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<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"> Performances of a new generation tracking detector: the MEG II cylindrical drfit chamber </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+A+M">A. M. Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Benmansour%2C+H">H. Benmansour</a>, <a href="/search/physics?searchtype=author&amp;query=Boca%2C+G">G. Boca</a>, <a href="/search/physics?searchtype=author&amp;query=Cavoto%2C+G">G. Cavoto</a>, <a href="/search/physics?searchtype=author&amp;query=Cei%2C+F">F. Cei</a>, <a href="/search/physics?searchtype=author&amp;query=Chiappini%2C+M">M. Chiappini</a>, <a href="/search/physics?searchtype=author&amp;query=Chiarello%2C+G">G. Chiarello</a>, <a href="/search/physics?searchtype=author&amp;query=Corvaglia%2C+A">A. Corvaglia</a>, <a href="/search/physics?searchtype=author&amp;query=Cuna%2C+F">F. Cuna</a>, <a href="/search/physics?searchtype=author&amp;query=Francesconi%2C+M">M. Francesconi</a>, <a href="/search/physics?searchtype=author&amp;query=Galli%2C+L">L. Galli</a>, <a href="/search/physics?searchtype=author&amp;query=Grancagnolo%2C+F">F. Grancagnolo</a>, <a href="/search/physics?searchtype=author&amp;query=Grandoni%2C+E+G">E. G. Grandoni</a>, <a href="/search/physics?searchtype=author&amp;query=Grassi%2C+M">M. Grassi</a>, <a href="/search/physics?searchtype=author&amp;query=Hildebrandt%2C+M">M. Hildebrandt</a>, <a href="/search/physics?searchtype=author&amp;query=Ignatov%2C+F">F. Ignatov</a>, <a href="/search/physics?searchtype=author&amp;query=Meucci%2C+M">M. Meucci</a>, <a href="/search/physics?searchtype=author&amp;query=Molzon%2C+W">W. Molzon</a>, <a href="/search/physics?searchtype=author&amp;query=Nicolo%27%2C+D">D. Nicolo&#39;</a>, <a href="/search/physics?searchtype=author&amp;query=Oya%2C+A">A. Oya</a>, <a href="/search/physics?searchtype=author&amp;query=Palo%2C+D">D. Palo</a>, <a href="/search/physics?searchtype=author&amp;query=Panareo%2C+M">M. Panareo</a>, <a href="/search/physics?searchtype=author&amp;query=Papa%2C+A">A. Papa</a>, <a href="/search/physics?searchtype=author&amp;query=Raffaelli%2C+F">F. Raffaelli</a>, <a href="/search/physics?searchtype=author&amp;query=Renga%2C+F">F. Renga</a> , et al. (6 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="2310.12865v2-abstract-short" style="display: inline;"> The cylindrical drift chamber is the most innovative part of the MEG~II detector, the upgraded version of the MEG experiment. The MEG~II chamber differs from the MEG one because it is a single volume cylindrical structure, instead of a segmented one, chosen to improve its resolutions and efficiency in detecting low energy positrons from muon decays at rest. In this paper, we show the characteristi&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2310.12865v2-abstract-full').style.display = 'inline'; document.getElementById('2310.12865v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2310.12865v2-abstract-full" style="display: none;"> The cylindrical drift chamber is the most innovative part of the MEG~II detector, the upgraded version of the MEG experiment. The MEG~II chamber differs from the MEG one because it is a single volume cylindrical structure, instead of a segmented one, chosen to improve its resolutions and efficiency in detecting low energy positrons from muon decays at rest. In this paper, we show the characteristics and performances of this fundamental part of the MEG~II apparatus and we discuss the impact of its higher resolution and efficiency on the sensitivity of the MEG~II experiment. Because of its innovative structure and high quality resolution and efficiency the MEG~II cylindrical drift chamber will be a cornerstone in the development of an ideal tracking detector for future positron-electron collider machines. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2310.12865v2-abstract-full').style.display = 'none'; document.getElementById('2310.12865v2-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 May, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 19 October, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 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">27 pages, 42 figures, published on EPJC 84(2024)5,473</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2207.10990">arXiv:2207.10990</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2207.10990">pdf</a>, <a href="https://arxiv.org/format/2207.10990">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 measuring systems of the wire tension for the MEG II Drift Chamber by means of the resonant frequency technique </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Baldini%2C+A+M">A. M. Baldini</a>, <a href="/search/physics?searchtype=author&amp;query=Benmansour%2C+H">H. Benmansour</a>, <a href="/search/physics?searchtype=author&amp;query=Cavoto%2C+G">G. Cavoto</a>, <a href="/search/physics?searchtype=author&amp;query=Cei%2C+F">F. Cei</a>, <a href="/search/physics?searchtype=author&amp;query=Chiappini%2C+M">M. Chiappini</a>, <a href="/search/physics?searchtype=author&amp;query=Chiarello%2C+G">G. Chiarello</a>, <a href="/search/physics?searchtype=author&amp;query=Chiri%2C+C">C. Chiri</a>, <a href="/search/physics?searchtype=author&amp;query=Cocciolo%2C+G">G. Cocciolo</a>, <a href="/search/physics?searchtype=author&amp;query=Corvaglia%2C+A">A. Corvaglia</a>, <a href="/search/physics?searchtype=author&amp;query=Cuna%2C+F">F. Cuna</a>, <a href="/search/physics?searchtype=author&amp;query=Francesconi%2C+M">M. Francesconi</a>, <a href="/search/physics?searchtype=author&amp;query=Galli%2C+L">L. Galli</a>, <a href="/search/physics?searchtype=author&amp;query=Grancagnolo%2C+F">F. Grancagnolo</a>, <a href="/search/physics?searchtype=author&amp;query=Grassi%2C+M">M. Grassi</a>, <a href="/search/physics?searchtype=author&amp;query=Meucci%2C+M">M. Meucci</a>, <a href="/search/physics?searchtype=author&amp;query=Miccoli%2C+A">A. Miccoli</a>, <a href="/search/physics?searchtype=author&amp;query=Nicolo%27%2C+D">D. Nicolo&#39;</a>, <a href="/search/physics?searchtype=author&amp;query=Panareo%2C+M">M. Panareo</a>, <a href="/search/physics?searchtype=author&amp;query=Papa%2C+A">A. Papa</a>, <a href="/search/physics?searchtype=author&amp;query=Pinto%2C+C">C. Pinto</a>, <a href="/search/physics?searchtype=author&amp;query=Raffaelli%2C+F">F. Raffaelli</a>, <a href="/search/physics?searchtype=author&amp;query=Renga%2C+F">F. Renga</a>, <a href="/search/physics?searchtype=author&amp;query=Signorelli%2C+G">G. Signorelli</a>, <a href="/search/physics?searchtype=author&amp;query=Tassielli%2C+G+F">G. F. Tassielli</a>, <a href="/search/physics?searchtype=author&amp;query=Venturini%2C+A">A. Venturini</a> , et al. (2 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="2207.10990v2-abstract-short" style="display: inline;"> The ultra-low mass cylindrical drift chamber designed for the MEG II experiment is a challenging apparatus made of 1728 phi = 20 micron gold plated tungsten sense wires, 7680 phi = 40 micron and 2496 phi = 50 micron silver plated aluminum field wires. Because of electrostatic stability requirements all the wires have to be stretched at mechanical tensions of about 25, 19 and 29 g respectively whic&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2207.10990v2-abstract-full').style.display = 'inline'; document.getElementById('2207.10990v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2207.10990v2-abstract-full" style="display: none;"> The ultra-low mass cylindrical drift chamber designed for the MEG II experiment is a challenging apparatus made of 1728 phi = 20 micron gold plated tungsten sense wires, 7680 phi = 40 micron and 2496 phi = 50 micron silver plated aluminum field wires. Because of electrostatic stability requirements all the wires have to be stretched at mechanical tensions of about 25, 19 and 29 g respectively which must be controlled at a level better than 0.5 g. This chamber is presently in acquisition, but during its construction about 100 field wires broke, because of chemical corrosion induced by the atmospheric humidity. On the basis of the experience gained with this chamber we decided to build a new one, equipped with a different type of wires less sensitive to corrosion. The choice of the new wire required a deep inspection of its characteristics and one of the main tools for doing this is a system for measuring the wire tension by means of the resonant frequency technique, which is described in this paper. The system forces the wires to oscillate by applying a sinusoidal signal at a known frequency, and then measures the variation of the capacitance between a wire and a common ground plane as a function of the external signal frequency. We present the details of the measuring system and the results obtained by scanning the mechanical tensions of two samples of MEG II cylindrical drift chamber wires and discuss the possible improvements of the experimental apparatus and of the measuring technique. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2207.10990v2-abstract-full').style.display = 'none'; document.getElementById('2207.10990v2-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 October, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 22 July, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 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">Nineteen pages, thirteen figures, published on Nuclear Instruments and Methods A</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 1045 (2023) 167534 </p> </li> </ol> <div class="is-hidden-tablet"> <!-- feedback for mobile only --> <span class="help" style="display: inline-block;"><a href="https://github.com/arXiv/arxiv-search/releases">Search v0.5.6 released 2020-02-24</a>&nbsp;&nbsp;</span> </div> </div> </main> <footer> <div class="columns is-desktop" role="navigation" aria-label="Secondary"> <!-- MetaColumn 1 --> <div class="column"> <div class="columns"> <div class="column"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/about">About</a></li> <li><a href="https://info.arxiv.org/help">Help</a></li> </ul> </div> <div class="column"> <ul class="nav-spaced"> <li> <svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 512 512" class="icon filter-black" role="presentation"><title>contact 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