Barrel time-of-flight detector for the PANDA experiment at FAIR
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The barrel time-of-flight detector for the PANDA experiment at FAIR is foreseen as a Scintillator Tile (SciTil) Hodoscope based on several thousand small plastic scintillator tiles read-out with directly attached Silicon Photomultipliers (SiPMs). The main tasks of the system are an accurate determination of the time origin of particle tracks to avoid event mixing at high collision rates, relative time-of-flight measurements as well as particle identification in the low momentum regime. The main requirements are the use of a minimum material amount and a time resolution of <span id="mmlsi0002" class="mathmlsrc">source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0168900215013479&_mathId=si0002.gif&_user=111111111&_pii=S0168900215013479&_rdoc=1&_issn=01689002&md5=6c01707ecda0b19eafdf150c5e08b623">ss="imgLazyJSB inlineImage" height="13" width="66" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0168900215013479-si0002.gif">script>border="0" style="vertical-align:bottom" width="66" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S0168900215013479-si0002.gif">script><span class="mathContainer hidden"><span class="mathCode">si0002.gif" overflow="scroll">σ<100space width="0.25em">space>psspan>span>span>. We have performed extensive optimization studies and prototype tests to prove the feasibility of the SciTil design and finalize the R&D phase. In a 2.7 GeV/c proton beam at Forschungszentrum Jülich a time resolution of about 80 ps has been achieved using SiPMs from KETEK and Hamamatsu with an active area of <span id="mmlsi0003" class="mathmlsrc">source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0168900215013479&_mathId=si0003.gif&_user=111111111&_pii=S0168900215013479&_rdoc=1&_issn=01689002&md5=d333ae58b700f889e5e27e235fd1786c">ss="imgLazyJSB inlineImage" height="12" width="66" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0168900215013479-si0003.gif">script>border="0" style="vertical-align:bottom" width="66" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S0168900215013479-si0003.gif">script><span class="mathContainer hidden"><span class="mathCode">si0003.gif" overflow="scroll">3&times;3space width="0.25em">space>sup>mm2sup>span>span>span>. Employing the Digital Photon Counter from Philips a time resolution of about 30 ps has been reached.

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