000217933 001__ 217933
000217933 005__ 20230317222557.0
000217933 037__ $$aGSI-2019-00053
000217933 041__ $$aEnglish
000217933 1001_ $$0P:(DE-HGF)0$$aDzhygadlo, Roman$$b0$$eCorresponding author
000217933 1112_ $$a2018 IEEE Nuclear Science Symposium and Medical Imaging Conference$$cSydney$$d2018-11-10 - 2018-11-17$$wAustralia
000217933 245__ $$aThe PANDA Barrel DIRC Detector at FAIR
000217933 260__ $$c2018
000217933 3367_ $$033$$2EndNote$$aConference Paper
000217933 3367_ $$2DataCite$$aOther
000217933 3367_ $$2BibTeX$$aINPROCEEDINGS
000217933 3367_ $$2DRIVER$$aconferenceObject
000217933 3367_ $$2ORCID$$aLECTURE_SPEECH
000217933 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1547025860_9159$$xOther
000217933 520__ $$aThe PANDA experiment at the international accelerator Facility for Antiproton andIon Research in Europe (FAIR) near GSI, Darmstadt, Germany will address fundamentalquestions of hadron physics. Excellent Particle Identification (PID) over a largerange of solid angles and particle momenta will be essential to meet the objectivesof the rich physics program. Charged PID for the barrel region of the PANDA targetspectrometer will be provided by a DIRC (Detection of Internally Reflected Cherenkov light) detector.The PANDA Barrel DIRC is designed to cover the polar angle range of 22-140 degreesand separate charged pions from kaons for momenta between 0.5 GeV/c and 3.5 GeV/cwith a separation power of at least 3 standard deviations. The design is based onthe successful BABAR DIRC and the SuperB FDIRC R&D with several importantimprovements to optimize the performance for PANDA, such as a focusing lens system,fast timing, a compact fused silica prism as expansion region, and lifetime-enhanced Microchannel-Plate PMTs for photon detection.Detailed Monte-Carlo simulations were performed and two reconstruction methodwere developed to study the performance of the design.We will discuss the baseline design of the PANDA Barrel DIRC, based on narrow barsmade of synthetic fused silica and a complex multi-layer spherical lens system andpresent the result of tests of a large system prototype with a mixed hadron beam at CERN.
000217933 536__ $$0G:(DE-HGF)POF3-612$$a612 - Cosmic Matter in the Laboratory (POF3-612)$$cPOF3-612$$fPOF III$$x0
000217933 909CO $$ooai:repository.gsi.de:217933$$pVDB
000217933 9101_ $$0I:(DE-Ds200)20121206GSI$$6P:(DE-HGF)0$$aGSI Helmholtzzentrum für Schwerionenforschung GmbH$$b0$$kGSI
000217933 9131_ $$0G:(DE-HGF)POF3-612$$1G:(DE-HGF)POF3-610$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Universum$$vCosmic Matter in the Laboratory$$x0
000217933 9132_ $$0G:(DE-HGF)POF4-612$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vCosmic Matter in the Laboratory$$x0
000217933 9141_ $$y2018
000217933 920__ $$lyes
000217933 9201_ $$0I:(DE-Ds200)HPD-20121002OR242$$kHPD$$lPANDA Detektoren$$x0
000217933 9201_ $$0I:(DE-Ds200)HSP-20080821OR101$$kHSP$$lHadronenspektroskopie$$x1
000217933 980__ $$aconf
000217933 980__ $$aVDB
000217933 980__ $$aI:(DE-Ds200)20121002OR242
000217933 980__ $$aI:(DE-Ds200)HPD-20121002OR242
000217933 980__ $$aI:(DE-Ds200)20110830OR101
000217933 980__ $$aI:(DE-Ds200)HSP-20080821OR101
000217933 980__ $$aUNRESTRICTED