focus is placed on a systematic evaluation of the influence of excited states in three-point correlation functions, w&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1504.04628v2-abstract-full').style.display = 'inline'; document.getElementById('1504.04628v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1504.04628v2-abstract-full" style="display: none;"> We present results for the nucleon electromagnetic form factors, including the momentum transfer dependence and derived quantities (charge radii and magnetic moment). The analysis is performed using O(a) improved Wilson fermions in Nf=2 QCD measured on the CLS ensembles. Particular focus is placed on a systematic evaluation of the influence of excited states in three-point correlation functions, which lead to a biased evaluation, if not accounted for correctly. We argue that the use of summed operator insertions and fit ans盲tze including excited states allow us to suppress and control this effect. We employ a novel method to perform joint chiral and continuum extrapolations, by fitting the form factors directly to the expressions of covariant baryonic chiral effective field theory. The final results for the charge radii and magnetic moment from our lattice calculations include, for the first time, a full error budget. We find that our estimates are compatible with experimental results within their overall uncertainties. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1504.04628v2-abstract-full').style.display = 'none'; document.getElementById('1504.04628v2-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 April, 2015; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 17 April, 2015; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2015. </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">22 pages, 10 figures, citations modified</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> MITP/15-026, HIM-2015-01, CP3-Origins-2015-012, DIAS-2015-12 </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 92, 054511 (2015) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1411.5828">arXiv:1411.5828</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1411.5828">pdf</a>, <a href="https://arxiv.org/format/1411.5828">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 - Lattice">hep-lat</span> </div> </div> <p class="title is-5 mathjax"> Nucleon axial form factors from two-flavour Lattice QCD </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Junnarkar%2C+P+M">P. M. Junnarkar</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Capitani%2C+S">S. Capitani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Djukanovic%2C+D">D. Djukanovic</a>, <a href="/search/hep-lat?searchtype=author&amp;query=von+Hippel%2C+G">G. von Hippel</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">J. Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=J%C3%A4ger%2C+B">B. J盲ger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Meyer%2C+H+B">H. B. Meyer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Rae%2C+T+D">T. D. Rae</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wittig%2C+H">H. Wittig</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="1411.5828v1-abstract-short" style="display: inline;"> We present preliminary results on the axial form factor $G_A(Q^2)$ and the induced pseudoscalar form factor $G_P(Q^2)$ of the nucleon. A systematic analysis of the excited-state contributions to form factors is performed on the CLS ensemble `N6&#39; with $m_蟺= 340 \ \text{MeV}$ and lattice spacing $a \sim 0.05 \ \text{fm}$. The relevant three-point functions were computed with source-sink separations&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1411.5828v1-abstract-full').style.display = 'inline'; document.getElementById('1411.5828v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1411.5828v1-abstract-full" style="display: none;"> We present preliminary results on the axial form factor $G_A(Q^2)$ and the induced pseudoscalar form factor $G_P(Q^2)$ of the nucleon. A systematic analysis of the excited-state contributions to form factors is performed on the CLS ensemble `N6&#39; with $m_蟺= 340 \ \text{MeV}$ and lattice spacing $a \sim 0.05 \ \text{fm}$. The relevant three-point functions were computed with source-sink separations ranging from $t_s \sim 0.6 \ \text{fm}$ to $t_s \sim \ 1.4 \ \text{fm}$. We observe that the form factors suffer from non-trivial excited-state contributions at the source-sink separations available to us. It is noted that naive plateau fits underestimate the excited-state contributions and that the method of summed operator insertions correctly accounts for these effects. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1411.5828v1-abstract-full').style.display = 'none'; document.getElementById('1411.5828v1-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, 2014; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2014. </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">7 pages, 12 figures; talk presented at Lattice 2014 -- 32nd International Symposium on Lattice Field Theory, 23-28 June, 2014, Columbia University New York, NY</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> PoS(LATTICE2014)150 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1411.4804">arXiv:1411.4804</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1411.4804">pdf</a>, <a href="https://arxiv.org/format/1411.4804">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 - Lattice">hep-lat</span> </div> </div> <p class="title is-5 mathjax"> Suppression of excited-state effects in lattice determination of nucleon electromagnetic form factors </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=von+Hippel%2C+G+M">G. M. von Hippel</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Capitani%2C+S">S. Capitani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Djukanovic%2C+D">D. Djukanovic</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hua%2C+J">J. Hua</a>, <a href="/search/hep-lat?searchtype=author&amp;query=J%C3%A4ger%2C+B">B. J盲ger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Junnarkar%2C+P">P. Junnarkar</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Meyer%2C+H+B">H. B. Meyer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Rae%2C+T+D">T. D. Rae</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Wittig%2C+H">H. Wittig</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="1411.4804v1-abstract-short" style="display: inline;"> We study the ability of a variety of fitting techniques to extract the ground state matrix elements of the vector current from ratios of nucleon three- and two-point functions that contain contaminations from excited states. Extending our high-statistics study of nucleon form factors, we are able to demonstrate that the treatment of excited-state contributions in conjunction with approaching the p&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1411.4804v1-abstract-full').style.display = 'inline'; document.getElementById('1411.4804v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1411.4804v1-abstract-full" style="display: none;"> We study the ability of a variety of fitting techniques to extract the ground state matrix elements of the vector current from ratios of nucleon three- and two-point functions that contain contaminations from excited states. Extending our high-statistics study of nucleon form factors, we are able to demonstrate that the treatment of excited-state contributions in conjunction with approaching the physical pion mass has a significant impact on the $Q^2$-dependence of the form factors. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1411.4804v1-abstract-full').style.display = 'none'; document.getElementById('1411.4804v1-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, 2014; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2014. </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">7 pages, 5 pdf figures; talk presented at Lattice 2014 -- 32nd International Symposium on Lattice Field Theory, 23-28 June, 2014, Columbia University New York, NY</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> PoS(LATTICE2014)147 </p> </li> </ol> <div class="is-hidden-tablet"> <!-- feedback for mobile only --> <span class="help" style="display: inline-block;"><a href="https://github.com/arXiv/arxiv-search/releases">Search v0.5.6 released 2020-02-24</a>&nbsp;&nbsp;</span> </div> </div> </main> <footer> <div class="columns is-desktop" role="navigation" aria-label="Secondary"> <!-- MetaColumn 1 --> <div class="column"> <div class="columns"> <div class="column"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/about">About</a></li> <li><a href="https://info.arxiv.org/help">Help</a></li> </ul> </div> <div class="column"> <ul class="nav-spaced"> <li> <svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 512 512" class="icon filter-black" role="presentation"><title>contact arXiv</title><desc>Click here to contact 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