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name="order"><option selected value="-announced_date_first">Announcement date (newest first)</option><option value="announced_date_first">Announcement date (oldest first)</option><option value="-submitted_date">Submission date (newest first)</option><option value="submitted_date">Submission date (oldest first)</option><option value="">Relevance</option></select> </span> </div> <div class="control"> <button class="button is-small is-link">Go</button> </div> </div> </form> </div> </div> <ol class="breathe-horizontal" start="1"> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.02966">arXiv:2411.02966</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.02966">pdf</a>, <a href="https://arxiv.org/format/2411.02966">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Accelerator Physics">physics.acc-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/10.5281/zenodo.13970100">10.5281/zenodo.13970100 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> MuCol Milestone Report No. 5: Preliminary Parameters </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Accettura%2C+C">Carlotta Accettura</a>, <a href="/search/physics?searchtype=author&amp;query=Adrian%2C+S">Simon Adrian</a>, <a href="/search/physics?searchtype=author&amp;query=Agarwal%2C+R">Rohit Agarwal</a>, <a href="/search/physics?searchtype=author&amp;query=Ahdida%2C+C">Claudia Ahdida</a>, <a href="/search/physics?searchtype=author&amp;query=Aim%C3%A9%2C+C">Chiara Aim茅</a>, <a href="/search/physics?searchtype=author&amp;query=Aksoy%2C+A">Avni Aksoy</a>, <a href="/search/physics?searchtype=author&amp;query=Alberghi%2C+G+L">Gian Luigi Alberghi</a>, <a href="/search/physics?searchtype=author&amp;query=Alden%2C+S">Siobhan Alden</a>, <a href="/search/physics?searchtype=author&amp;query=Alfonso%2C+L">Luca Alfonso</a>, <a href="/search/physics?searchtype=author&amp;query=Amapane%2C+N">Nicola Amapane</a>, <a href="/search/physics?searchtype=author&amp;query=Amorim%2C+D">David Amorim</a>, <a href="/search/physics?searchtype=author&amp;query=Andreetto%2C+P">Paolo Andreetto</a>, <a href="/search/physics?searchtype=author&amp;query=Anulli%2C+F">Fabio Anulli</a>, <a href="/search/physics?searchtype=author&amp;query=Appleby%2C+R">Rob Appleby</a>, <a href="/search/physics?searchtype=author&amp;query=Apresyan%2C+A">Artur Apresyan</a>, <a href="/search/physics?searchtype=author&amp;query=Asadi%2C+P">Pouya Asadi</a>, <a href="/search/physics?searchtype=author&amp;query=Mahmoud%2C+M+A">Mohammed Attia Mahmoud</a>, <a href="/search/physics?searchtype=author&amp;query=Auchmann%2C+B">Bernhard Auchmann</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+J">John Back</a>, <a href="/search/physics?searchtype=author&amp;query=Badea%2C+A">Anthony Badea</a>, <a href="/search/physics?searchtype=author&amp;query=Bae%2C+K+J">Kyu Jung Bae</a>, <a href="/search/physics?searchtype=author&amp;query=Bahng%2C+E+J">E. J. Bahng</a>, <a href="/search/physics?searchtype=author&amp;query=Balconi%2C+L">Lorenzo Balconi</a>, <a href="/search/physics?searchtype=author&amp;query=Balli%2C+F">Fabrice Balli</a>, <a href="/search/physics?searchtype=author&amp;query=Bandiera%2C+L">Laura Bandiera</a> , et al. (369 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2411.02966v1-abstract-short" style="display: inline;"> This document is comprised of a collection of updated preliminary parameters for the key parts of the muon collider. The updated preliminary parameters follow on from the October 2023 Tentative Parameters Report. Particular attention has been given to regions of the facility that are believed to hold greater technical uncertainty in their design and that have a strong impact on the cost and power&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.02966v1-abstract-full').style.display = 'inline'; document.getElementById('2411.02966v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.02966v1-abstract-full" style="display: none;"> This document is comprised of a collection of updated preliminary parameters for the key parts of the muon collider. The updated preliminary parameters follow on from the October 2023 Tentative Parameters Report. Particular attention has been given to regions of the facility that are believed to hold greater technical uncertainty in their design and that have a strong impact on the cost and power consumption of the facility. The data is collected from a collaborative spreadsheet and transferred to overleaf. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.02966v1-abstract-full').style.display = 'none'; document.getElementById('2411.02966v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2407.12450">arXiv:2407.12450</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2407.12450">pdf</a>, <a href="https://arxiv.org/format/2407.12450">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Accelerator Physics">physics.acc-ph</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"> Interim report for the International Muon Collider Collaboration (IMCC) </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Accettura%2C+C">C. Accettura</a>, <a href="/search/physics?searchtype=author&amp;query=Adrian%2C+S">S. Adrian</a>, <a href="/search/physics?searchtype=author&amp;query=Agarwal%2C+R">R. Agarwal</a>, <a href="/search/physics?searchtype=author&amp;query=Ahdida%2C+C">C. Ahdida</a>, <a href="/search/physics?searchtype=author&amp;query=Aim%C3%A9%2C+C">C. Aim茅</a>, <a href="/search/physics?searchtype=author&amp;query=Aksoy%2C+A">A. Aksoy</a>, <a href="/search/physics?searchtype=author&amp;query=Alberghi%2C+G+L">G. L. Alberghi</a>, <a href="/search/physics?searchtype=author&amp;query=Alden%2C+S">S. Alden</a>, <a href="/search/physics?searchtype=author&amp;query=Amapane%2C+N">N. Amapane</a>, <a href="/search/physics?searchtype=author&amp;query=Amorim%2C+D">D. Amorim</a>, <a href="/search/physics?searchtype=author&amp;query=Andreetto%2C+P">P. Andreetto</a>, <a href="/search/physics?searchtype=author&amp;query=Anulli%2C+F">F. Anulli</a>, <a href="/search/physics?searchtype=author&amp;query=Appleby%2C+R">R. Appleby</a>, <a href="/search/physics?searchtype=author&amp;query=Apresyan%2C+A">A. Apresyan</a>, <a href="/search/physics?searchtype=author&amp;query=Asadi%2C+P">P. Asadi</a>, <a href="/search/physics?searchtype=author&amp;query=Mahmoud%2C+M+A">M. Attia Mahmoud</a>, <a href="/search/physics?searchtype=author&amp;query=Auchmann%2C+B">B. Auchmann</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+J">J. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Badea%2C+A">A. Badea</a>, <a href="/search/physics?searchtype=author&amp;query=Bae%2C+K+J">K. J. Bae</a>, <a href="/search/physics?searchtype=author&amp;query=Bahng%2C+E+J">E. J. Bahng</a>, <a href="/search/physics?searchtype=author&amp;query=Balconi%2C+L">L. Balconi</a>, <a href="/search/physics?searchtype=author&amp;query=Balli%2C+F">F. Balli</a>, <a href="/search/physics?searchtype=author&amp;query=Bandiera%2C+L">L. Bandiera</a>, <a href="/search/physics?searchtype=author&amp;query=Barbagallo%2C+C">C. Barbagallo</a> , et al. (362 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="2407.12450v1-abstract-short" style="display: inline;"> The International Muon Collider Collaboration (IMCC) [1] was established in 2020 following the recommendations of the European Strategy for Particle Physics (ESPP) and the implementation of the European Strategy for Particle Physics-Accelerator R&amp;D Roadmap by the Laboratory Directors Group [2], hereinafter referred to as the the European LDG roadmap. The Muon Collider Study (MuC) covers the accele&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2407.12450v1-abstract-full').style.display = 'inline'; document.getElementById('2407.12450v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2407.12450v1-abstract-full" style="display: none;"> The International Muon Collider Collaboration (IMCC) [1] was established in 2020 following the recommendations of the European Strategy for Particle Physics (ESPP) and the implementation of the European Strategy for Particle Physics-Accelerator R&amp;D Roadmap by the Laboratory Directors Group [2], hereinafter referred to as the the European LDG roadmap. The Muon Collider Study (MuC) covers the accelerator complex, detectors and physics for a future muon collider. In 2023, European Commission support was obtained for a design study of a muon collider (MuCol) [3]. This project started on 1st March 2023, with work-packages aligned with the overall muon collider studies. In preparation of and during the 2021-22 U.S. Snowmass process, the muon collider project parameters, technical studies and physics performance studies were performed and presented in great detail. Recently, the P5 panel [4] in the U.S. recommended a muon collider R&amp;D, proposed to join the IMCC and envisages that the U.S. should prepare to host a muon collider, calling this their &#34;muon shot&#34;. In the past, the U.S. Muon Accelerator Programme (MAP) [5] has been instrumental in studies of concepts and technologies for a muon collider. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2407.12450v1-abstract-full').style.display = 'none'; document.getElementById('2407.12450v1-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 July, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">This document summarises the International Muon Collider Collaboration (IMCC) progress and status of the Muon Collider R&amp;D programme</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2111.11359">arXiv:2111.11359</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2111.11359">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Materials Science">cond-mat.mtrl-sci</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Computational Physics">physics.comp-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.diamond.2022.109072">10.1016/j.diamond.2022.109072 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Ab-initio calculation of point defect equilibria during heat treatment: Nitrogen, hydrogen, and silicon doped diamond </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Mansoor%2C+M">Mubashir Mansoor</a>, <a href="/search/physics?searchtype=author&amp;query=Mansoor%2C+M">Mehya Mansoor</a>, <a href="/search/physics?searchtype=author&amp;query=Mansoor%2C+M">Maryam Mansoor</a>, <a href="/search/physics?searchtype=author&amp;query=Aksoy%2C+A">Ammar Aksoy</a>, <a href="/search/physics?searchtype=author&amp;query=Seyhan%2C+S+N">Sinem Nergiz Seyhan</a>, <a href="/search/physics?searchtype=author&amp;query=Yildirim%2C+B">Betul Yildirim</a>, <a href="/search/physics?searchtype=author&amp;query=Tahiri%2C+A">Ahmet Tahiri</a>, <a href="/search/physics?searchtype=author&amp;query=Solak%2C+N">Nuri Solak</a>, <a href="/search/physics?searchtype=author&amp;query=Kazmanli%2C+K">Kursat Kazmanli</a>, <a href="/search/physics?searchtype=author&amp;query=Er%2C+Z">Zuhal Er</a>, <a href="/search/physics?searchtype=author&amp;query=Czelej%2C+K">Kamil Czelej</a>, <a href="/search/physics?searchtype=author&amp;query=Urgen%2C+M">Mustafa Urgen</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="2111.11359v1-abstract-short" style="display: inline;"> Point defects are responsible for a wide range of optoelectronic properties in materials, making it crucial to engineer their concentrations for novel materials design. However, considering the plethora of defects in co-doped semiconducting and dielectric materials and the dependence of defect formation energies on heat treatment parameters, process design based on an experimental trial and error&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.11359v1-abstract-full').style.display = 'inline'; document.getElementById('2111.11359v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2111.11359v1-abstract-full" style="display: none;"> Point defects are responsible for a wide range of optoelectronic properties in materials, making it crucial to engineer their concentrations for novel materials design. However, considering the plethora of defects in co-doped semiconducting and dielectric materials and the dependence of defect formation energies on heat treatment parameters, process design based on an experimental trial and error approach is not an efficient strategy. This makes it necessary to explore computational pathways for predicting defect equilibria during heat treatments. The accumulated experimental knowledge on defect transformations in diamond is unparalleled. Therefore, diamond is an excellent material for benchmarking computational approaches. By considering nitrogen, hydrogen, and silicon doped diamond as a model system, we have investigated the pressure dependence of defect formation energies and calculated the defect equilibria during heat treatment of diamond through ab-initio calculations. We have plotted monolithic-Kr枚ger-Vink diagrams for various defects, representing defect concentrations based on process parameters, such as temperature and partial pressure of gases used during heat treatments of diamond. The method demonstrated predicts the majority of experimental data, such as nitrogen aggregation path leading towards the formation of the B center, annealing of the B, H3, N3, and NVHx centers at ultra high temperatures, the thermal stability of the SiV center, and temperature dependence of NV concentration. We demonstrate the possibility of designing heat treatments for a wide range of semiconducting and dielectric materials by using a relatively inexpensive yet robust first principles approach, significantly accelerating defect engineering and high-throughput novel materials design. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.11359v1-abstract-full').style.display = 'none'; document.getElementById('2111.11359v1-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 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">Comments:</span> <span class="has-text-grey-dark mathjax">This preprint includes 17 pages, 1 cover photo, 7 figures and 2 appendices</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2107.13331">arXiv:2107.13331</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2107.13331">pdf</a>, <a href="https://arxiv.org/format/2107.13331">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Accelerator Physics">physics.acc-ph</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/10.1103/PhysRevAccelBeams.24.100701">10.1103/PhysRevAccelBeams.24.100701 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Bright 脜ngstrom and Picometre Free Electron Laser Based on the LHeC Energy Recovery Linac </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Nergiz%2C+Z">Z. Nergiz</a>, <a href="/search/physics?searchtype=author&amp;query=Mirian%2C+N+S">N. S. Mirian</a>, <a href="/search/physics?searchtype=author&amp;query=Aksoy%2C+A">A. Aksoy</a>, <a href="/search/physics?searchtype=author&amp;query=Zhou%2C+D">D. Zhou</a>, <a href="/search/physics?searchtype=author&amp;query=Zimmermann%2C+F">F. Zimmermann</a>, <a href="/search/physics?searchtype=author&amp;query=Aksakal%2C+H">H. Aksakal</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="2107.13331v2-abstract-short" style="display: inline;"> The Large Hadron electron Collider (LHeC) is a proposed future particle-physics project colliding 60 GeV electrons from a six-pass recirculating energy-recovery Linac (ERL) with 7 TeV protons stored in the LHC. The ERL technology allows for much higher beam current and, therefore, higher luminosity than a traditional Linac. The high-current, high-energy electron beam can also be used to drive a fr&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.13331v2-abstract-full').style.display = 'inline'; document.getElementById('2107.13331v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2107.13331v2-abstract-full" style="display: none;"> The Large Hadron electron Collider (LHeC) is a proposed future particle-physics project colliding 60 GeV electrons from a six-pass recirculating energy-recovery Linac (ERL) with 7 TeV protons stored in the LHC. The ERL technology allows for much higher beam current and, therefore, higher luminosity than a traditional Linac. The high-current, high-energy electron beam can also be used to drive a free electron laser (FEL). In this study, we investigate the performance of an LHeC-based FEL, operated in the self-amplified spontaneous emission mode using electron beams after one or two turns, with beam energies of, e.g., 10, 20, 30 and 40 GeV, and aim at producing X-ray pulses at wavelengths ranging from 8~脜 to 0.5~脜. In addition, we explore a possible path to use the 40 GeV electron beam for generating photon pulses at much lower wavelengths, down to a few picometre. We demonstrate that such ERL-based high-energy FEL would have the potential to provide orders of magnitude higher average brilliance at 脜 wavelengths than any other FEL either existing or proposed. It might also allow a pioneering step into the picometre wavelength regime. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.13331v2-abstract-full').style.display = 'none'; document.getElementById('2107.13331v2-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 August, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 28 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">13 pages, 13 figures, submitted to Physical Review Accelerators and Beams (PRAB)</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Accel. Beams 24, 100701 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1812.06018">arXiv:1812.06018</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1812.06018">pdf</a>, <a href="https://arxiv.org/format/1812.06018">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Accelerator Physics">physics.acc-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/10.23731/CYRM-2018-002">10.23731/CYRM-2018-002 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> The Compact Linear Collider (CLIC) - 2018 Summary Report </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=CLIC%2C+T">The CLIC</a>, <a href="/search/physics?searchtype=author&amp;query=collaborations%2C+C">CLICdp collaborations</a>, <a href="/search/physics?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/physics?searchtype=author&amp;query=Charles%2C+T+K">T. K. Charles</a>, <a href="/search/physics?searchtype=author&amp;query=Giansiracusa%2C+P+J">P. J. Giansiracusa</a>, <a href="/search/physics?searchtype=author&amp;query=Lucas%2C+T+G">T. G. Lucas</a>, <a href="/search/physics?searchtype=author&amp;query=Rassool%2C+R+P">R. P. Rassool</a>, <a href="/search/physics?searchtype=author&amp;query=Volpi%2C+M">M. Volpi</a>, <a href="/search/physics?searchtype=author&amp;query=Balazs%2C+C">C. Balazs</a>, <a href="/search/physics?searchtype=author&amp;query=Afanaciev%2C+K">K. Afanaciev</a>, <a href="/search/physics?searchtype=author&amp;query=Makarenko%2C+V">V. Makarenko</a>, <a href="/search/physics?searchtype=author&amp;query=Patapenka%2C+A">A. Patapenka</a>, <a href="/search/physics?searchtype=author&amp;query=Zhuk%2C+I">I. Zhuk</a>, <a href="/search/physics?searchtype=author&amp;query=Collette%2C+C">C. Collette</a>, <a href="/search/physics?searchtype=author&amp;query=Boland%2C+M+J">M. J. Boland</a>, <a href="/search/physics?searchtype=author&amp;query=Hoffman%2C+A+C+A">A. C. Abusleme Hoffman</a>, <a href="/search/physics?searchtype=author&amp;query=Diaz%2C+M+A">M. A. Diaz</a>, <a href="/search/physics?searchtype=author&amp;query=Garay%2C+F">F. Garay</a>, <a href="/search/physics?searchtype=author&amp;query=Chi%2C+Y">Y. Chi</a>, <a href="/search/physics?searchtype=author&amp;query=He%2C+X">X. He</a>, <a href="/search/physics?searchtype=author&amp;query=Pei%2C+G">G. Pei</a>, <a href="/search/physics?searchtype=author&amp;query=Pei%2C+S">S. Pei</a>, <a href="/search/physics?searchtype=author&amp;query=Shu%2C+G">G. Shu</a>, <a href="/search/physics?searchtype=author&amp;query=Wang%2C+X">X. Wang</a>, <a href="/search/physics?searchtype=author&amp;query=Zhang%2C+J">J. Zhang</a> , et al. (671 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="1812.06018v3-abstract-short" style="display: inline;"> The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^-$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1812.06018v3-abstract-full').style.display = 'inline'; document.getElementById('1812.06018v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1812.06018v3-abstract-full" style="display: none;"> The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^-$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively. CLIC uses a two-beam acceleration scheme, in which 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept has been refined using improved software tools. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations and parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25-30 years. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1812.06018v3-abstract-full').style.display = 'none'; document.getElementById('1812.06018v3-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 6 May, 2019; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 14 December, 2018; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2018. </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">112 pages, 59 figures; published as CERN Yellow Report Monograph Vol. 2/2018; corresponding editors: Philip N. Burrows, Nuria Catalan Lasheras, Lucie Linssen, Marko Petri膷, Aidan Robson, Daniel Schulte, Eva Sicking, Steinar Stapnes</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> CERN-2018-005-M </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1608.07537">arXiv:1608.07537</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1608.07537">pdf</a>, <a href="https://arxiv.org/format/1608.07537">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Accelerator Physics">physics.acc-ph</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/10.5170/CERN-2016-004">10.5170/CERN-2016-004 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Updated baseline for a staged Compact Linear Collider </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=CLIC%2C+T">The CLIC</a>, <a href="/search/physics?searchtype=author&amp;query=collaborations%2C+C">CLICdp collaborations</a>, <a href="/search/physics?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/physics?searchtype=author&amp;query=Boland%2C+M+J">M. J. Boland</a>, <a href="/search/physics?searchtype=author&amp;query=Felzmann%2C+U">U. Felzmann</a>, <a href="/search/physics?searchtype=author&amp;query=Giansiracusa%2C+P+J">P. J. Giansiracusa</a>, <a href="/search/physics?searchtype=author&amp;query=Lucas%2C+T+G">T. G. Lucas</a>, <a href="/search/physics?searchtype=author&amp;query=Rassool%2C+R+P">R. P. Rassool</a>, <a href="/search/physics?searchtype=author&amp;query=Balazs%2C+C">C. Balazs</a>, <a href="/search/physics?searchtype=author&amp;query=Charles%2C+T+K">T. K. Charles</a>, <a href="/search/physics?searchtype=author&amp;query=Afanaciev%2C+K">K. Afanaciev</a>, <a href="/search/physics?searchtype=author&amp;query=Emeliantchik%2C+I">I. Emeliantchik</a>, <a href="/search/physics?searchtype=author&amp;query=Ignatenko%2C+A">A. Ignatenko</a>, <a href="/search/physics?searchtype=author&amp;query=Makarenko%2C+V">V. Makarenko</a>, <a href="/search/physics?searchtype=author&amp;query=Shumeiko%2C+N">N. Shumeiko</a>, <a href="/search/physics?searchtype=author&amp;query=Patapenka%2C+A">A. Patapenka</a>, <a href="/search/physics?searchtype=author&amp;query=Zhuk%2C+I">I. Zhuk</a>, <a href="/search/physics?searchtype=author&amp;query=Hoffman%2C+A+C+A">A. C. Abusleme Hoffman</a>, <a href="/search/physics?searchtype=author&amp;query=Gutierrez%2C+M+A+D">M. A. Diaz Gutierrez</a>, <a href="/search/physics?searchtype=author&amp;query=Gonzalez%2C+M+V">M. Vogel Gonzalez</a>, <a href="/search/physics?searchtype=author&amp;query=Chi%2C+Y">Y. Chi</a>, <a href="/search/physics?searchtype=author&amp;query=He%2C+X">X. He</a>, <a href="/search/physics?searchtype=author&amp;query=Pei%2C+G">G. Pei</a>, <a href="/search/physics?searchtype=author&amp;query=Pei%2C+S">S. Pei</a>, <a href="/search/physics?searchtype=author&amp;query=Shu%2C+G">G. Shu</a> , et al. (493 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="1608.07537v3-abstract-short" style="display: inline;"> The Compact Linear Collider (CLIC) is a multi-TeV high-luminosity linear e+e- collider under development. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in a staged approach with three centre-of-mass energy stages ranging from a few hundred GeV up to 3 TeV. The first stage will focus on precision Standard Model physics, in particular Higgs and top-q&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1608.07537v3-abstract-full').style.display = 'inline'; document.getElementById('1608.07537v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1608.07537v3-abstract-full" style="display: none;"> The Compact Linear Collider (CLIC) is a multi-TeV high-luminosity linear e+e- collider under development. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in a staged approach with three centre-of-mass energy stages ranging from a few hundred GeV up to 3 TeV. The first stage will focus on precision Standard Model physics, in particular Higgs and top-quark measurements. Subsequent stages will focus on measurements of rare Higgs processes, as well as searches for new physics processes and precision measurements of new states, e.g. states previously discovered at LHC or at CLIC itself. In the 2012 CLIC Conceptual Design Report, a fully optimised 3 TeV collider was presented, while the proposed lower energy stages were not studied to the same level of detail. This report presents an updated baseline staging scenario for CLIC. The scenario is the result of a comprehensive study addressing the performance, cost and power of the CLIC accelerator complex as a function of centre-of-mass energy and it targets optimal physics output based on the current physics landscape. The optimised staging scenario foresees three main centre-of-mass energy stages at 380 GeV, 1.5 TeV and 3 TeV for a full CLIC programme spanning 22 years. For the first stage, an alternative to the CLIC drive beam scheme is presented in which the main linac power is produced using X-band klystrons. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1608.07537v3-abstract-full').style.display = 'none'; document.getElementById('1608.07537v3-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 March, 2017; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 26 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">57 pages, 27 figures, 12 tables, published as CERN Yellow Report. Updated version: Minor layout changes for print version</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> CERN-2016-004 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1409.4514">arXiv:1409.4514</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1409.4514">pdf</a>, <a href="https://arxiv.org/ps/1409.4514">ps</a>, <a href="https://arxiv.org/format/1409.4514">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Accelerator Physics">physics.acc-ph</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1674-1137/39/6/067002">10.1088/1674-1137/39/6/067002 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Low emittance lattice for the storage ring of Turkish Light Source Facility TURKAY </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Nergiz%2C+Z">Zafer Nergiz</a>, <a href="/search/physics?searchtype=author&amp;query=Aksoy%2C+A">Avni Aksoy</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="1409.4514v1-abstract-short" style="display: inline;"> Turkish Accelerator Center) project is aimed to build an accelerator center in Turkey. The first step of the project is to construct IR-FEL facility. The second stage is to build a synchrotron radiation facility named TURKAY, which is the third generation synchrotron radiation light source that aimed to achieve high brilliance photon beam from low emittance electron beam at 3 GeV. The electron bea&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1409.4514v1-abstract-full').style.display = 'inline'; document.getElementById('1409.4514v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1409.4514v1-abstract-full" style="display: none;"> Turkish Accelerator Center) project is aimed to build an accelerator center in Turkey. The first step of the project is to construct IR-FEL facility. The second stage is to build a synchrotron radiation facility named TURKAY, which is the third generation synchrotron radiation light source that aimed to achieve high brilliance photon beam from low emittance electron beam at 3 GeV. The electron beam parameters highly depend on the magnetic lattice of the storage ring. In this paper a low emittance storage ring for TURKAY is proposed and beam dynamic properties of the magnetic lattice are investigated. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1409.4514v1-abstract-full').style.display = 'none'; document.getElementById('1409.4514v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 16 September, 2014; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 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">5 pages, 5 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Chinese Physics C Vol. 39, No. 6 (2015) 067002 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1202.5628">arXiv:1202.5628</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1202.5628">pdf</a>, <a href="https://arxiv.org/ps/1202.5628">ps</a>, <a href="https://arxiv.org/format/1202.5628">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Accelerator Physics">physics.acc-ph</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"> Simulations for CLIC Drive Beam Linac </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Aksoy%2C+A">Avni Aksoy</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="1202.5628v1-abstract-short" style="display: inline;"> The Drive Beam Linac of the Compact Linear Collider (CLIC) has to accelerate an electron beam with 4.2 A up to 2.4 GeV in almost fully-loaded structures. The pulse contains about 70000 bunches, one in every second rf bucket, and has a length of 140 $渭$s. The beam stability along the beamline is of concern for such a high current and pulse length. We present different options for the lattice of the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1202.5628v1-abstract-full').style.display = 'inline'; document.getElementById('1202.5628v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1202.5628v1-abstract-full" style="display: none;"> The Drive Beam Linac of the Compact Linear Collider (CLIC) has to accelerate an electron beam with 4.2 A up to 2.4 GeV in almost fully-loaded structures. The pulse contains about 70000 bunches, one in every second rf bucket, and has a length of 140 $渭$s. The beam stability along the beamline is of concern for such a high current and pulse length. We present different options for the lattice of the linac based on FODO, triplet and doublet cells and compare the transverse instability for each lattice including the effects of beam jitter, alignment and beam-based correction. Additionally longitudinal stability is discussed for different bunch compressors using FODO type of lattice. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1202.5628v1-abstract-full').style.display = 'none'; document.getElementById('1202.5628v1-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 February, 2012; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 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">11 pages, 10 figures. This work has been represented at Iternational Workshop on Future Linear Colliders 2011 (LCWS11)</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/0911.2336">arXiv:0911.2336</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/0911.2336">pdf</a>, <a href="https://arxiv.org/format/0911.2336">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Accelerator Physics">physics.acc-ph</span> </div> </div> <p class="title is-5 mathjax"> The TAC IR FEL Oscillator Facility Project </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Ketenoglu%2C+B">B. Ketenoglu</a>, <a href="/search/physics?searchtype=author&amp;query=Aksoy%2C+A">A. Aksoy</a>, <a href="/search/physics?searchtype=author&amp;query=Yavas%2C+O">O. Yavas</a>, <a href="/search/physics?searchtype=author&amp;query=Tural%2C+M">M. Tural</a>, <a href="/search/physics?searchtype=author&amp;query=Karsli%2C+O">O. Karsli</a>, <a href="/search/physics?searchtype=author&amp;query=Ozkorucuklu%2C+S">S. Ozkorucuklu</a>, <a href="/search/physics?searchtype=author&amp;query=Arikan%2C+P">P. Arikan</a>, <a href="/search/physics?searchtype=author&amp;query=Kasap%2C+E">E. Kasap</a>, <a href="/search/physics?searchtype=author&amp;query=Yildiz%2C+H">H. Yildiz</a>, <a href="/search/physics?searchtype=author&amp;query=Bilen%2C+B">B. Bilen</a>, <a href="/search/physics?searchtype=author&amp;query=Aksakal%2C+H">H. Aksakal</a>, <a href="/search/physics?searchtype=author&amp;query=Tapan%2C+I">I. Tapan</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="0911.2336v1-abstract-short" style="display: inline;"> The TAC (Turkish Accelerator Center) IR FEL Oscillator facility, which has been supported by Turkish State Planning Organization (SPO) since 2006, will be based on a 15-40 MeV electron linac accompanying two different undulators with 2.5 cm and 9 cm periods in order to obtain IR FEL ranging between 2-250 microns. The electron linac will consist of two sequenced modules, each housing two 9-cell s&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('0911.2336v1-abstract-full').style.display = 'inline'; document.getElementById('0911.2336v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="0911.2336v1-abstract-full" style="display: none;"> The TAC (Turkish Accelerator Center) IR FEL Oscillator facility, which has been supported by Turkish State Planning Organization (SPO) since 2006, will be based on a 15-40 MeV electron linac accompanying two different undulators with 2.5 cm and 9 cm periods in order to obtain IR FEL ranging between 2-250 microns. The electron linac will consist of two sequenced modules, each housing two 9-cell superconducting TESLA cavities for cw operation. It is planned that the TAC IR FEL facility will be completed in 2012 at Golbasi campus of Ankara University. This facility will give an opportunity to the scientists and industry to use FEL in research and development in Turkey and our region. In this study, the results of optimization studies and present plans about construction process of the facility are presented. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('0911.2336v1-abstract-full').style.display = 'none'; document.getElementById('0911.2336v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 12 November, 2009; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 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">3 pages, 11 figures, FEL09 Conference, August 23-28, 2009, Liverpool, UK</span> </p> </li> </ol> <div class="is-hidden-tablet"> <!-- feedback for mobile only --> <span class="help" style="display: inline-block;"><a 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