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value="license">License (URI)</option><option value="author_id">arXiv author ID</option><option value="help">Help pages</option><option value="full_text">Full text</option></select> <input id="query" name="query" type="text" value="Ahmad, S"> <ul id="abstracts"><li><input checked id="abstracts-0" name="abstracts" type="radio" value="show"> <label for="abstracts-0">Show abstracts</label></li><li><input id="abstracts-1" name="abstracts" type="radio" value="hide"> <label for="abstracts-1">Hide abstracts</label></li></ul> </div> <div class="box field is-grouped is-grouped-multiline level-item"> <div class="control"> <span class="select is-small"> <select id="size" name="size"><option value="25">25</option><option selected value="50">50</option><option value="100">100</option><option value="200">200</option></select> </span> <label for="size">results per page</label>. </div> <div class="control"> <label for="order">Sort results by</label> <span class="select is-small"> <select id="order" 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/2501.19197">arXiv:2501.19197</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.19197">pdf</a>, <a href="https://arxiv.org/ps/2501.19197">ps</a>, <a href="https://arxiv.org/format/2501.19197">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computational Physics">physics.comp-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Statistical Mechanics">cond-mat.stat-mech</span> </div> </div> <p class="title is-5 mathjax"> Aging Dynamics and Velocity Field Correlations in Three-Dimensional Uniformly Heated Granular Gases: A Molecular Dynamics Study </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Shah%2C+R+F">Rameez Farooq Shah</a>, <a href="/search/physics?searchtype=author&amp;query=Kumari%2C+S">Shikha Kumari</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S+R">Syed Rashid Ahmad</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="2501.19197v1-abstract-short" style="display: inline;"> We conduct a molecular dynamics simulation of an inelastic gas system utilizing an event-driven algorithm combined with a thermostat mechanism. Initially, the kinetic energy of the system experiences a decay before settling into a non-equilibrium steady state. To explore the aging characteristics, we analyze the velocity autocorrelation function, denoted as \( C(t_w, t) \). Our findings indicate t&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.19197v1-abstract-full').style.display = 'inline'; document.getElementById('2501.19197v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.19197v1-abstract-full" style="display: none;"> We conduct a molecular dynamics simulation of an inelastic gas system utilizing an event-driven algorithm combined with a thermostat mechanism. Initially, the kinetic energy of the system experiences a decay before settling into a non-equilibrium steady state. To explore the aging characteristics, we analyze the velocity autocorrelation function, denoted as \( C(t_w, t) \). Our findings indicate that \( C(t_w, t) \) exhibits a dependence on both waiting time \( t_w \) and correlation time \( t \) in an independent manner. At the outset, \( C(t_w, t) \) demonstrates an exponential decay pattern. With increasing \( t_w \), a slower decay is observed, which can be attributed to the development of correlations in the velocity field. The explicit relationship of \( C(t_w, t) \) with respect to \( t_w \) serves as compelling evidence of the aging properties present in the system. These results deepen our comprehension of non-equilibrium statistical mechanics and the dynamics of dissipative systems. Our research has significant implications for a range of applications involving inelastic collisions, extending from granular materials to phenomena observed in astrophysics. The simulation methodology and the insights gained contribute to the wider field of complex systems, shedding light on the behavior of systems that are far from equilibrium, particularly those characterized by energy dissipation due to inelastic interactions. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.19197v1-abstract-full').style.display = 'none'; document.getElementById('2501.19197v1-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> 31 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.18900">arXiv:2501.18900</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.18900">pdf</a>, <a href="https://arxiv.org/ps/2501.18900">ps</a>, <a href="https://arxiv.org/format/2501.18900">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Computational Physics">physics.comp-ph</span> </div> </div> <p class="title is-5 mathjax"> Velocity Distribution of a Uniformly Heated Hard Sphere Granular Gas </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Shah%2C+R+F">Rameez Farooq Shah</a>, <a href="/search/physics?searchtype=author&amp;query=Kumari%2C+S">Shikha Kumari</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S+R">Syed Rashid Ahmad</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="2501.18900v1-abstract-short" style="display: inline;"> This paper presents a molecular dynamics simulation of an inelastic gas, where collisions between molecules are characterized by a coefficient of restitution less than unity. The simulation employs an event-driven algorithm to efficiently propagate the system in time, tracking molecular positions and velocities. A thermostat mechanism is incorporated to maintain the system&#39;s temperature by applyin&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.18900v1-abstract-full').style.display = 'inline'; document.getElementById('2501.18900v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.18900v1-abstract-full" style="display: none;"> This paper presents a molecular dynamics simulation of an inelastic gas, where collisions between molecules are characterized by a coefficient of restitution less than unity. The simulation employs an event-driven algorithm to efficiently propagate the system in time, tracking molecular positions and velocities. A thermostat mechanism is incorporated to maintain the system&#39;s temperature by applying Gaussian white noise to the molecular velocities. The system&#39;s kinetic energy evolves towards a non-equilibrium steady state, with the initial dynamics governed by the interplay between energy input from the thermostat and energy dissipation through inelastic collisions. This steady state emerges when the energy gain from the thermostat balances the energy loss due to inelastic collisions. We calculate the coefficients of the Sonine polynomial expansion of the velocity distribution function to show that the velocity distribution exhibits a departure from the Maxwell-Boltzmann distribution in the steady state. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.18900v1-abstract-full').style.display = 'none'; document.getElementById('2501.18900v1-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> 31 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.03273">arXiv:2410.03273</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.03273">pdf</a>, <a href="https://arxiv.org/ps/2410.03273">ps</a>, <a href="https://arxiv.org/format/2410.03273">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Soft Condensed Matter">cond-mat.soft</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Pattern Formation and Solitons">nlin.PS</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Computational Physics">physics.comp-ph</span> </div> </div> <p class="title is-5 mathjax"> Probing 3D Velocity Distributions Insights from a Vibrated Dual-Species Granular System </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Shah%2C+R+F">Rameez Farooq Shah</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S+R">Syed Rashid Ahmad</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="2410.03273v1-abstract-short" style="display: inline;"> We explore the velocity distributions in a vibrated binary granular gas system, focusing on how these distributions are influenced by the coefficient of restitution (CoR) and the inelasticity of particle collisions. Through molecular dynamics simulations, we examine the system&#39;s behavior for a range of CoR values below unity: specifically, 0.80, 0.85, 0.90, and 0.95. We track the evolution of velo&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.03273v1-abstract-full').style.display = 'inline'; document.getElementById('2410.03273v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.03273v1-abstract-full" style="display: none;"> We explore the velocity distributions in a vibrated binary granular gas system, focusing on how these distributions are influenced by the coefficient of restitution (CoR) and the inelasticity of particle collisions. Through molecular dynamics simulations, we examine the system&#39;s behavior for a range of CoR values below unity: specifically, 0.80, 0.85, 0.90, and 0.95. We track the evolution of velocity distributions as the system approaches a non-equilibrium steady state. Our findings reveal a clear departure from the classical Maxwell-Boltzmann distribution, with increasing deviations as CoR decreases, indicating non-equipartition of energy between the two particle types. This behavior underscores the intricate dynamics inherent in inelastic collisions and highlights the significance of particle inelasticity in determining the system&#39;s velocity distributions. These results provide insight into non-equilibrium statistical mechanics and have implications for real-world applications where granular materials are subject to external vibrations. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.03273v1-abstract-full').style.display = 'none'; document.getElementById('2410.03273v1-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> 4 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/2405.17860">arXiv:2405.17860</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2405.17860">pdf</a>, <a href="https://arxiv.org/format/2405.17860">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="Instrumentation and Detectors">physics.ins-det</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/ad83aa">10.1088/1674-1137/ad83aa <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Prediction of Energy Resolution in the JUNO Experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=JUNO+Collaboration"> JUNO Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Adamowicz%2C+K">Kai Adamowicz</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmed%2C+R">Rizwan Ahmed</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Bai%2C+W">Weidong Bai</a>, <a href="/search/physics?searchtype=author&amp;query=Balashov%2C+N">Nikita Balashov</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Basilico%2C+D">Davide Basilico</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Beretta%2C+M">Marco Beretta</a>, <a href="/search/physics?searchtype=author&amp;query=Bergnoli%2C+A">Antonio Bergnoli</a>, <a href="/search/physics?searchtype=author&amp;query=Bick%2C+D">Daniel Bick</a> , et al. (629 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="2405.17860v2-abstract-short" style="display: inline;"> This paper presents an energy resolution study of the JUNO experiment, incorporating the latest knowledge acquired during the detector construction phase. The determination of neutrino mass ordering in JUNO requires an exceptional energy resolution better than 3\% at 1~MeV. To achieve this ambitious goal, significant efforts have been undertaken in the design and production of the key components o&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2405.17860v2-abstract-full').style.display = 'inline'; document.getElementById('2405.17860v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2405.17860v2-abstract-full" style="display: none;"> This paper presents an energy resolution study of the JUNO experiment, incorporating the latest knowledge acquired during the detector construction phase. The determination of neutrino mass ordering in JUNO requires an exceptional energy resolution better than 3\% at 1~MeV. To achieve this ambitious goal, significant efforts have been undertaken in the design and production of the key components of the JUNO detector. Various factors affecting the detection of inverse beta decay signals have an impact on the energy resolution, extending beyond the statistical fluctuations of the detected number of photons, such as the properties of the liquid scintillator, performance of photomultiplier tubes, and the energy reconstruction algorithm. To account for these effects, a full JUNO simulation and reconstruction approach is employed. This enables the modeling of all relevant effects and the evaluation of associated inputs to accurately estimate the energy resolution. The results of study reveal an energy resolution of 2.95\% at 1~MeV. Furthermore, this study assesses the contribution of major effects to the overall energy resolution budget. This analysis serves as a reference for interpreting future measurements of energy resolution during JUNO data collection. Moreover, it provides a guideline for comprehending the energy resolution characteristics of liquid scintillator-based detectors. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2405.17860v2-abstract-full').style.display = 'none'; document.getElementById('2405.17860v2-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 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 28 May, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Chinese Phys. C 49 013003 (2025) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2306.04616">arXiv:2306.04616</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2306.04616">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 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/10.1088/2053-1583/acfa0f">10.1088/2053-1583/acfa0f <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Dielectric breakdown and sub-wavelength patterning of monolayer hexagonal boron nitride using femtosecond pulses </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S+I">Sabeeh Irfan Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Sarpong%2C+E">Emmanuel Sarpong</a>, <a href="/search/physics?searchtype=author&amp;query=Dave%2C+A">Arpit Dave</a>, <a href="/search/physics?searchtype=author&amp;query=Yao%2C+H">Hsin-Yu Yao</a>, <a href="/search/physics?searchtype=author&amp;query=Solomon%2C+J+M">Joel M. Solomon</a>, <a href="/search/physics?searchtype=author&amp;query=Jiang%2C+J">Jing-Kai Jiang</a>, <a href="/search/physics?searchtype=author&amp;query=Luo%2C+C">Chih-Wei Luo</a>, <a href="/search/physics?searchtype=author&amp;query=Chang%2C+W">Wen-Hao Chang</a>, <a href="/search/physics?searchtype=author&amp;query=Her%2C+T">Tsing-Hua Her</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="2306.04616v1-abstract-short" style="display: inline;"> Hexagonal boron nitride (hBN) has emerged as a promising two-dimensional (2D) material for many applications in photonics. Although its linear and nonlinear optical properties have been extensively studied, its interaction with high-intensity laser pulses, which is important for high-harmonic generation, fabricating quantum emitters, and maskless patterning of hBN, has not been investigated. Here&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2306.04616v1-abstract-full').style.display = 'inline'; document.getElementById('2306.04616v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2306.04616v1-abstract-full" style="display: none;"> Hexagonal boron nitride (hBN) has emerged as a promising two-dimensional (2D) material for many applications in photonics. Although its linear and nonlinear optical properties have been extensively studied, its interaction with high-intensity laser pulses, which is important for high-harmonic generation, fabricating quantum emitters, and maskless patterning of hBN, has not been investigated. Here we report the first study of dielectric breakdown in hBN monolayers induced by single femtosecond laser pulses. We show that hBN has the highest breakdown threshold among all existing 2D materials. This enables us to observe clearly for the first time a linear dependence of breakdown threshold on the bandgap energy for 2D materials, demonstrating such a linear dependency is a universal scaling law independent of the dimensionality. We also observe counter-intuitively that hBN, which has a larger bandgap and mechanical strength than quartz, has a lower breakdown threshold. This implies carrier generation in hBN is much more efficient. Furthermore, we demonstrate the clean removal of hBN without damage to the surrounding hBN film or the substrate, indicating that hBN is optically very robust. The ablated features are shown to possess very small edge roughness, which is attributed to its ultrahigh fracture toughness. Finally, we demonstrate femtosecond laser patterning of hBN with sub-wavelength resolution, including an isolated stripe width of 200 nm. Our work advances the knowledge of light-hBN interaction in the strong field regime and firmly establishes femtosecond lasers as novel and promising tools for one-step deterministic patterning of hBN monolayers. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2306.04616v1-abstract-full').style.display = 'none'; document.getElementById('2306.04616v1-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 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">21 pages in total. 16 pages in the main text, the rest are supplementary. 6 figures in the main text, 5 figures in the supplementary data</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> https://iopscience.iop.org/article/10.1088/2053-1583/acfa0f </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2305.14855">arXiv:2305.14855</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2305.14855">pdf</a>, <a href="https://arxiv.org/format/2305.14855">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> Study experimental time resolution limits of recent ASICs at Weeroc with different SiPMs and scintillators </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Saleem%2C+T">Tasneem Saleem</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Salleh Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Cizel%2C+J">Jean-Baptiste Cizel</a>, <a href="/search/physics?searchtype=author&amp;query=De+La+Taille%2C+C">Christophe De La Taille</a>, <a href="/search/physics?searchtype=author&amp;query=Morenas%2C+M">Maxime Morenas</a>, <a href="/search/physics?searchtype=author&amp;query=Nadig%2C+V">Vanessa Nadig</a>, <a href="/search/physics?searchtype=author&amp;query=Perez%2C+F">Florent Perez</a>, <a href="/search/physics?searchtype=author&amp;query=Schulz%2C+V">Volkmar Schulz</a>, <a href="/search/physics?searchtype=author&amp;query=Gundacker%2C+S">Stefan Gundacker</a>, <a href="/search/physics?searchtype=author&amp;query=Fleury%2C+J">Julien Fleury</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="2305.14855v3-abstract-short" style="display: inline;"> Medical applications, such as Positron Emission Tomography (PET), and space applications, such as Light Detection and Ranging (LIDAR), are in need of highly specialized ASICs. Weeroc, in collaboration with different partners, is highly involved in developing a new generation of front-end ASICs. In the context of a joined LIDAR project among Weeroc, CNES, and Airbus, Weeroc is working on the develo&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2305.14855v3-abstract-full').style.display = 'inline'; document.getElementById('2305.14855v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2305.14855v3-abstract-full" style="display: none;"> Medical applications, such as Positron Emission Tomography (PET), and space applications, such as Light Detection and Ranging (LIDAR), are in need of highly specialized ASICs. Weeroc, in collaboration with different partners, is highly involved in developing a new generation of front-end ASICs. In the context of a joined LIDAR project among Weeroc, CNES, and Airbus, Weeroc is working on the development of Liroc, an ASIC for space LIDAR application. Weeroc is also working on advancing ASICs for medical applications with Radioroc under development and intended to be used for PET applications. This study experimentally evaluates the time resolution limits of these ASICs in different configurations, with some of the most recent silicon photomultiplier (SiPM) technologies available on the market, coupled to different scintillation crystals. The best single-photon time resolution (SPTR) was achieved using FBK NUV-HD SiPMs with an FWHM of 90 ps with Liroc and 73 ps with Radioroc. Furthermore, the coincidence time resolution (CTR) of Radioroc was studied with different crystal sizes. Using a large LYSO:Ce,Ca crystal of (3 x 3 x 20 mm3) with Broadcom Near UltraViolet-Metal in Trench (NUV-MT) yields a CTR of 127 ps (FWHM). The best CTR of Radioroc was determined to 83 ps (FWHM) with Broadcom NUV-MT SiPMs coupled to LYSO:Ce,Ca (2 x 2 x 3 mm3) from Taiwan Applied Crystal (TAC). <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2305.14855v3-abstract-full').style.display = 'none'; document.getElementById('2305.14855v3-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 October, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 24 May, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">Prepared for submission to JINST</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2303.05172">arXiv:2303.05172</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2303.05172">pdf</a>, <a href="https://arxiv.org/format/2303.05172">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="Instrumentation and Detectors">physics.ins-det</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/10.1016/j.nima.2023.168680">10.1016/j.nima.2023.168680 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> The JUNO experiment Top Tracker </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=JUNO+Collaboration"> JUNO Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmed%2C+R">Rizwan Ahmed</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=Aleem%2C+A">Abid Aleem</a>, <a href="/search/physics?searchtype=author&amp;query=Alexandros%2C+T">Tsagkarakis Alexandros</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Bai%2C+W">Weidong Bai</a>, <a href="/search/physics?searchtype=author&amp;query=Balashov%2C+N">Nikita Balashov</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Basilico%2C+D">Davide Basilico</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a> , et al. (592 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="2303.05172v1-abstract-short" style="display: inline;"> The main task of the Top Tracker detector of the neutrino reactor experiment Jiangmen Underground Neutrino Observatory (JUNO) is to reconstruct and extrapolate atmospheric muon tracks down to the central detector. This muon tracker will help to evaluate the contribution of the cosmogenic background to the signal. The Top Tracker is located above JUNO&#39;s water Cherenkov Detector and Central Detector&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.05172v1-abstract-full').style.display = 'inline'; document.getElementById('2303.05172v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2303.05172v1-abstract-full" style="display: none;"> The main task of the Top Tracker detector of the neutrino reactor experiment Jiangmen Underground Neutrino Observatory (JUNO) is to reconstruct and extrapolate atmospheric muon tracks down to the central detector. This muon tracker will help to evaluate the contribution of the cosmogenic background to the signal. The Top Tracker is located above JUNO&#39;s water Cherenkov Detector and Central Detector, covering about 60% of the surface above them. The JUNO Top Tracker is constituted by the decommissioned OPERA experiment Target Tracker modules. The technology used consists in walls of two planes of plastic scintillator strips, one per transverse direction. Wavelength shifting fibres collect the light signal emitted by the scintillator strips and guide it to both ends where it is read by multianode photomultiplier tubes. Compared to the OPERA Target Tracker, the JUNO Top Tracker uses new electronics able to cope with the high rate produced by the high rock radioactivity compared to the one in Gran Sasso underground laboratory. This paper will present the new electronics and mechanical structure developed for the Top Tracker of JUNO along with its expected performance based on the current detector simulation. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.05172v1-abstract-full').style.display = 'none'; document.getElementById('2303.05172v1-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 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 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">20 pages</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nucl.Instrum.Meth.A 1057 (2023) 168680 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2303.03910">arXiv:2303.03910</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2303.03910">pdf</a>, <a href="https://arxiv.org/format/2303.03910">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="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> JUNO sensitivity to $^7$Be, $pep$, and CNO solar neutrinos </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmed%2C+R">Rizwan Ahmed</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=Aleem%2C+A">Abid Aleem</a>, <a href="/search/physics?searchtype=author&amp;query=Alexandros%2C+T">Tsagkarakis Alexandros</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Bai%2C+W">Weidong Bai</a>, <a href="/search/physics?searchtype=author&amp;query=Balashov%2C+N">Nikita Balashov</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Basilico%2C+D">Davide Basilico</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Beretta%2C+M">Marco Beretta</a> , et al. (592 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="2303.03910v1-abstract-short" style="display: inline;"> The Jiangmen Underground Neutrino Observatory (JUNO), the first multi-kton liquid scintillator detector, which is under construction in China, will have a unique potential to perform a real-time measurement of solar neutrinos well below the few MeV threshold typical for Water Cherenkov detectors. JUNO&#39;s large target mass and excellent energy resolution are prerequisites for reaching unprecedented&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.03910v1-abstract-full').style.display = 'inline'; document.getElementById('2303.03910v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2303.03910v1-abstract-full" style="display: none;"> The Jiangmen Underground Neutrino Observatory (JUNO), the first multi-kton liquid scintillator detector, which is under construction in China, will have a unique potential to perform a real-time measurement of solar neutrinos well below the few MeV threshold typical for Water Cherenkov detectors. JUNO&#39;s large target mass and excellent energy resolution are prerequisites for reaching unprecedented levels of precision. In this paper, we provide estimation of the JUNO sensitivity to 7Be, pep, and CNO solar neutrinos that can be obtained via a spectral analysis above the 0.45 MeV threshold. This study is performed assuming different scenarios of the liquid scintillator radiopurity, ranging from the most opti mistic one corresponding to the radiopurity levels obtained by the Borexino experiment, up to the minimum requirements needed to perform the neutrino mass ordering determination with reactor antineutrinos - the main goal of JUNO. Our study shows that in most scenarios, JUNO will be able to improve the current best measurements on 7Be, pep, and CNO solar neutrino fluxes. We also perform a study on the JUNO capability to detect periodical time variations in the solar neutrino flux, such as the day-night modulation induced by neutrino flavor regeneration in Earth, and the modulations induced by temperature changes driven by helioseismic waves. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.03910v1-abstract-full').style.display = 'none'; document.getElementById('2303.03910v1-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 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2023. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2205.08830">arXiv:2205.08830</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2205.08830">pdf</a>, <a href="https://arxiv.org/format/2205.08830">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 Astrophysical Phenomena">astro-ph.HE</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="Instrumentation and Detectors">physics.ins-det</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/10.1088/1475-7516/2022/10/033">10.1088/1475-7516/2022/10/033 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Prospects for Detecting the Diffuse Supernova Neutrino Background with JUNO </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=JUNO+Collaboration"> JUNO Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmed%2C+R">Rizwan Ahmed</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Balashov%2C+N">Nikita Balashov</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Basilico%2C+D">Davide Basilico</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Bergnoli%2C+A">Antonio Bergnoli</a>, <a href="/search/physics?searchtype=author&amp;query=Birkenfeld%2C+T">Thilo Birkenfeld</a>, <a href="/search/physics?searchtype=author&amp;query=Blin%2C+S">Sylvie Blin</a> , et al. (577 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="2205.08830v2-abstract-short" style="display: inline;"> We present the detection potential for the diffuse supernova neutrino background (DSNB) at the Jiangmen Underground Neutrino Observatory (JUNO), using the inverse-beta-decay (IBD) detection channel on free protons. We employ the latest information on the DSNB flux predictions, and investigate in detail the background and its reduction for the DSNB search at JUNO. The atmospheric neutrino induced n&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2205.08830v2-abstract-full').style.display = 'inline'; document.getElementById('2205.08830v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2205.08830v2-abstract-full" style="display: none;"> We present the detection potential for the diffuse supernova neutrino background (DSNB) at the Jiangmen Underground Neutrino Observatory (JUNO), using the inverse-beta-decay (IBD) detection channel on free protons. We employ the latest information on the DSNB flux predictions, and investigate in detail the background and its reduction for the DSNB search at JUNO. The atmospheric neutrino induced neutral current (NC) background turns out to be the most critical background, whose uncertainty is carefully evaluated from both the spread of model predictions and an envisaged \textit{in situ} measurement. We also make a careful study on the background suppression with the pulse shape discrimination (PSD) and triple coincidence (TC) cuts. With latest DSNB signal predictions, more realistic background evaluation and PSD efficiency optimization, and additional TC cut, JUNO can reach the significance of 3$蟽$ for 3 years of data taking, and achieve better than 5$蟽$ after 10 years for a reference DSNB model. In the pessimistic scenario of non-observation, JUNO would strongly improve the limits and exclude a significant region of the model parameter space. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2205.08830v2-abstract-full').style.display = 'none'; document.getElementById('2205.08830v2-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 October, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 18 May, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">29 pages, 11 figures, final published version in JCAP</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JCAP 10 (2022) 033 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2205.08629">arXiv:2205.08629</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2205.08629">pdf</a>, <a href="https://arxiv.org/format/2205.08629">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</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/10.1140/epjc/s10052-022-11002-8">10.1140/epjc/s10052-022-11002-8 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Mass Testing and Characterization of 20-inch PMTs for JUNO </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmed%2C+R">Rizwan Ahmed</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=Aleem%2C+A">Abid Aleem</a>, <a href="/search/physics?searchtype=author&amp;query=Alexandros%2C+T">Tsagkarakis Alexandros</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andre%2C+J+P+A+M">Joao Pedro Athayde Marcondes de Andre</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Bai%2C+W">Weidong Bai</a>, <a href="/search/physics?searchtype=author&amp;query=Balashov%2C+N">Nikita Balashov</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Basilico%2C+D">Davide Basilico</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Bergnoli%2C+A">Antonio Bergnoli</a> , et al. (541 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="2205.08629v2-abstract-short" style="display: inline;"> Main goal of the JUNO experiment is to determine the neutrino mass ordering using a 20kt liquid-scintillator detector. Its key feature is an excellent energy resolution of at least 3 % at 1 MeV, for which its instruments need to meet a certain quality and thus have to be fully characterized. More than 20,000 20-inch PMTs have been received and assessed by JUNO after a detailed testing program whic&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2205.08629v2-abstract-full').style.display = 'inline'; document.getElementById('2205.08629v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2205.08629v2-abstract-full" style="display: none;"> Main goal of the JUNO experiment is to determine the neutrino mass ordering using a 20kt liquid-scintillator detector. Its key feature is an excellent energy resolution of at least 3 % at 1 MeV, for which its instruments need to meet a certain quality and thus have to be fully characterized. More than 20,000 20-inch PMTs have been received and assessed by JUNO after a detailed testing program which began in 2017 and elapsed for about four years. Based on this mass characterization and a set of specific requirements, a good quality of all accepted PMTs could be ascertained. This paper presents the performed testing procedure with the designed testing systems as well as the statistical characteristics of all 20-inch PMTs intended to be used in the JUNO experiment, covering more than fifteen performance parameters including the photocathode uniformity. This constitutes the largest sample of 20-inch PMTs ever produced and studied in detail to date, i.e. 15,000 of the newly developed 20-inch MCP-PMTs from Northern Night Vision Technology Co. (NNVT) and 5,000 of dynode PMTs from Hamamatsu Photonics K. K.(HPK). <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2205.08629v2-abstract-full').style.display = 'none'; document.getElementById('2205.08629v2-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 September, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 17 May, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2022. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.07323">arXiv:2203.07323</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.07323">pdf</a>, <a href="https://arxiv.org/format/2203.07323">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="Cosmology and Nongalactic Astrophysics">astro-ph.CO</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="Instrumentation and Detectors">physics.ins-det</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/10.1088/1361-6471/ad307f">10.1088/1361-6471/ad307f <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> White Paper on Light Sterile Neutrino Searches and Related Phenomenology </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Acero%2C+M+A">M. A. Acero</a>, <a href="/search/physics?searchtype=author&amp;query=Arg%C3%BCelles%2C+C+A">C. A. Arg眉elles</a>, <a href="/search/physics?searchtype=author&amp;query=Hostert%2C+M">M. Hostert</a>, <a href="/search/physics?searchtype=author&amp;query=Kalra%2C+D">D. Kalra</a>, <a href="/search/physics?searchtype=author&amp;query=Karagiorgi%2C+G">G. Karagiorgi</a>, <a href="/search/physics?searchtype=author&amp;query=Kelly%2C+K+J">K. J. Kelly</a>, <a href="/search/physics?searchtype=author&amp;query=Littlejohn%2C+B">B. Littlejohn</a>, <a href="/search/physics?searchtype=author&amp;query=Machado%2C+P">P. Machado</a>, <a href="/search/physics?searchtype=author&amp;query=Pettus%2C+W">W. Pettus</a>, <a href="/search/physics?searchtype=author&amp;query=Toups%2C+M">M. Toups</a>, <a href="/search/physics?searchtype=author&amp;query=Ross-Lonergan%2C+M">M. Ross-Lonergan</a>, <a href="/search/physics?searchtype=author&amp;query=Sousa%2C+A">A. Sousa</a>, <a href="/search/physics?searchtype=author&amp;query=Surukuchi%2C+P+T">P. T. Surukuchi</a>, <a href="/search/physics?searchtype=author&amp;query=Wong%2C+Y+Y+Y">Y. Y. Y. Wong</a>, <a href="/search/physics?searchtype=author&amp;query=Abdallah%2C+W">W. Abdallah</a>, <a href="/search/physics?searchtype=author&amp;query=Abdullahi%2C+A+M">A. M. Abdullahi</a>, <a href="/search/physics?searchtype=author&amp;query=Akutsu%2C+R">R. Akutsu</a>, <a href="/search/physics?searchtype=author&amp;query=Alvarez-Ruso%2C+L">L. Alvarez-Ruso</a>, <a href="/search/physics?searchtype=author&amp;query=Alves%2C+D+S+M">D. S. M. Alves</a>, <a href="/search/physics?searchtype=author&amp;query=Aurisano%2C+A">A. Aurisano</a>, <a href="/search/physics?searchtype=author&amp;query=Balantekin%2C+A+B">A. B. Balantekin</a>, <a href="/search/physics?searchtype=author&amp;query=Berryman%2C+J+M">J. M. Berryman</a>, <a href="/search/physics?searchtype=author&amp;query=Bert%C3%B3lez-Mart%C3%ADnez%2C+T">T. Bert贸lez-Mart铆nez</a>, <a href="/search/physics?searchtype=author&amp;query=Brunner%2C+J">J. Brunner</a>, <a href="/search/physics?searchtype=author&amp;query=Blennow%2C+M">M. Blennow</a> , et al. (147 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="2203.07323v3-abstract-short" style="display: inline;"> This white paper provides a comprehensive review of our present understanding of experimental neutrino anomalies that remain unresolved, charting the progress achieved over the last decade at the experimental and phenomenological level, and sets the stage for future programmatic prospects in addressing those anomalies. It is purposed to serve as a guiding and motivational &#34;encyclopedic&#34; reference,&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.07323v3-abstract-full').style.display = 'inline'; document.getElementById('2203.07323v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.07323v3-abstract-full" style="display: none;"> This white paper provides a comprehensive review of our present understanding of experimental neutrino anomalies that remain unresolved, charting the progress achieved over the last decade at the experimental and phenomenological level, and sets the stage for future programmatic prospects in addressing those anomalies. It is purposed to serve as a guiding and motivational &#34;encyclopedic&#34; reference, with emphasis on needs and options for future exploration that may lead to the ultimate resolution of the anomalies. We see the main experimental, analysis, and theory-driven thrusts that will be essential to achieving this goal being: 1) Cover all anomaly sectors -- given the unresolved nature of all four canonical anomalies, it is imperative to support all pillars of a diverse experimental portfolio, source, reactor, decay-at-rest, decay-in-flight, and other methods/sources, to provide complementary probes of and increased precision for new physics explanations; 2) Pursue diverse signatures -- it is imperative that experiments make design and analysis choices that maximize sensitivity to as broad an array of these potential new physics signatures as possible; 3) Deepen theoretical engagement -- priority in the theory community should be placed on development of standard and beyond standard models relevant to all four short-baseline anomalies and the development of tools for efficient tests of these models with existing and future experimental datasets; 4) Openly share data -- Fluid communication between the experimental and theory communities will be required, which implies that both experimental data releases and theoretical calculations should be publicly available; and 5) Apply robust analysis techniques -- Appropriate statistical treatment is crucial to assess the compatibility of data sets within the context of any given model. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.07323v3-abstract-full').style.display = 'none'; document.getElementById('2203.07323v3-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 14 March, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 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">Contribution to Snowmass 2021 by the NF02 Topical Group (Understanding Experimental Neutrino Anomalies). Published in J. Phys. G as a Major Report</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> J. Phys. G: Nucl. Part. Phys. 51 120501 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2112.10743">arXiv:2112.10743</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2112.10743">pdf</a>, <a href="https://arxiv.org/format/2112.10743">other</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> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Applied Physics">physics.app-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/10.1063/5.0078054">10.1063/5.0078054 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Ultrafast Multi-Shot Ablation and Defect Generation in Monolayer Transition Metal Dichalcogenides </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Solomon%2C+J+M">Joel M. Solomon</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S+I">Sabeeh Irfan Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Dave%2C+A">Arpit Dave</a>, <a href="/search/physics?searchtype=author&amp;query=Lu%2C+L">Li-Syuan Lu</a>, <a href="/search/physics?searchtype=author&amp;query=Wu%2C+Y">Yu-Chen Wu</a>, <a href="/search/physics?searchtype=author&amp;query=Chang%2C+W">Wen-Hao Chang</a>, <a href="/search/physics?searchtype=author&amp;query=Luo%2C+C">Chih-Wei Luo</a>, <a href="/search/physics?searchtype=author&amp;query=Her%2C+T">Tsing-Hua Her</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="2112.10743v1-abstract-short" style="display: inline;"> Transition metal dichalcogenides are known to possess large optical nonlinearities and driving these materials at high intensities is desirable for many applications. Understanding their optical responses under repetitive intense excitation is essential to improve the performance limit of these strong-field devices and to achieve efficient laser patterning. Here, we report the incubation study of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.10743v1-abstract-full').style.display = 'inline'; document.getElementById('2112.10743v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2112.10743v1-abstract-full" style="display: none;"> Transition metal dichalcogenides are known to possess large optical nonlinearities and driving these materials at high intensities is desirable for many applications. Understanding their optical responses under repetitive intense excitation is essential to improve the performance limit of these strong-field devices and to achieve efficient laser patterning. Here, we report the incubation study of monolayer MoS${}_{2}$ and WS${}_{2}$ induced by 160 fs, 800 nm pulses in air to examine how their ablation threshold scales with the number of admitted laser pulses. Both materials were shown to outperform graphene and most bulk materials; specifically, MoS${}_{2}$ is as resistant to radiation degradation as the best of the bulk thin films with a record fast saturation. Our modeling provides convincing evidence that the small reduction in threshold and fast saturation of MoS${}_{2}$ originates in its excellent bonding integrity against radiation-induced softening. Sub-ablation damages, in the forms of vacancies, lattice disorder, and nano-voids, were revealed by transmission electron microscopy, photoluminescence, Raman, and second harmonic generation studies, which were attributed to the observed incubation. For the first time, a sub-ablation damage threshold is identified for monolayer MoS${}_{2}$ to be 78% of single-shot ablation threshold, below which MoS${}_{2}$ remains intact for many laser pulses. Our results firmly establish MoS${}_{2}$ as a robust material for strong-field devices and for high-throughput laser patterning. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.10743v1-abstract-full').style.display = 'none'; document.getElementById('2112.10743v1-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 December, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> AIP Advances 12, 015217 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2111.01352">arXiv:2111.01352</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2111.01352">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> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Applied Physics">physics.app-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/10.1038/s41598-022-10820-w">10.1038/s41598-022-10820-w <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Ultrafast Laser Ablation, Intrinsic Threshold, and Nanopatterning of Monolayer Molybdenum Disulfide </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Solomon%2C+J+M">Joel M. Solomon</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S+I">Sabeeh Irfan Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Dave%2C+A">Arpit Dave</a>, <a href="/search/physics?searchtype=author&amp;query=Lu%2C+L">Li-Syuan Lu</a>, <a href="/search/physics?searchtype=author&amp;query=HadavandMirzaee%2C+F">Fatemeh HadavandMirzaee</a>, <a href="/search/physics?searchtype=author&amp;query=Lin%2C+S">Shih-Chu Lin</a>, <a href="/search/physics?searchtype=author&amp;query=Chen%2C+S">Sih-Hua Chen</a>, <a href="/search/physics?searchtype=author&amp;query=Luo%2C+C">Chih-Wei Luo</a>, <a href="/search/physics?searchtype=author&amp;query=Chang%2C+W">Wen-Hao Chang</a>, <a href="/search/physics?searchtype=author&amp;query=Her%2C+T">Tsing-Hua Her</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="2111.01352v1-abstract-short" style="display: inline;"> Laser direct writing is an attractive method for patterning 2D materials without contamination. Literature shows that the femtosecond ablation threshold of graphene across substrates varies by an order of magnitude. Some attribute it to the thermal coupling to the substrates, but it remains by and large an open question. For the first time the effect of substrates on femtosecond ablation of 2D mat&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.01352v1-abstract-full').style.display = 'inline'; document.getElementById('2111.01352v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2111.01352v1-abstract-full" style="display: none;"> Laser direct writing is an attractive method for patterning 2D materials without contamination. Literature shows that the femtosecond ablation threshold of graphene across substrates varies by an order of magnitude. Some attribute it to the thermal coupling to the substrates, but it remains by and large an open question. For the first time the effect of substrates on femtosecond ablation of 2D materials is studied using MoS$_{2}$ as an example. We show unambiguously that femtosecond ablation of MoS$_{2}$ is an adiabatic process with negligible heat transfer to the substrates. The observed threshold variation is due to the etalon effect which was not identified before for the laser ablation of 2D materials. Subsequently, an intrinsic ablation threshold is proposed as a true threshold parameter for 2D materials. Additionally, we demonstrate for the first time femtosecond laser patterning of monolayer MoS$_{2}$ with sub-micron resolution and mm/s speed. Moreover, engineered substrates are shown to enhance the ablation efficiency, enabling patterning with low-power femtosecond oscillators. Finally, a zero-thickness approximation is introduced to predict the field enhancement with simple analytical expressions. Our work clarifies the role of substrates on ablation and firmly establishes femtosecond laser ablation as a viable route to pattern 2D materials. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.01352v1-abstract-full').style.display = 'none'; document.getElementById('2111.01352v1-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 November, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Scientific Reports 12, 6910 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2107.03669">arXiv:2107.03669</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2107.03669">pdf</a>, <a href="https://arxiv.org/format/2107.03669">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</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/JHEP11(2021)102">10.1007/JHEP11(2021)102 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Radioactivity control strategy for the JUNO detector </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=JUNO+collaboration"> JUNO collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmed%2C+R">Rizwan Ahmed</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Babic%2C+A">Andrej Babic</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Basilico%2C+D">Davide Basilico</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Bergnoli%2C+A">Antonio Bergnoli</a>, <a href="/search/physics?searchtype=author&amp;query=Birkenfeld%2C+T">Thilo Birkenfeld</a>, <a href="/search/physics?searchtype=author&amp;query=Blin%2C+S">Sylvie Blin</a> , et al. (578 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="2107.03669v2-abstract-short" style="display: inline;"> JUNO is a massive liquid scintillator detector with a primary scientific goal of determining the neutrino mass ordering by studying the oscillated anti-neutrino flux coming from two nuclear power plants at 53 km distance. The expected signal anti-neutrino interaction rate is only 60 counts per day, therefore a careful control of the background sources due to radioactivity is critical. In particula&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.03669v2-abstract-full').style.display = 'inline'; document.getElementById('2107.03669v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2107.03669v2-abstract-full" style="display: none;"> JUNO is a massive liquid scintillator detector with a primary scientific goal of determining the neutrino mass ordering by studying the oscillated anti-neutrino flux coming from two nuclear power plants at 53 km distance. The expected signal anti-neutrino interaction rate is only 60 counts per day, therefore a careful control of the background sources due to radioactivity is critical. In particular, natural radioactivity present in all materials and in the environment represents a serious issue that could impair the sensitivity of the experiment if appropriate countermeasures were not foreseen. In this paper we discuss the background reduction strategies undertaken by the JUNO collaboration to reduce at minimum the impact of natural radioactivity. We describe our efforts for an optimized experimental design, a careful material screening and accurate detector production handling, and a constant control of the expected results through a meticulous Monte Carlo simulation program. We show that all these actions should allow us to keep the background count rate safely below the target value of 10 Hz in the default fiducial volume, above an energy threshold of 0.7 MeV. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.03669v2-abstract-full').style.display = 'none'; document.getElementById('2107.03669v2-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 October, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 8 July, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 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">35 pages, 12 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/2103.16900">arXiv:2103.16900</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2103.16900">pdf</a>, <a href="https://arxiv.org/format/2103.16900">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> The Design and Sensitivity of JUNO&#39;s scintillator radiopurity pre-detector OSIRIS </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=JUNO+Collaboration"> JUNO Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmed%2C+R">Rizwan Ahmed</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+G">Guangpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Babic%2C+A">Andrej Babic</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Basilico%2C+D">Davide Basilico</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Bergnoli%2C+A">Antonio Bergnoli</a>, <a href="/search/physics?searchtype=author&amp;query=Birkenfeld%2C+T">Thilo Birkenfeld</a> , et al. (582 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="2103.16900v1-abstract-short" style="display: inline;"> The OSIRIS detector is a subsystem of the liquid scintillator fillling chain of the JUNO reactor neutrino experiment. Its purpose is to validate the radiopurity of the scintillator to assure that all components of the JUNO scintillator system work to specifications and only neutrino-grade scintillator is filled into the JUNO Central Detector. The aspired sensitivity level of $10^{-16}$ g/g of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2103.16900v1-abstract-full').style.display = 'inline'; document.getElementById('2103.16900v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2103.16900v1-abstract-full" style="display: none;"> The OSIRIS detector is a subsystem of the liquid scintillator fillling chain of the JUNO reactor neutrino experiment. Its purpose is to validate the radiopurity of the scintillator to assure that all components of the JUNO scintillator system work to specifications and only neutrino-grade scintillator is filled into the JUNO Central Detector. The aspired sensitivity level of $10^{-16}$ g/g of $^{238}$U and $^{232}$Th requires a large ($\sim$20 m$^3$) detection volume and ultralow background levels. The present paper reports on the design and major components of the OSIRIS detector, the detector simulation as well as the measuring strategies foreseen and the sensitivity levels to U/Th that can be reached in this setup. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2103.16900v1-abstract-full').style.display = 'none'; document.getElementById('2103.16900v1-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> 31 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">32 pages, 22 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/2011.06405">arXiv:2011.06405</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.06405">pdf</a>, <a href="https://arxiv.org/format/2011.06405">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</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/JHEP03(2021)004">10.1007/JHEP03(2021)004 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Calibration Strategy of the JUNO Experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=JUNO+collaboration"> JUNO collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmed%2C+R">Rizwan Ahmed</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+G">Guangpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Babic%2C+A">Andrej Babic</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Bergnoli%2C+A">Antonio Bergnoli</a>, <a href="/search/physics?searchtype=author&amp;query=Bernieri%2C+E">Enrico Bernieri</a>, <a href="/search/physics?searchtype=author&amp;query=Birkenfeld%2C+T">Thilo Birkenfeld</a> , et al. (571 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="2011.06405v3-abstract-short" style="display: inline;"> We present the calibration strategy for the 20 kton liquid scintillator central detector of the Jiangmen Underground Neutrino Observatory (JUNO). By utilizing a comprehensive multiple-source and multiple-positional calibration program, in combination with a novel dual calorimetry technique exploiting two independent photosensors and readout systems, we demonstrate that the JUNO central detector ca&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.06405v3-abstract-full').style.display = 'inline'; document.getElementById('2011.06405v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.06405v3-abstract-full" style="display: none;"> We present the calibration strategy for the 20 kton liquid scintillator central detector of the Jiangmen Underground Neutrino Observatory (JUNO). By utilizing a comprehensive multiple-source and multiple-positional calibration program, in combination with a novel dual calorimetry technique exploiting two independent photosensors and readout systems, we demonstrate that the JUNO central detector can achieve a better than 1% energy linearity and a 3% effective energy resolution, required by the neutrino mass ordering determination. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.06405v3-abstract-full').style.display = 'none'; document.getElementById('2011.06405v3-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 January, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 12 November, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2020. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2007.00314">arXiv:2007.00314</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2007.00314">pdf</a>, <a href="https://arxiv.org/format/2007.00314">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Optimization of the JUNO liquid scintillator composition using a Daya Bay antineutrino detector </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Bay%2C+D">Daya Bay</a>, <a href="/search/physics?searchtype=author&amp;query=collaborations%2C+J">JUNO collaborations</a>, <a href="/search/physics?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">A. Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">T. Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">S. Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">S. Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">M. Akram</a>, <a href="/search/physics?searchtype=author&amp;query=Ali%2C+N">N. Ali</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F+P">F. P. An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+G+P">G. P. An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">G. Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">N. Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">V. Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">T. Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">B. Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">J. P. A. M. de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Babic%2C+A">A. Babic</a>, <a href="/search/physics?searchtype=author&amp;query=Balantekin%2C+A+B">A. B. Balantekin</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">W. Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Baldoncini%2C+M">M. Baldoncini</a>, <a href="/search/physics?searchtype=author&amp;query=Band%2C+H+R">H. R. Band</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">A. Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">E. Baussan</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="2007.00314v1-abstract-short" style="display: inline;"> To maximize the light yield of the liquid scintillator (LS) for the Jiangmen Underground Neutrino Observatory (JUNO), a 20 t LS sample was produced in a pilot plant at Daya Bay. The optical properties of the new LS in various compositions were studied by replacing the gadolinium-loaded LS in one antineutrino detector. The concentrations of the fluor, PPO, and the wavelength shifter, bis-MSB, were&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2007.00314v1-abstract-full').style.display = 'inline'; document.getElementById('2007.00314v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2007.00314v1-abstract-full" style="display: none;"> To maximize the light yield of the liquid scintillator (LS) for the Jiangmen Underground Neutrino Observatory (JUNO), a 20 t LS sample was produced in a pilot plant at Daya Bay. The optical properties of the new LS in various compositions were studied by replacing the gadolinium-loaded LS in one antineutrino detector. The concentrations of the fluor, PPO, and the wavelength shifter, bis-MSB, were increased in 12 steps from 0.5 g/L and &lt;0.01 mg/L to 4 g/L and 13 mg/L, respectively. The numbers of total detected photoelectrons suggest that, with the optically purified solvent, the bis-MSB concentration does not need to be more than 4 mg/L. To bridge the one order of magnitude in the detector size difference between Daya Bay and JUNO, the Daya Bay data were used to tune the parameters of a newly developed optical model. Then, the model and tuned parameters were used in the JUNO simulation. This enabled to determine the optimal composition for the JUNO LS: purified solvent LAB with 2.5 g/L PPO, and 1 to 4 mg/L bis-MSB. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2007.00314v1-abstract-full').style.display = 'none'; document.getElementById('2007.00314v1-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 July, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 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">13 pages, 8 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/2006.11760">arXiv:2006.11760</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2006.11760">pdf</a>, <a href="https://arxiv.org/format/2006.11760">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> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> Feasibility and physics potential of detecting $^8$B solar neutrinos at JUNO </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=JUNO+collaboration"> JUNO collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=Ali%2C+N">Nawab Ali</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+G">Guangpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Babic%2C+A">Andrej Babic</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Bergnoli%2C+A">Antonio Bergnoli</a>, <a href="/search/physics?searchtype=author&amp;query=Bernieri%2C+E">Enrico Bernieri</a>, <a href="/search/physics?searchtype=author&amp;query=Biare%2C+D">David Biare</a> , et al. (572 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="2006.11760v1-abstract-short" style="display: inline;"> The Jiangmen Underground Neutrino Observatory~(JUNO) features a 20~kt multi-purpose underground liquid scintillator sphere as its main detector. Some of JUNO&#39;s features make it an excellent experiment for $^8$B solar neutrino measurements, such as its low-energy threshold, its high energy resolution compared to water Cherenkov detectors, and its much large target mass compared to previous liquid s&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2006.11760v1-abstract-full').style.display = 'inline'; document.getElementById('2006.11760v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2006.11760v1-abstract-full" style="display: none;"> The Jiangmen Underground Neutrino Observatory~(JUNO) features a 20~kt multi-purpose underground liquid scintillator sphere as its main detector. Some of JUNO&#39;s features make it an excellent experiment for $^8$B solar neutrino measurements, such as its low-energy threshold, its high energy resolution compared to water Cherenkov detectors, and its much large target mass compared to previous liquid scintillator detectors. In this paper we present a comprehensive assessment of JUNO&#39;s potential for detecting $^8$B solar neutrinos via the neutrino-electron elastic scattering process. A reduced 2~MeV threshold on the recoil electron energy is found to be achievable assuming the intrinsic radioactive background $^{238}$U and $^{232}$Th in the liquid scintillator can be controlled to 10$^{-17}$~g/g. With ten years of data taking, about 60,000 signal and 30,000 background events are expected. This large sample will enable an examination of the distortion of the recoil electron spectrum that is dominated by the neutrino flavor transformation in the dense solar matter, which will shed new light on the tension between the measured electron spectra and the predictions of the standard three-flavor neutrino oscillation framework. If $螖m^{2}_{21}=4.8\times10^{-5}~(7.5\times10^{-5})$~eV$^{2}$, JUNO can provide evidence of neutrino oscillation in the Earth at the about 3$蟽$~(2$蟽$) level by measuring the non-zero signal rate variation with respect to the solar zenith angle. Moveover, JUNO can simultaneously measure $螖m^2_{21}$ using $^8$B solar neutrinos to a precision of 20\% or better depending on the central value and to sub-percent precision using reactor antineutrinos. A comparison of these two measurements from the same detector will help elucidate the current tension between the value of $螖m^2_{21}$ reported by solar neutrino experiments and the KamLAND experiment. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2006.11760v1-abstract-full').style.display = 'none'; document.getElementById('2006.11760v1-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 June, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 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">29 pages, 14 plots, 7 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/2005.11569">arXiv:2005.11569</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2005.11569">pdf</a>, <a href="https://arxiv.org/ps/2005.11569">ps</a>, <a href="https://arxiv.org/format/2005.11569">other</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="Mesoscale and Nanoscale Physics">cond-mat.mes-hall</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/PhysRevApplied.13.064062">10.1103/PhysRevApplied.13.064062 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Generalized scaling law for exciton binding energy in two-dimensional materials </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">S. Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Zubair%2C+M">M. Zubair</a>, <a href="/search/physics?searchtype=author&amp;query=Jalil%2C+O">O. Jalil</a>, <a href="/search/physics?searchtype=author&amp;query=Mehmood%2C+M+Q">M. Q. Mehmood</a>, <a href="/search/physics?searchtype=author&amp;query=Younis%2C+U">U. Younis</a>, <a href="/search/physics?searchtype=author&amp;query=Liu%2C+X">X. Liu</a>, <a href="/search/physics?searchtype=author&amp;query=Ang%2C+K+W">K. W. Ang</a>, <a href="/search/physics?searchtype=author&amp;query=Ang%2C+L+K">L. K. Ang</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="2005.11569v1-abstract-short" style="display: inline;"> Binding energy calculation in two-dimensional (2D) materials is crucial in determining their electronic and optical properties pertaining to enhanced Coulomb interactions between charge carriers due to quantum confinement and reduced dielectric screening. Based on full solutions of the Schr枚dinger equation in screened hydrogen model with a modified Coulomb potential ($1/r^{尾-2}$), we present a gen&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.11569v1-abstract-full').style.display = 'inline'; document.getElementById('2005.11569v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2005.11569v1-abstract-full" style="display: none;"> Binding energy calculation in two-dimensional (2D) materials is crucial in determining their electronic and optical properties pertaining to enhanced Coulomb interactions between charge carriers due to quantum confinement and reduced dielectric screening. Based on full solutions of the Schr枚dinger equation in screened hydrogen model with a modified Coulomb potential ($1/r^{尾-2}$), we present a generalized and analytical scaling law for exciton binding energy, $E_尾 = E_{0}\times \big (\,a尾^{b}+c\big )\, (渭/蔚^{2})$, where $尾$ is a fractional-dimension parameter accounted for the reduced dielectric screening. The model is able to provide accurate binding energies, benchmarked with the reported Bethe-Salpeter Equation (BSE) and experimental data, for 58 mono-layer 2D and 8 bulk materials respectively through $尾$. For a given material, $尾$ is varied from $尾$ = 3 for bulk 3D materials to a value lying in the range 2.55$-$2.7 for 2D mono-layer materials. With $尾_{\text{mean}}$ = 2.625, our model improves the average relative mean square error by 3 times in comparison to existing models. The results can be used for Coulomb engineering of exciton binding energies in the optimal design of 2D materials. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.11569v1-abstract-full').style.display = 'none'; document.getElementById('2005.11569v1-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 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">Accepted (in-press) for publication in Physical Review Applied. Accepted article is available at this URL: https://journals.aps.org/prapplied/accepted/8607dYcbA3b1de6467a97ee13f63bee882eb2d391</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Applied 13, 064062 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2005.08745">arXiv:2005.08745</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2005.08745">pdf</a>, <a href="https://arxiv.org/format/2005.08745">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</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="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> TAO Conceptual Design Report: A Precision Measurement of the Reactor Antineutrino Spectrum with Sub-percent Energy Resolution </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=JUNO+Collaboration"> JUNO Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Abusleme%2C+A">Angel Abusleme</a>, <a href="/search/physics?searchtype=author&amp;query=Adam%2C+T">Thomas Adam</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeel Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Aiello%2C+S">Sebastiano Aiello</a>, <a href="/search/physics?searchtype=author&amp;query=Akram%2C+M">Muhammad Akram</a>, <a href="/search/physics?searchtype=author&amp;query=Ali%2C+N">Nawab Ali</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+F">Fengpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+G">Guangpeng An</a>, <a href="/search/physics?searchtype=author&amp;query=An%2C+Q">Qi An</a>, <a href="/search/physics?searchtype=author&amp;query=Andronico%2C+G">Giuseppe Andronico</a>, <a href="/search/physics?searchtype=author&amp;query=Anfimov%2C+N">Nikolay Anfimov</a>, <a href="/search/physics?searchtype=author&amp;query=Antonelli%2C+V">Vito Antonelli</a>, <a href="/search/physics?searchtype=author&amp;query=Antoshkina%2C+T">Tatiana Antoshkina</a>, <a href="/search/physics?searchtype=author&amp;query=Asavapibhop%2C+B">Burin Asavapibhop</a>, <a href="/search/physics?searchtype=author&amp;query=de+Andr%C3%A9%2C+J+P+A+M">Jo茫o Pedro Athayde Marcondes de Andr茅</a>, <a href="/search/physics?searchtype=author&amp;query=Auguste%2C+D">Didier Auguste</a>, <a href="/search/physics?searchtype=author&amp;query=Babic%2C+A">Andrej Babic</a>, <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+W">Wander Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Barresi%2C+A">Andrea Barresi</a>, <a href="/search/physics?searchtype=author&amp;query=Baussan%2C+E">Eric Baussan</a>, <a href="/search/physics?searchtype=author&amp;query=Bellato%2C+M">Marco Bellato</a>, <a href="/search/physics?searchtype=author&amp;query=Bergnoli%2C+A">Antonio Bergnoli</a>, <a href="/search/physics?searchtype=author&amp;query=Bernieri%2C+E">Enrico Bernieri</a>, <a href="/search/physics?searchtype=author&amp;query=Biare%2C+D">David Biare</a> , et al. (568 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="2005.08745v1-abstract-short" style="display: inline;"> The Taishan Antineutrino Observatory (TAO, also known as JUNO-TAO) is a satellite experiment of the Jiangmen Underground Neutrino Observatory (JUNO). A ton-level liquid scintillator detector will be placed at about 30 m from a core of the Taishan Nuclear Power Plant. The reactor antineutrino spectrum will be measured with sub-percent energy resolution, to provide a reference spectrum for future re&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.08745v1-abstract-full').style.display = 'inline'; document.getElementById('2005.08745v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2005.08745v1-abstract-full" style="display: none;"> The Taishan Antineutrino Observatory (TAO, also known as JUNO-TAO) is a satellite experiment of the Jiangmen Underground Neutrino Observatory (JUNO). A ton-level liquid scintillator detector will be placed at about 30 m from a core of the Taishan Nuclear Power Plant. The reactor antineutrino spectrum will be measured with sub-percent energy resolution, to provide a reference spectrum for future reactor neutrino experiments, and to provide a benchmark measurement to test nuclear databases. A spherical acrylic vessel containing 2.8 ton gadolinium-doped liquid scintillator will be viewed by 10 m^2 Silicon Photomultipliers (SiPMs) of &gt;50% photon detection efficiency with almost full coverage. The photoelectron yield is about 4500 per MeV, an order higher than any existing large-scale liquid scintillator detectors. The detector operates at -50 degree C to lower the dark noise of SiPMs to an acceptable level. The detector will measure about 2000 reactor antineutrinos per day, and is designed to be well shielded from cosmogenic backgrounds and ambient radioactivities to have about 10% background-to-signal ratio. The experiment is expected to start operation in 2022. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.08745v1-abstract-full').style.display = 'none'; document.getElementById('2005.08745v1-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, 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">134 pages, 114 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/2005.04937">arXiv:2005.04937</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2005.04937">pdf</a>, <a href="https://arxiv.org/format/2005.04937">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Populations and Evolution">q-bio.PE</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Physics and Society">physics.soc-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/10.1016/j.idm.2020.06.008">10.1016/j.idm.2020.06.008 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Using statistics and mathematical modelling to understand infectious disease outbreaks: COVID-19 as an example </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Overton%2C+C+E">Christopher E. Overton</a>, <a href="/search/physics?searchtype=author&amp;query=Stage%2C+H+B">Helena B. Stage</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shazaad Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Curran-Sebastian%2C+J">Jacob Curran-Sebastian</a>, <a href="/search/physics?searchtype=author&amp;query=Dark%2C+P">Paul Dark</a>, <a href="/search/physics?searchtype=author&amp;query=Das%2C+R">Rajenki Das</a>, <a href="/search/physics?searchtype=author&amp;query=Fearon%2C+E">Elizabeth Fearon</a>, <a href="/search/physics?searchtype=author&amp;query=Felton%2C+T">Timothy Felton</a>, <a href="/search/physics?searchtype=author&amp;query=Fyles%2C+M">Martyn Fyles</a>, <a href="/search/physics?searchtype=author&amp;query=Gent%2C+N">Nick Gent</a>, <a href="/search/physics?searchtype=author&amp;query=Hall%2C+I">Ian Hall</a>, <a href="/search/physics?searchtype=author&amp;query=House%2C+T">Thomas House</a>, <a href="/search/physics?searchtype=author&amp;query=Lewkowicz%2C+H">Hugo Lewkowicz</a>, <a href="/search/physics?searchtype=author&amp;query=Pang%2C+X">Xiaoxi Pang</a>, <a href="/search/physics?searchtype=author&amp;query=Pellis%2C+L">Lorenzo Pellis</a>, <a href="/search/physics?searchtype=author&amp;query=Sawko%2C+R">Robert Sawko</a>, <a href="/search/physics?searchtype=author&amp;query=Ustianowski%2C+A">Andrew Ustianowski</a>, <a href="/search/physics?searchtype=author&amp;query=Vekaria%2C+B">Bindu Vekaria</a>, <a href="/search/physics?searchtype=author&amp;query=Webb%2C+L">Luke Webb</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="2005.04937v1-abstract-short" style="display: inline;"> During an infectious disease outbreak, biases in the data and complexities of the underlying dynamics pose significant challenges in mathematically modelling the outbreak and designing policy. Motivated by the ongoing response to COVID-19, we provide a toolkit of statistical and mathematical models beyond the simple SIR-type differential equation models for analysing the early stages of an outbrea&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.04937v1-abstract-full').style.display = 'inline'; document.getElementById('2005.04937v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2005.04937v1-abstract-full" style="display: none;"> During an infectious disease outbreak, biases in the data and complexities of the underlying dynamics pose significant challenges in mathematically modelling the outbreak and designing policy. Motivated by the ongoing response to COVID-19, we provide a toolkit of statistical and mathematical models beyond the simple SIR-type differential equation models for analysing the early stages of an outbreak and assessing interventions. In particular, we focus on parameter estimation in the presence of known biases in the data, and the effect of non-pharmaceutical interventions in enclosed subpopulations, such as households and care homes. We illustrate these methods by applying them to the COVID-19 pandemic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.04937v1-abstract-full').style.display = 'none'; document.getElementById('2005.04937v1-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 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">Journal ref:</span> Infectious Disease Modelling, Volume 5 (2020), 409-441 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2004.12283">arXiv:2004.12283</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2004.12283">pdf</a>, <a href="https://arxiv.org/format/2004.12283">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Social and Information Networks">cs.SI</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Physics and Society">physics.soc-ph</span> </div> </div> <p class="title is-5 mathjax"> Hierarchical Clustering of World Cuisines </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Sharma%2C+T">Tript Sharma</a>, <a href="/search/physics?searchtype=author&amp;query=Upadhyay%2C+U">Utkarsh Upadhyay</a>, <a href="/search/physics?searchtype=author&amp;query=Kalra%2C+J">Jushaan Kalra</a>, <a href="/search/physics?searchtype=author&amp;query=Arora%2C+S">Sakshi Arora</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Saad Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Aggarwal%2C+B">Bhavay Aggarwal</a>, <a href="/search/physics?searchtype=author&amp;query=Bagler%2C+G">Ganesh Bagler</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="2004.12283v1-abstract-short" style="display: inline;"> Cultures across the world have evolved to have unique patterns despite shared ingredients and cooking techniques. Using data obtained from RecipeDB, an online resource for recipes, we extract patterns in 26 world cuisines and further probe for their inter-relatedness. By application of frequent itemset mining and ingredient authenticity we characterize the quintessential patterns in the cuisines a&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2004.12283v1-abstract-full').style.display = 'inline'; document.getElementById('2004.12283v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2004.12283v1-abstract-full" style="display: none;"> Cultures across the world have evolved to have unique patterns despite shared ingredients and cooking techniques. Using data obtained from RecipeDB, an online resource for recipes, we extract patterns in 26 world cuisines and further probe for their inter-relatedness. By application of frequent itemset mining and ingredient authenticity we characterize the quintessential patterns in the cuisines and build a hierarchical tree of the world cuisines. This tree provides interesting insights into the evolution of cuisines and their geographical as well as historical relatedness. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2004.12283v1-abstract-full').style.display = 'none'; document.getElementById('2004.12283v1-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 April, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 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">36th IEEE International Conference on Data Engineering (ICDE 2020), DECOR Workshop; 6 pages, 6 figures, 1 table</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2004.11590">arXiv:2004.11590</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2004.11590">pdf</a>, <a href="https://arxiv.org/format/2004.11590">other</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="Materials Science">cond-mat.mtrl-sci</span> </div> </div> <p class="title is-5 mathjax"> Towards unification of perovskite stability and photovoltaic performance assessment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Wenger%2C+B">Bernard Wenger</a>, <a href="/search/physics?searchtype=author&amp;query=Snaith%2C+H+J">Henry J. Snaith</a>, <a href="/search/physics?searchtype=author&amp;query=S%C3%B6rensen%2C+I+H">Isabel H. S枚rensen</a>, <a href="/search/physics?searchtype=author&amp;query=Ripperger%2C+J">Johannes Ripperger</a>, <a href="/search/physics?searchtype=author&amp;query=Kazim%2C+S">Samrana Kazim</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shahzada Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Nandayapa%2C+E+R">Edgar R. Nandayapa</a>, <a href="/search/physics?searchtype=author&amp;query=Boeffel%2C+C">Christine Boeffel</a>, <a href="/search/physics?searchtype=author&amp;query=Colodrero%2C+S">Silvia Colodrero</a>, <a href="/search/physics?searchtype=author&amp;query=Anaya%2C+M">Miguel Anaya</a>, <a href="/search/physics?searchtype=author&amp;query=Stranks%2C+S+D">Samuel D. Stranks</a>, <a href="/search/physics?searchtype=author&amp;query=Mora-Ser%C3%B3%2C+I">Iv谩n Mora-Ser贸</a>, <a href="/search/physics?searchtype=author&amp;query=Yang%2C+T+C">Terry Chien-Jen Yang</a>, <a href="/search/physics?searchtype=author&amp;query=Br%C3%A4uninger%2C+M">Matthias Br盲uninger</a>, <a href="/search/physics?searchtype=author&amp;query=Rissom%2C+T">Thorsten Rissom</a>, <a href="/search/physics?searchtype=author&amp;query=Aernouts%2C+T">Tom Aernouts</a>, <a href="/search/physics?searchtype=author&amp;query=Hadjipanayi%2C+M">Maria Hadjipanayi</a>, <a href="/search/physics?searchtype=author&amp;query=Paraskeva%2C+V">Vasiliki Paraskeva</a>, <a href="/search/physics?searchtype=author&amp;query=Georghiou%2C+G+E">George E. Georghiou</a>, <a href="/search/physics?searchtype=author&amp;query=Walker%2C+A+B">Alison B. Walker</a>, <a href="/search/physics?searchtype=author&amp;query=Walter%2C+A">Arnaud Walter</a>, <a href="/search/physics?searchtype=author&amp;query=Nicolay%2C+S">Sylvain Nicolay</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="2004.11590v2-abstract-short" style="display: inline;"> With the rapid progress of perovskite photovoltaics (PV), further challenges arise to meet meet the minimum standards required for commercial deployment. Along with the push towards higher efficiencies, we identify a need to improve the quality and uniformity of reported research data and to focus efforts upon understanding and overcoming failures during operation. In this perspective, as a large&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2004.11590v2-abstract-full').style.display = 'inline'; document.getElementById('2004.11590v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2004.11590v2-abstract-full" style="display: none;"> With the rapid progress of perovskite photovoltaics (PV), further challenges arise to meet meet the minimum standards required for commercial deployment. Along with the push towards higher efficiencies, we identify a need to improve the quality and uniformity of reported research data and to focus efforts upon understanding and overcoming failures during operation. In this perspective, as a large and representative consortium of researchers active in this field, we discuss which methods require special attention and issue a series of recommendations to improve research practices and reporting. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2004.11590v2-abstract-full').style.display = 'none'; document.getElementById('2004.11590v2-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 April, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 24 April, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2020. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1904.08323">arXiv:1904.08323</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1904.08323">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="Materials Science">cond-mat.mtrl-sci</span> </div> </div> <p class="title is-5 mathjax"> Gas-phase synthesis of carbon nanotube-graphene heterostructures </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Saeed Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Jiang%2C+H">Hua Jiang</a>, <a href="/search/physics?searchtype=author&amp;query=Mustonen%2C+K">Kimmo Mustonen</a>, <a href="/search/physics?searchtype=author&amp;query=Zhang%2C+Q">Qiang Zhang</a>, <a href="/search/physics?searchtype=author&amp;query=Hussain%2C+A">Aqeel Hussain</a>, <a href="/search/physics?searchtype=author&amp;query=Khan%2C+A+T">Abu Taher Khan</a>, <a href="/search/physics?searchtype=author&amp;query=Wei%2C+N">Nan Wei</a>, <a href="/search/physics?searchtype=author&amp;query=Tavakkoli%2C+M">Mohammad Tavakkoli</a>, <a href="/search/physics?searchtype=author&amp;query=Liao%2C+Y">Yongping Liao</a>, <a href="/search/physics?searchtype=author&amp;query=Ding%2C+E">Er-Xiong Ding</a>, <a href="/search/physics?searchtype=author&amp;query=Kotakoski%2C+J">Jani Kotakoski</a>, <a href="/search/physics?searchtype=author&amp;query=Kauppinen%2C+E+I">Esko I. Kauppinen</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="1904.08323v1-abstract-short" style="display: inline;"> Graphene and carbon nanotubes (CNTs) share the same atomic structure of hexagonal carbon lattice. Yet, their synthesis differs in many aspects, including the shape and size of the catalyst. Here, we demonstrate a floating-catalyst chemical vapor deposition (FCCVD) technique for substrate-free, single-step growth of CNT-graphene heterostructures (CNT-G-H) using ethylene as a carbon source. The form&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1904.08323v1-abstract-full').style.display = 'inline'; document.getElementById('1904.08323v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1904.08323v1-abstract-full" style="display: none;"> Graphene and carbon nanotubes (CNTs) share the same atomic structure of hexagonal carbon lattice. Yet, their synthesis differs in many aspects, including the shape and size of the catalyst. Here, we demonstrate a floating-catalyst chemical vapor deposition (FCCVD) technique for substrate-free, single-step growth of CNT-graphene heterostructures (CNT-G-H) using ethylene as a carbon source. The formation of CNT-G-H is directly evidenced by lattice-resolved (scanning) transmission electron microscopy (STEM) and electron diffraction experiments, corroborated by atomic force microscopy (AFM). Our experiments show the relative number density of graphene-nanoflakes can be tuned by optimizing the synthesis conditions. Since in the applied process the formation of the structures take place in gas-suspension, the as-synthesized CNT-G-H films can be deposited on any surface in ambient temperature with an arbitrary thickness. Moreover, this process of CNT-G-H synthesis with strong universality has also been realized in multiple systems of ethylene-based FCCVD with various catalysts and set-ups. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1904.08323v1-abstract-full').style.display = 'none'; document.getElementById('1904.08323v1-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 April, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2019. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1903.09801">arXiv:1903.09801</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1903.09801">pdf</a>, <a href="https://arxiv.org/ps/1903.09801">ps</a>, <a href="https://arxiv.org/format/1903.09801">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Plasma Physics">physics.plasm-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</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.122.105101">10.1103/PhysRevLett.122.105101 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of the Electrical Properties of a Thundercloud Through Muon Imaging by the GRAPES-3 Experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Hariharan%2C+B">B. Hariharan</a>, <a href="/search/physics?searchtype=author&amp;query=Chandra%2C+A">A. Chandra</a>, <a href="/search/physics?searchtype=author&amp;query=Dugad%2C+S+R">S. R. Dugad</a>, <a href="/search/physics?searchtype=author&amp;query=Gupta%2C+S+K">S. K. Gupta</a>, <a href="/search/physics?searchtype=author&amp;query=Jagadeesan%2C+P">P. Jagadeesan</a>, <a href="/search/physics?searchtype=author&amp;query=Jain%2C+A">A. Jain</a>, <a href="/search/physics?searchtype=author&amp;query=Mohanty%2C+P+K">P. K. Mohanty</a>, <a href="/search/physics?searchtype=author&amp;query=Morris%2C+S+D">S. D. Morris</a>, <a href="/search/physics?searchtype=author&amp;query=Nayak%2C+P+K">P. K. Nayak</a>, <a href="/search/physics?searchtype=author&amp;query=Rakshe%2C+P+S">P. S. Rakshe</a>, <a href="/search/physics?searchtype=author&amp;query=Ramesh%2C+K">K. Ramesh</a>, <a href="/search/physics?searchtype=author&amp;query=Rao%2C+B+S">B. S. Rao</a>, <a href="/search/physics?searchtype=author&amp;query=Reddy%2C+L+V">L. V. Reddy</a>, <a href="/search/physics?searchtype=author&amp;query=Zuberi%2C+M">M. Zuberi</a>, <a href="/search/physics?searchtype=author&amp;query=Hayashi%2C+Y">Y. Hayashi</a>, <a href="/search/physics?searchtype=author&amp;query=Kawakami%2C+S">S. Kawakami</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">S. Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Kojima%2C+H">H. Kojima</a>, <a href="/search/physics?searchtype=author&amp;query=Oshima%2C+A">A. Oshima</a>, <a href="/search/physics?searchtype=author&amp;query=Shibata%2C+S">S. Shibata</a>, <a href="/search/physics?searchtype=author&amp;query=Muraki%2C+Y">Y. Muraki</a>, <a href="/search/physics?searchtype=author&amp;query=Tanaka%2C+K">K. Tanaka</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="1903.09801v1-abstract-short" style="display: inline;"> The GRAPES-3 muon telescope located in Ooty, India records rapid ($\sim$10 min) variations in the muon intensity during major thunderstorms. Out of a total of 184 thunderstorms recorded during the interval April 2011-December 2014, the one on 1 December 2014 produced a massive potential of 1.3 GV. The electric field measured by four well-separated (up to 6 km) monitors on the ground was used to he&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1903.09801v1-abstract-full').style.display = 'inline'; document.getElementById('1903.09801v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1903.09801v1-abstract-full" style="display: none;"> The GRAPES-3 muon telescope located in Ooty, India records rapid ($\sim$10 min) variations in the muon intensity during major thunderstorms. Out of a total of 184 thunderstorms recorded during the interval April 2011-December 2014, the one on 1 December 2014 produced a massive potential of 1.3 GV. The electric field measured by four well-separated (up to 6 km) monitors on the ground was used to help estimate some of the properties of this thundercloud including its altitude and area that were found to be 11.4 km above mean sea level (amsl) and $\geq$380 km$^2$, respectively. A charging time of 6 min to reach 1.3 GV implied the delivery of a power of $\geq$2 GW by this thundercloud that was moving at a speed of $\sim$60 km h$^{-1}$. This work possibly provides the first direct evidence for the generation of GV potentials in thunderclouds that could also possibly explain the production of highest energy (100 MeV) $纬$-rays in the terrestrial $纬$-ray flashes. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1903.09801v1-abstract-full').style.display = 'none'; document.getElementById('1903.09801v1-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 March, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2019. </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">Received 6 January 2019, Revised 21 January 2019, Published 15 March 2019</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 122, 105101 (2019) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1712.02937">arXiv:1712.02937</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1712.02937">pdf</a>, <a href="https://arxiv.org/ps/1712.02937">ps</a>, <a href="https://arxiv.org/format/1712.02937">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Physics and Society">physics.soc-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Econometrics">econ.EM</span> </div> </div> <p class="title is-5 mathjax"> On Metropolis Growth </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S+A">Syed Amaar Ahmad</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="1712.02937v2-abstract-short" style="display: inline;"> We consider the scaling laws, second-order statistics and entropy of the consumed energy of metropolis cities which are hybrid complex systems comprising social networks, engineering systems, agricultural output, economic activity and energy components. We abstract a city in terms of two fundamental variables; $s$ resource cells (of unit area) that represent energy-consuming geographic or spatial&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1712.02937v2-abstract-full').style.display = 'inline'; document.getElementById('1712.02937v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1712.02937v2-abstract-full" style="display: none;"> We consider the scaling laws, second-order statistics and entropy of the consumed energy of metropolis cities which are hybrid complex systems comprising social networks, engineering systems, agricultural output, economic activity and energy components. We abstract a city in terms of two fundamental variables; $s$ resource cells (of unit area) that represent energy-consuming geographic or spatial zones (e.g. land, housing or infrastructure etc.) and a population comprising $n$ mobile units that can migrate between these cells. We show that with a constant metropolis area (fixed $s$), the variance and entropy of consumed energy initially increase with $n$, reach a maximum and then eventually diminish to zero as saturation is reached. These metrics are indicators of the spatial mobility of the population. Under certain situations, the variance is bounded as a quadratic function of the mean consumed energy of the metropolis. However, when population and metropolis area are endogenous, growth in the latter is arrested when $n\leq\frac{s}{2}\log(s)$ due to diminished population density. Conversely, the population growth reaches equilibrium when $n\geq {s}\log{n}$ or equivalently when the aggregate of both over-populated and under-populated areas is large. Moreover, we also draw the relationship between our approach and multi-scalar information, when economic dependency between a metropolis&#39;s sub-regions is based on the entropy of consumed energy. Finally, if the city&#39;s economic size (domestic product etc.) is proportional to the consumed energy, then for a constant population density, we show that the economy scales linearly with the surface area (or $s$). <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1712.02937v2-abstract-full').style.display = 'none'; document.getElementById('1712.02937v2-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 December, 2017; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 7 December, 2017; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 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">19 pages, 16 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/1611.04863">arXiv:1611.04863</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1611.04863">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Plasma Physics">physics.plasm-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/10.1088/0022-3727/40/5/015">10.1088/0022-3727/40/5/015 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Regenerative Soot-IX: C3 as the dominant, stable carbon cluster in high pressure sooting discharges </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Janjua%2C+S+A">Sohail Ahmad Janjua</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+M">M. Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Khan%2C+S+D">S. D. Khan</a>, <a href="/search/physics?searchtype=author&amp;query=Khalid%2C+R">R. Khalid</a>, <a href="/search/physics?searchtype=author&amp;query=Aleem%2C+A">A. Aleem</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shoaib Ahmad</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="1611.04863v1-abstract-short" style="display: inline;"> Results are presented that have been obtained while operating the graphite hollow cathode duoplasmatron ion source in dual mode under constant discharge current. This dual mode operation enabled us to obtain the mass and emission spectra simultaneously. In mass spectra C3 is the main feature but C4 and C5 are also prominent, whereas in emission spectra C2 is also there and its presence shows that&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1611.04863v1-abstract-full').style.display = 'inline'; document.getElementById('1611.04863v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1611.04863v1-abstract-full" style="display: none;"> Results are presented that have been obtained while operating the graphite hollow cathode duoplasmatron ion source in dual mode under constant discharge current. This dual mode operation enabled us to obtain the mass and emission spectra simultaneously. In mass spectra C3 is the main feature but C4 and C5 are also prominent, whereas in emission spectra C2 is also there and its presence shows that it is in an excited state rather than in an ionic state. These facts provide evidence that C3 is produced due to the regeneration of a soot forming sequence and leave it in ionic state. C3 is a stable molecule and the only dominant species among the carbon clusters that survives in a regenerative sooting environment at high-pressure discharges. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1611.04863v1-abstract-full').style.display = 'none'; document.getElementById('1611.04863v1-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, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2016. </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, 5 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> J. Phys. D: Appl. Phys. 40, 1416, 2007 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1609.09347">arXiv:1609.09347</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1609.09347">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Atomic and Molecular Clusters">physics.atm-clus</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="Instrumentation and Detectors">physics.ins-det</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/10.1016/j.nimb.2012.10.012">10.1016/j.nimb.2012.10.012 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Dynamics of fragmentation and multiple vacancy generation in irradiated single-walled carbon nanotubes </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Javeed%2C+S">Sumera Javeed</a>, <a href="/search/physics?searchtype=author&amp;query=Zeeshan%2C+S">Sumaira Zeeshan</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shoaib Ahmad</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="1609.09347v1-abstract-short" style="display: inline;"> The results from mass spectrometry of clusters sputtered from Cs+ irradiated single-walled carbon nano-tubes (SWCNTs) as a function of energy and dose identify the nature of the resulting damage in the form of multiple vacancy generation. For pristine SWCNTs at all Cs+ energies, C2 is the most dominant species, followed by C3, C4 and C1. The experiments were performed in three stages: in the first&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.09347v1-abstract-full').style.display = 'inline'; document.getElementById('1609.09347v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1609.09347v1-abstract-full" style="display: none;"> The results from mass spectrometry of clusters sputtered from Cs+ irradiated single-walled carbon nano-tubes (SWCNTs) as a function of energy and dose identify the nature of the resulting damage in the form of multiple vacancy generation. For pristine SWCNTs at all Cs+ energies, C2 is the most dominant species, followed by C3, C4 and C1. The experiments were performed in three stages: in the first stage, Cs+ energy E(Cs+) was varied. During the second stage, the nanotubes were irradiated continuously at E(Cs+) = 5 keV for 1,800 s. Afterwards, the entire sequence of irradiation energies was repeated to differentiate between the fragmentation patterns of the pristine and of heavily irradiated SWCNTs. The sputtering and normalized yields identify the quantitative and relative extent of the ion-induced damage by creating double, triple and quadruple vacancies; the single vacancies are least favored. Sputtering from the heavily irradiated SWCNTs occurs not only from the damaged and fragmented nanotubes, but also from the inter-nanotube structures that are grown due to the accumulation of the sputtered clusters. Similar irradiation experiments were performed with the multi-walled carbon nanotubes; the results confirmed the dominant C2 followed by C3, C4 and C1. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.09347v1-abstract-full').style.display = 'none'; document.getElementById('1609.09347v1-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 September, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2016. </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, 9 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nuclear Instruments and Methods in Physics Research B 295,22, 2013 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1609.06746">arXiv:1609.06746</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1609.06746">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</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/10.1016/S0168-583X(96)00683-0">10.1016/S0168-583X(96)00683-0 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Carbon cluster diagnostics-I: Direct Recoil Spectroscopy (DRS) of Ar+ and Kr+ bombarded graphite </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shoaib Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Akhtar%2C+M+N">M. N. Akhtar</a>, <a href="/search/physics?searchtype=author&amp;query=Qayyum%2C+A">A. Qayyum</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+B">B. Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Bahar%2C+K">K. Bahar</a>, <a href="/search/physics?searchtype=author&amp;query=Arshed%2C+W">W. Arshed</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="1609.06746v1-abstract-short" style="display: inline;"> Measurements of the energy spectra of multiply charged positive and negative carbon ions recoiling from graphite surface under 100 and 150 keV argon and krypton ion bombardment are presented. With the energy spectrometer set at recoil angle of 79.5 degrees, direct recoil (DR) peaks have been observed with singly as well as multiply charged carbon ions , where n = 1 to 6. These monatomic and cluste&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.06746v1-abstract-full').style.display = 'inline'; document.getElementById('1609.06746v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1609.06746v1-abstract-full" style="display: none;"> Measurements of the energy spectra of multiply charged positive and negative carbon ions recoiling from graphite surface under 100 and 150 keV argon and krypton ion bombardment are presented. With the energy spectrometer set at recoil angle of 79.5 degrees, direct recoil (DR) peaks have been observed with singly as well as multiply charged carbon ions , where n = 1 to 6. These monatomic and cluster ions have been observed recoiling with the characteristic recoil energy E(DR) . We have observed sharp DR peaks. A collimated projectile beam with small divergence is supplemented with a similar collimation before the energy analyzer to reduce the background of sputtered ions due to scattered projectiles. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.06746v1-abstract-full').style.display = 'none'; document.getElementById('1609.06746v1-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 September, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2016. </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, 5 figures, 2 tables</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nuclear Instruments and Methods in Physics Research B 122, 19, 1997 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1609.02070">arXiv:1609.02070</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1609.02070">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Atomic and Molecular Clusters">physics.atm-clus</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Mesoscale and Nanoscale Physics">cond-mat.mes-hall</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/10.1016/j.ijms.2011.11.006">10.1016/j.ijms.2011.11.006 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Mass spectrometric identification of C60 fragmentation regimes under energetic Cs+ bombardment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Zeeshan%2C+S">Sumaira Zeeshan</a>, <a href="/search/physics?searchtype=author&amp;query=Javeed%2C+S">Sumera Javeed</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shoaib Ahmad</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="1609.02070v1-abstract-short" style="display: inline;"> Three C60 fragmentation regimes in fullerite bombarded by Cs+ are identified as a function of its energy. C2 is the major species sputtered at all energies. For E(Cs+) &lt; 1 keV C2 emissions dominate. C2 and C1 have highest intensities between 1 and 3 keV with increasing contributions from C3 and C4. Intensities of all fragments maximize around 2 keV. Above 3 keV, fragments densities stabilize. The&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.02070v1-abstract-full').style.display = 'inline'; document.getElementById('1609.02070v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1609.02070v1-abstract-full" style="display: none;"> Three C60 fragmentation regimes in fullerite bombarded by Cs+ are identified as a function of its energy. C2 is the major species sputtered at all energies. For E(Cs+) &lt; 1 keV C2 emissions dominate. C2 and C1 have highest intensities between 1 and 3 keV with increasing contributions from C3 and C4. Intensities of all fragments maximize around 2 keV. Above 3 keV, fragments densities stabilize. The roles of and the contributions from direct recoils and collision cascades are determined. Maximum direct recoil energy delivered to the C60 fullerite cage is 210 eV at which only C2 emissions occur is identified and an explanation provided. The three fragmentation regimes under continued Cs+ bombardment eventually lead to complete destruction of the C60 cages transforming fullerite into amorphous carbon <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.02070v1-abstract-full').style.display = 'none'; document.getElementById('1609.02070v1-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 September, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2016. </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> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> International Journal of Mass Spectrometry 311, 1, 2012 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1609.01947">arXiv:1609.01947</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1609.01947">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Chemical Physics">physics.chem-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Mesoscale and Nanoscale Physics">cond-mat.mes-hall</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/10.1088/0957-4484/17/18/021">10.1088/0957-4484/17/18/021 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Modelling of C2 addition route to the formation of C60 </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Khan%2C+S+D">Sabih D Khan</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shoaib Ahmad</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="1609.01947v1-abstract-short" style="display: inline;"> To understand the phenomenon of fullerene growth during its synthesis, an attempt is made to model a minimum energy growth route using a semi-empirical quantum mechanics code. C2 addition leading to C60 was modelled and three main routes, i.e. cyclic ring growth, pentagon and fullerene road, were studied. The growth starts with linear chains and, at n = 10, ring structures begins to dominate. The&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.01947v1-abstract-full').style.display = 'inline'; document.getElementById('1609.01947v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1609.01947v1-abstract-full" style="display: none;"> To understand the phenomenon of fullerene growth during its synthesis, an attempt is made to model a minimum energy growth route using a semi-empirical quantum mechanics code. C2 addition leading to C60 was modelled and three main routes, i.e. cyclic ring growth, pentagon and fullerene road, were studied. The growth starts with linear chains and, at n = 10, ring structures begins to dominate. The rings continue to grow and, at some point n &gt; 30, they transform into close-cage fullerenes and the growth is shown to progress by the fullerene road until C60 is formed. The computer simulations predict a transition from a C38 ring to fullerene. Other growth mechanisms could also occur in the energetic environment commonly encountered in fullerene synthesis, but our purpose was to identify a minimal energy route which is the most probable structure. Our results also indicate that, at n = 20, the corannulene structure is energetically more stable than the corresponding fullerene and graphene sheet, however a ring structure has lower energy among all the structures up to n 6 40. Additionally, we have also proved that the fullerene road is energetically more favored than the pentagon road. The overall growth leading to cage closure for n = 60 may not occur by a single route but by a combination of more than one route. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.01947v1-abstract-full').style.display = 'none'; document.getElementById('1609.01947v1-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 September, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2016. </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, 5 figures, 2 tables</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nanotechnology, 17, 4654, 2006 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1609.01944">arXiv:1609.01944</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1609.01944">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Atomic and Molecular Clusters">physics.atm-clus</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Mesoscale and Nanoscale Physics">cond-mat.mes-hall</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/10.1016/S0375-9601(97)00581-1">10.1016/S0375-9601(97)00581-1 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Evolution of clusters in energetic heavy ion bombarded amorphous graphite </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Akhtar%2C+M+N">M. N. Akhtar</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+B">Bashir Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shoaib Ahmad</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="1609.01944v1-abstract-short" style="display: inline;"> Carbon clusters have been generated by a novel technique of energetic heavy ion bombardment of amorphous graphite. The evolution of clusters and their subsequent fragmentation under continuing ion bombardment is revealed by detecting various clusters in the energy spectra of the direct recoils emitted as a result of collision between ions and the surface constituents. </span> <span class="abstract-full has-text-grey-dark mathjax" id="1609.01944v1-abstract-full" style="display: none;"> Carbon clusters have been generated by a novel technique of energetic heavy ion bombardment of amorphous graphite. The evolution of clusters and their subsequent fragmentation under continuing ion bombardment is revealed by detecting various clusters in the energy spectra of the direct recoils emitted as a result of collision between ions and the surface constituents. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1609.01944v1-abstract-full').style.display = 'none'; document.getElementById('1609.01944v1-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 September, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2016. </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, 3 figures, 1 table</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Physics Letters A234,367, 1997 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1608.07687">arXiv:1608.07687</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1608.07687">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="Chemical Physics">physics.chem-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/10.1140/epjd/e2013-30646-0">10.1140/epjd/e2013-30646-0 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> The role of the C2 gas in the emergence of C60 from the condensing carbon vapour </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shoaib Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Yaqub%2C+K">Kashif Yaqub</a>, <a href="/search/physics?searchtype=author&amp;query=Tasneem%2C+A">Afshan Tasneem</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="1608.07687v1-abstract-short" style="display: inline;"> A model has been developed that illustrates the emergence of C60 from the condensing carbon vapor. It is shown to depend upon the decreasing heats of formation for larger cages, exponentially increasing number of isomers for fullerenes that are larger than C60, large cages buckling induced by the pentagon-related protrusions that initiate fragmentation, the structural instability induces fragmenta&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1608.07687v1-abstract-full').style.display = 'inline'; document.getElementById('1608.07687v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1608.07687v1-abstract-full" style="display: none;"> A model has been developed that illustrates the emergence of C60 from the condensing carbon vapor. It is shown to depend upon the decreasing heats of formation for larger cages, exponentially increasing number of isomers for fullerenes that are larger than C60, large cages buckling induced by the pentagon-related protrusions that initiate fragmentation, the structural instability induces fragmentation that shrinks large cages and an evolving gas of C2 that is crucial to the whole process. The model describes a mechanism for the provision and presence of plenty of C2 during the formation and fragmentation processes. The bottom-up formations of large cages followed by the top-down cage shrinkage are shown to be stable, dynamical processes that lead to the C60 dominated fullerene ensemble. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1608.07687v1-abstract-full').style.display = 'none'; document.getElementById('1608.07687v1-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 August, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2016. </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, 7 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Eur. Phys. J. D., 67, 51, 2013 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1505.06664">arXiv:1505.06664</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1505.06664">pdf</a>, <a href="https://arxiv.org/ps/1505.06664">ps</a>, <a href="https://arxiv.org/format/1505.06664">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Physics and Society">physics.soc-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Systems and Control">eess.SY</span> </div> </div> <p class="title is-5 mathjax"> Quantifying the robustness of metro networks </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Wang%2C+X">Xiangrong Wang</a>, <a href="/search/physics?searchtype=author&amp;query=Ko%C3%A7%2C+Y">Yakup Ko莽</a>, <a href="/search/physics?searchtype=author&amp;query=Derrible%2C+S">Sybil Derrible</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S+N">Sk Nasir Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Kooij%2C+R+E">Robert E. Kooij</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="1505.06664v2-abstract-short" style="display: inline;"> Metros (heavy rail transit systems) are integral parts of urban transportation systems. Failures in their operations can have serious impacts on urban mobility, and measuring their robustness is therefore critical. Moreover, as physical networks, metros can be viewed as network topological entities, and as such they possess measurable network properties. In this paper, by using network science and&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1505.06664v2-abstract-full').style.display = 'inline'; document.getElementById('1505.06664v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1505.06664v2-abstract-full" style="display: none;"> Metros (heavy rail transit systems) are integral parts of urban transportation systems. Failures in their operations can have serious impacts on urban mobility, and measuring their robustness is therefore critical. Moreover, as physical networks, metros can be viewed as network topological entities, and as such they possess measurable network properties. In this paper, by using network science and graph theoretical concepts, we investigate both theoretical and experimental robustness metrics (i.e., the robustness indicator, the effective graph conductance, and the critical thresholds) and their performance in quantifying the robustness of metro networks under random failures or targeted attacks. We find that the theoretical metrics quantify different aspects of the robustness of metro networks. In particular, the robustness indicator captures the number of alternative paths and the effective graph conductance focuses on the length of each path. Moreover, the high positive correlation between the theoretical metrics and experimental metrics and the negative correlation within the theoretical metrics provide significant insights for planners to design more robust system while accommodating for transit specificities (e.g., alternative paths, fast transferring). <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1505.06664v2-abstract-full').style.display = 'none'; document.getElementById('1505.06664v2-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 May, 2015; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 25 May, 2015; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">13 pages, 4 figures, conference</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1408.4015">arXiv:1408.4015</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1408.4015">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Atomic Physics">physics.atom-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/10.1016/j.nima.2014.08.022">10.1016/j.nima.2014.08.022 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Photostimulated phosphor based image plate detection system for HRVUV beamline at Indus-1 synchrotron radiation source </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Haris%2C+K">K. Haris</a>, <a href="/search/physics?searchtype=author&amp;query=Singh%2C+P+J">Param Jeet Singh</a>, <a href="/search/physics?searchtype=author&amp;query=Shastri%2C+A">Aparna Shastri</a>, <a href="/search/physics?searchtype=author&amp;query=K.%2C+S">Sunanda K.</a>, <a href="/search/physics?searchtype=author&amp;query=K.%2C+B">Babita K.</a>, <a href="/search/physics?searchtype=author&amp;query=Rao%2C+S+V+N+B">S. V. N. Bhaskara Rao</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shabbir Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Tauheed%2C+A">A. Tauheed</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="1408.4015v1-abstract-short" style="display: inline;"> A high resolution vacuum ultraviolet (HRVUV) beamline based on a 6.65 meter off-plane Eagle spectrometer is in operation at the Indus-1 synchrotron radiation source, RRCAT, Indore, India. To facilitate position sensitive detection and fast spectral recording, a new BaFBr:Eu2+ phosphor based image plate (IP) detection system interchangeable with the existing photomultiplier (PMT) scanning system ha&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1408.4015v1-abstract-full').style.display = 'inline'; document.getElementById('1408.4015v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1408.4015v1-abstract-full" style="display: none;"> A high resolution vacuum ultraviolet (HRVUV) beamline based on a 6.65 meter off-plane Eagle spectrometer is in operation at the Indus-1 synchrotron radiation source, RRCAT, Indore, India. To facilitate position sensitive detection and fast spectral recording, a new BaFBr:Eu2+ phosphor based image plate (IP) detection system interchangeable with the existing photomultiplier (PMT) scanning system has been installed on this beamline. VUV photoabsorption studies on Xe, O2, N2O and SO2 are carried out to evaluate the performance of the IP detection system. An FWHM of ~ 0.5 脜 is achieved for the Xe atomic line at 1469.6 脜. Reproducibility of spectra is found to be within the experimental resolution. Compared to the PMT scanning system, the IP shows several advantages in terms of sensitivity, recording time and S/N ratio, which are highlighted in the paper. This is the first report of incorporation of an IP detection system in a VUV beamline using synchrotron radiation. Commissioning of the new detection system is expected to greatly enhance the utilization of the HRVUV beamline as a number of spectroscopic experiments which require fast recording times combined with a good signal to noise ratio are now feasible. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1408.4015v1-abstract-full').style.display = 'none'; document.getElementById('1408.4015v1-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 August, 2014; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 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">Accepted in NIM-A</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 767 (2014), p. 199 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1309.5159">arXiv:1309.5159</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1309.5159">pdf</a>, <a href="https://arxiv.org/ps/1309.5159">ps</a>, <a href="https://arxiv.org/format/1309.5159">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="General Physics">physics.gen-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/10.1088/0253-6102/59/4/09">10.1088/0253-6102/59/4/09 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> General Formalism For the BRST Symmetry </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Suhail Ahmad</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="1309.5159v1-abstract-short" style="display: inline;"> In this paper we will discuss Faddeev-Popov method for field theories with a gauge symmetry in an abstract way. We will then develope a general formalism for dealing with the BRST symmetry. This formalism will make it possible to analyse the BRST symmetry for any theory. </span> <span class="abstract-full has-text-grey-dark mathjax" id="1309.5159v1-abstract-full" style="display: none;"> In this paper we will discuss Faddeev-Popov method for field theories with a gauge symmetry in an abstract way. We will then develope a general formalism for dealing with the BRST symmetry. This formalism will make it possible to analyse the BRST symmetry for any theory. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1309.5159v1-abstract-full').style.display = 'none'; document.getElementById('1309.5159v1-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 September, 2013; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2013. </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">Published in Communications in Theoretical Physics</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Communications in Theoretical Physics, Volume 59, Issue 4, article id. 439-442 (2013) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1207.1317">arXiv:1207.1317</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1207.1317">pdf</a>, <a href="https://arxiv.org/ps/1207.1317">ps</a>, <a href="https://arxiv.org/format/1207.1317">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="General Physics">physics.gen-ph</span> </div> </div> <p class="title is-5 mathjax"> Subleading Corrections to entropy formulae (convergences and divergences) </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Suhail Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Alam%2C+S">Sharf Alam</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="1207.1317v1-abstract-short" style="display: inline;"> We know that sub-leading corrections to the hawking area law is riddled with issues which have some convergent and divergent aspects. Depending on the theory, scheme, model or even method sub-leading terms turn out to have trivial and non- trivial aspects which we are going to dwell upon. The generic character of the first sub leading logarithmic term comes out unanimously the same from all theori&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1207.1317v1-abstract-full').style.display = 'inline'; document.getElementById('1207.1317v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1207.1317v1-abstract-full" style="display: none;"> We know that sub-leading corrections to the hawking area law is riddled with issues which have some convergent and divergent aspects. Depending on the theory, scheme, model or even method sub-leading terms turn out to have trivial and non- trivial aspects which we are going to dwell upon. The generic character of the first sub leading logarithmic term comes out unanimously the same from all theories of quantum gravity like Strings, Loops, or even semi-classical methods with the exception that sometimes the pre-factor of logarithmic term turns out to be model dependent parameter or number hence consensus on this issue is yet to be finalized. In this paper we will try to compare and contrast how we get the corrections in various theories of quantum gravity including semi-classical methods on the variant of Black Hole that is BTZ Black Hole. Towards the end we see how the addition of chern-simon terms affects the entropy of black holes and we will make brief observations regarding the same. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1207.1317v1-abstract-full').style.display = 'none'; document.getElementById('1207.1317v1-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 July, 2012; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2012. </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">This is an updated version of paper sent to conference proceedings ICGC Goa December 2011</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1112.5048">arXiv:1112.5048</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1112.5048">pdf</a>, <a href="https://arxiv.org/ps/1112.5048">ps</a>, <a href="https://arxiv.org/format/1112.5048">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="General Physics">physics.gen-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Theory">nucl-th</span> </div> </div> <p class="title is-5 mathjax"> On The Structure of A=3 Nuclei </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Abbas%2C+S+A">Syed Afsar Abbas</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeb Ahmad</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="1112.5048v1-abstract-short" style="display: inline;"> The hole in the charge distribution of $^3{\text He}$ is a major problem in A=3 nuclei. The canonical wavefucntion of A=3 nuclei which does well for electromagnetic properties of A=3 nuclei fails to produce the hole in A=3 nuclei. The hole is normally assumed to arise from explicit quark degree of freedom. Very often quark degrees of freedom are imposed to propose a different short range part of t&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1112.5048v1-abstract-full').style.display = 'inline'; document.getElementById('1112.5048v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1112.5048v1-abstract-full" style="display: none;"> The hole in the charge distribution of $^3{\text He}$ is a major problem in A=3 nuclei. The canonical wavefucntion of A=3 nuclei which does well for electromagnetic properties of A=3 nuclei fails to produce the hole in A=3 nuclei. The hole is normally assumed to arise from explicit quark degree of freedom. Very often quark degrees of freedom are imposed to propose a different short range part of the wavefunction for A=3 to explain the hole in $^3{\text He}$. So an hybrid model with nucleonic degree of freedom in outer part and quark degrees of freedom in the inner part of the nucleus have been invoked to understand the above problem. Here we present a different picture with a new wavefunction working at short range within nucleonic degrees of freedom itself. So the above problem is explained here based entirely on the nucleonic degree of freedom only. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1112.5048v1-abstract-full').style.display = 'none'; document.getElementById('1112.5048v1-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 December, 2011; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2011. </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">3 pages, 1 figure</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1103.4524">arXiv:1103.4524</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1103.4524">pdf</a>, <a href="https://arxiv.org/ps/1103.4524">ps</a>, <a href="https://arxiv.org/format/1103.4524">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="General Physics">physics.gen-ph</span> </div> </div> <p class="title is-5 mathjax"> On the New Puzzling Results from MiniBooNE </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Abbas%2C+S+A">Syed Afsar Abbas</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shakeb Ahmad</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="1103.4524v1-abstract-short" style="display: inline;"> We look into the recent puzzlng results from MiniBooNE and contrast their results with that from NOMAD. A pictuire which provides consistent decscriptiobn of both is discussed here. This also points to future directions in neutrino studies. </span> <span class="abstract-full has-text-grey-dark mathjax" id="1103.4524v1-abstract-full" style="display: none;"> We look into the recent puzzlng results from MiniBooNE and contrast their results with that from NOMAD. A pictuire which provides consistent decscriptiobn of both is discussed here. This also points to future directions in neutrino studies. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1103.4524v1-abstract-full').style.display = 'none'; document.getElementById('1103.4524v1-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 March, 2011; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2011. </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">2 pages including one figure</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1006.4454">arXiv:1006.4454</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1006.4454">pdf</a>, <a href="https://arxiv.org/format/1006.4454">other</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> <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"> A bright point source of ultrashort hard x-rays from laser bioplasmas </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Krishnamurthy%2C+M">M. Krishnamurthy</a>, <a href="/search/physics?searchtype=author&amp;query=Mondal%2C+S">Sudipta Mondal</a>, <a href="/search/physics?searchtype=author&amp;query=Lad%2C+A+D">Amit D. Lad</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Saima Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Narayanan%2C+V">V. Narayanan</a>, <a href="/search/physics?searchtype=author&amp;query=Rajeev%2C+R">R. Rajeev</a>, <a href="/search/physics?searchtype=author&amp;query=Kundu%2C+M">M. Kundu</a>, <a href="/search/physics?searchtype=author&amp;query=Kumar%2C+G+R">G. Ravindra Kumar</a>, <a href="/search/physics?searchtype=author&amp;query=Ray%2C+K">Krishanu Ray</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="1006.4454v2-abstract-short" style="display: inline;"> Micro and nano structures scatter light and amplify local electric fields very effectively. Energy incident as intense ultrashort laser pulses can be converted to x-rays and hot electrons more efficiently with a substrate that suitably modifies the local fields. Here we demonstrate that coating a plain glass surface with a few micron thick layer of an ubiquitous microbe, {\it Escherichia coli}, ca&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1006.4454v2-abstract-full').style.display = 'inline'; document.getElementById('1006.4454v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1006.4454v2-abstract-full" style="display: none;"> Micro and nano structures scatter light and amplify local electric fields very effectively. Energy incident as intense ultrashort laser pulses can be converted to x-rays and hot electrons more efficiently with a substrate that suitably modifies the local fields. Here we demonstrate that coating a plain glass surface with a few micron thick layer of an ubiquitous microbe, {\it Escherichia coli}, catapults the brightness of hard x-ray bremsstrahlung emission (up to 300 keV) by more than two orders of magnitude at an incident laser intensity of 10$^{16}$ W cm$^{-2}$. This increased yield is attributed to the local enhancement of electric fields around individual {\it E. coli} cells and is reproduced by detailed particle-in-cell (PIC) simulations. This combination of laser plasmas and biological targets can lead to turnkey, multi-kilohertz and environmentally safe sources of hard x-rays. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1006.4454v2-abstract-full').style.display = 'none'; document.getElementById('1006.4454v2-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 June, 2010; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 23 June, 2010; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 2010. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1005.5096">arXiv:1005.5096</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1005.5096">pdf</a>, <a href="https://arxiv.org/ps/1005.5096">ps</a>, <a href="https://arxiv.org/format/1005.5096">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Statistical Mechanics">cond-mat.stat-mech</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Fluid Dynamics">physics.flu-dyn</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/PhysRevE.82.040107">10.1103/PhysRevE.82.040107 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Kinetics of Phase Separation in Fluids: A Molecular Dynamics Study </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+S">Shaista Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Das%2C+S+K">Subir K. Das</a>, <a href="/search/physics?searchtype=author&amp;query=Puri%2C+S">Sanjay Puri</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="1005.5096v1-abstract-short" style="display: inline;"> We present results from extensive 3-d molecular dynamics (MD) simulations of phase separation kinetics in fluids. A coarse-graining procedure is used to obtain state-of-the-art MD results. We observe an extended period of temporally linear growth in the viscous hydrodynamic regime. The morphological similarity of coarsening in fluids and solids is also quantified. The velocity field is characteriz&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1005.5096v1-abstract-full').style.display = 'inline'; document.getElementById('1005.5096v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1005.5096v1-abstract-full" style="display: none;"> We present results from extensive 3-d molecular dynamics (MD) simulations of phase separation kinetics in fluids. A coarse-graining procedure is used to obtain state-of-the-art MD results. We observe an extended period of temporally linear growth in the viscous hydrodynamic regime. The morphological similarity of coarsening in fluids and solids is also quantified. The velocity field is characterized by the presence of monopole-like defects, which yield a generalized Porod tail in the corresponding structure factor. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1005.5096v1-abstract-full').style.display = 'none'; document.getElementById('1005.5096v1-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 May, 2010; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2010. </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">4 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/0901.2039">arXiv:0901.2039</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/0901.2039">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Biological Physics">physics.bio-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/10.1186/1757-5036-1-3">10.1186/1757-5036-1-3 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> ATR-FTIR spectroscopy detects alterations induced by organotin(IV) carboxylates in MCF-7 cells at sub-cytotoxic/-genotoxic concentrations </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+M+S">Muhammad S Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Mirza%2C+B">Bushra Mirza</a>, <a href="/search/physics?searchtype=author&amp;query=Hussain%2C+M">Mukhtiar Hussain</a>, <a href="/search/physics?searchtype=author&amp;query=Hanif%2C+M">Muhammad Hanif</a>, <a href="/search/physics?searchtype=author&amp;query=Ali%2C+S">Saqib Ali</a>, <a href="/search/physics?searchtype=author&amp;query=Walsh%2C+M+J">Michael J Walsh</a>, <a href="/search/physics?searchtype=author&amp;query=Martin%2C+F+L">Francis L Martin</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="0901.2039v1-abstract-short" style="display: inline;"> The environmental impact of metal complexes such as organotin(IV) compounds is of increasing concern. Genotoxic effects of organotin(IV) compounds (0.01 microg/ml, 0.1 microg/ml or 1.0 microg/ml) were measured using the alkaline single-cell gel electrophoresis (comet) assay to measure DNA single-strand breaks (SSBs) and the cytokinesis-block micronucleus (CBMN) assay to determine micronucleus fo&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('0901.2039v1-abstract-full').style.display = 'inline'; document.getElementById('0901.2039v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="0901.2039v1-abstract-full" style="display: none;"> The environmental impact of metal complexes such as organotin(IV) compounds is of increasing concern. Genotoxic effects of organotin(IV) compounds (0.01 microg/ml, 0.1 microg/ml or 1.0 microg/ml) were measured using the alkaline single-cell gel electrophoresis (comet) assay to measure DNA single-strand breaks (SSBs) and the cytokinesis-block micronucleus (CBMN) assay to determine micronucleus formation. Biochemical-cell signatures were also ascertained using attenuated total reflection Fourier-transform infrared (ATR-FTIR) spectroscopy. In the comet assay, organotin(IV) carboxylates induced significantly-elevated levels of DNA SSBs. Elevated micronucleus-forming activities were also observed. Following interrogation using ATR-FTIR spectroscopy, infrared spectra in the biomolecular range (900 cm-1 - 1800 cm-1) derived from orga... <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('0901.2039v1-abstract-full').style.display = 'none'; document.getElementById('0901.2039v1-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 January, 2009; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2009. </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">19 pages, 7 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> PMC Biophysics 2008, 1:3 </p> </li> </ol> <div class="is-hidden-tablet"> <!-- feedback for mobile only --> 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