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COMPASS experiment

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331:, which all originate from the Super Proton Synchrotron. The primary proton beam (400 GeV/c and up to 1.5E13 protons per super cycle) is steered on a beryllium production target producing secondary hadrons, mainly consisting of (anti-) protons, pions and kaons. The production target and the experiment are separated by a 1.1 km long transfer line, allowing through weak decay and use of massive hadron absorbers the production of a naturally spin-polarised muon beam. The beam line is designed to transport beams up to a momentum of 280 GeV/c. Usually, five different beams are used by COMPASS: 418:, most of the final states and the scattered particles are created along the beam axis. This leads to the distinctive set-up of a fixed-target experiment: most detectors are placed behind the target ("forward spectrometer"). For some processes it is necessary to detect the recoil nucleon from the target. Here, a recoil proton detector consisting of two barrels of scintillator material is used. The protons are identified by the time of flight and the energy loss. 1155: 312: 272: 225: 26: 426:
The COMPASS experiment consists of two spectrometer stages with various tracking detector types, each set-up around a spectrometer magnet to determine the momentum of the particles. The first stage is dedicated to tracks with large scattering (production) angles and the second one for small angles.
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The timing and the position of the incident particles are determined with cold silicon strip detectors and scintillating fibre detectors. These informations are crucial to determine the interaction point inside the target material. Depending on the beam type, modifications in the beam telescope are
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physics, the spins of the target material need to be oriented in one direction. The target cell contains either ammonium or deuterium, which are polarised by the means of microwave radiation and strong magnetic fields. To keep up the polarisation grade, a He/He
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The COMPASS experiment was proposed in 1996 and approved by the CERN research committee. Between 1999 and 2001, the experiment was set up and finally in 2001, the first commissioning run was performed. Until the start of the
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physics, mostly liquid hydrogen is used, allowing to study the proton properties. For other physics, where high atomic numbers are needed, nickel, lead and other nuclear targets are used.
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with numerous tracking detectors, particle identification and calorimetry. The physics results are extracted by recording and analysing the final states of the scattering processes.
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The versatile set-up, the use of different targets and particle beams allow the investigation of various processes. The main physics goals are the investigation of the
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experiments, COMPASS was the largest data-taking experiment at CERN. It is also a pioneer in adopting new detector and readout technologies, such as
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is used to cool down the target material to 50 mK. The target material can be polarised longitudinal or transverse to the beam axis.
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The experiment consists of three major parts: the beam telescope, the target area and the two-staged spectrometer.
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detectors and most recently THGEM photon detection. The data taking is divided into the COMPASS I and II phases.
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beams with a nominal momentum of 190 GeV/c and a composition of 1% anti-protons, 97% pions and 2% kaons,
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beams with a nominal momentum of 190 GeV/c and a composition of 75% protons, 24% pions and 1% kaons,
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Investigation of Charm Production in Hadronic Interactions Using High-Resolution Silicon Detectors
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The main advantage of a fixed target experiment is the large acceptance. Due to the
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The M2 beam line is able to transport various secondary and tertiary
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Neutral particles, i.e. photons are detected with electro-magnetic
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Unpolarised quark transverse momentum distribution and strangeness
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According to the physics goal, a suitable target is needed. For
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Common Muon and Proton Apparatus for Structure and Spectroscopy
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Common Muon and Proton Apparatus for Structure and Spectroscopy
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To distinguish between the different particle types in the
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beams with a nominal momentum of 160 GeV/c or 200 GeV/c,
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Safety of high-energy particle collision experiments
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Nucleon tomography (Deep Virtual Compton Scattering)
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Electron–Positron Collider 24: 478:, scintillating fibre stations, 429:Ring-Imaging CHerenkov detector 386:, a Cherenkov detector is used. 522:Collaboration Official website 450:, gaseous electron multiplier, 292:Pion and kaon polarisabilities 242:Gluon polarisation in nucleons 1: 1141:Scientific committees of CERN 1106:Worldwide LHC Computing Grid 1035:Non-accelerator experiments 818:81 cm Saclay Bubble Chamber 169:at the M2 beam line of the 2344: 527:COMPASS experimental setup 438:, micro mesh gas detector, 259:Search for exotic states: 136:Proton Synchrotron Booster 1149: 1136:Directors-general of CERN 204:History and physics goals 23: 2328:Fixed-target experiments 1068:Future Circular Collider 690:Super Proton Synchrotron 262:Light meson spectroscopy 17:Super Proton Synchrotron 1063:Compact Linear Collider 699:List of SPS experiments 660:List of LEP experiments 601:List of LHC experiments 188:COMPASS experiment logo 167:fixed-target experiment 316: 307:Experimental Apparatus 276: 239:Nucleon spin structure 229: 194:nucleon spin structure 189: 165:") is a 60-metre-long 592:Large Hadron Collider 545:experiment record on 543:CERN-NA-058 (COMPASS) 402:dilution refrigerator 314: 274: 227: 187: 2323:Particle experiments 1111:Microcosm exhibition 813:30 cm Bubble Chamber 442:Pixelised MicroMegas 302:d-Quark Transversity 827:Linear accelerators 265:Baryon spectroscopy 256:Pion polarisability 198:hadron spectroscopy 117:Linear accelerators 108:SPS preaccelerators 33:Key SPS Experiments 20: 1130:(2013 documentary) 873:Other accelerators 808:2 m Bubble Chamber 774:Proton Synchrotron 317: 277: 230: 190: 146:Proton Synchrotron 53:Underground Area 2 43:Underground Area 1 2305: 2304: 1167: 1166: 919:LPI (LIL and EPA) 151: 150: 132:(not marked) 2335: 2318:CERN experiments 1194: 1187: 1180: 1171: 1157: 1156: 1131: 1077:Related articles 1025: 937: 908: 885:AC (part of AAC) 880:AA (part of AAC) 576: 569: 562: 553: 537:The CERN Courier 28: 21: 2343: 2342: 2338: 2337: 2336: 2334: 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536: 498:calorimeters 495: 489: 481: 475: 467: 459: 453: 447: 441: 435: 425: 422:Spectrometer 413: 409:unpolarised 408: 406: 396: 394: 383: 376: 369: 358: 351: 345: 339: 335: 326: 318: 282:(2012-2021) 279: 278: 235:(2002-2011) 232: 231: 207: 191: 179:spectrometer 162: 158: 154: 152: 78: 798:PS215/CLOUD 547:INSPIRE-HEP 384:hadron beam 2312:Categories 803:Gargamelle 734:NA61/SHINE 490:Hodoscopes 436:MicroMegas 295:Polarised 280:COMPASS II 215:MicroMegas 397:polarised 377:muon beam 297:Drell-Yan 233:COMPASS I 127:(Linac 3) 1159:Category 1084:LHC@home 997:Miniball 992:LUCRECIA 987:ISOLTRAP 950:facility 504:See also 375:For the 359:electron 336:positive 113:p and Pb 1002:MIRACLS 962:COLLAPS 859:Linac 3 854:Linac 2 159:COMPASS 121:protons 79:COMPASS 1017:WISArD 972:EC-SLI 948:ISOLDE 864:Linac4 764:HOLEBC 670:DELPHI 631:MoEDAL 585:(CERN) 476:SciFis 469:Straws 391:Target 371:done: 2297:WA103 2292:WA102 2287:WA101 2282:WA100 1312:EMU20 1307:EMU19 1302:EMU18 1297:EMU17 1292:EMU16 1287:EMU15 1282:EMU14 1277:EMU13 1272:EMU12 1267:EMU11 1262:EMU10 1023:WITCH 924:n-TOF 906:PS210 849:Linac 844:CLEAR 834:AWAKE 704:AWAKE 692:(SPS) 665:ALEPH 653:(LEP) 641:FASER 636:TOTEM 611:ATLAS 606:ALICE 594:(LHC) 157:, or 89:SHINE 19:(SPS) 2273:WA99 2268:WA98 2263:WA97 2258:WA96 2253:WA95 2248:WA94 2243:WA93 2238:WA92 2233:WA91 2228:WA90 2223:WA89 2218:WA88 2213:WA87 2208:WA86 2203:WA85 2198:WA84 2193:WA83 2188:WA82 2183:WA81 2178:WA80 2173:WA79 2168:WA78 2163:WA77 2158:WA76 2153:WA75 2148:WA74 2143:WA73 2138:WA72 2133:WA71 2128:WA70 2123:WA69 2118:WA68 2113:WA67 2108:WA66 2103:WA65 2098:WA64 2093:WA63 2088:WA62 2083:WA61 2078:WA60 2073:WA59 2068:WA58 2063:WA57 2058:WA56 2053:WA55 2048:WA54 2043:WA53 2038:WA52 2033:WA51 2028:WA50 2023:WA49 2018:WA48 2013:WA47 2008:WA46 2003:WA45 1998:WA44 1993:WA43 1988:WA42 1983:WA41 1978:WA40 1973:WA39 1968:WA38 1963:WA37 1958:WA36 1953:WA35 1948:WA34 1943:WA33 1938:WA32 1933:WA31 1928:WA30 1923:WA29 1918:WA28 1913:WA27 1908:WA26 1903:WA25 1898:WA24 1893:WA23 1888:WA22 1883:WA21 1878:WA20 1873:WA19 1864:WA18 1859:WA17 1854:WA16 1849:WA15 1844:WA14 1839:WA13 1834:WA12 1829:WA11 1824:WA10 1691:NA66 1686:NA65 1681:NA64 1676:NA63 1671:NA62 1666:NA61 1661:NA60 1656:NA59 1651:NA58 1646:NA57 1641:NA56 1636:NA55 1631:NA54 1626:NA53 1621:NA52 1616:NA51 1611:NA50 1606:NA49 1593:NA48 1588:NA47 1583:NA46 1574:NA45 1569:NA44 1560:NA43 1555:NA42 1550:NA41 1545:NA40 1540:NA39 1535:NA38 1530:NA37 1525:NA36 1520:NA35 1507:NA34 1502:NA33 1497:NA32 1488:NA31 1483:NA30 1478:NA29 1473:NA28 1468:NA27 1463:NA26 1458:NA25 1453:NA24 1448:NA23 1443:NA22 1438:NA21 1433:NA20 1428:NA19 1423:NA18 1418:NA17 1413:NA16 1408:NA15 1399:NA14 1394:NA13 1385:NA12 1380:NA11 1375:NA10 1257:EMU9 1252:EMU8 1247:EMU7 1242:EMU6 1237:EMU5 1232:EMU4 1227:EMU3 1222:EMU2 1217:EMU1 1042:CAST 1012:VITO 967:CRIS 914:LEIR 900:LEAR 839:CTF3 793:BEBC 788:LEIR 776:(PS) 759:LEBC 754:BIBC 739:NA62 729:NA60 719:NA49 714:NA48 709:CNGS 675:OPAL 626:LHCf 621:LHCb 483:MWPC 448:GEMs 407:For 338:and 196:and 175:CERN 153:The 125:Lead 119:for 99:NA62 69:NA32 59:NA31 1819:WA9 1814:WA8 1809:WA7 1804:WA6 1799:WA5 1794:WA4 1789:WA3 1784:WA2 1775:WA1 1757:UA9 1752:UA8 1747:UA7 1742:UA6 1733:UA5 1724:UA4 1719:UA3 1714:UA2 1709:UA1 1370:NA9 1365:NA8 1360:NA7 1355:NA6 1350:NA5 1345:NA4 1340:NA3 1335:NA2 1330:NA1 1007:SEC 982:ISS 977:IDS 895:ISR 783:PSB 749:UA2 744:UA1 616:CMS 535:", 219:GEM 211:LHC 173:at 171:SPS 49:UA2 39:UA1 2314:: 934:Sp 929:SC 890:AD 680:L3 217:, 142:PS 2277:2 2275:/ 1868:2 1866:/ 1779:2 1777:/ 1737:2 1735:/ 1728:2 1726:/ 1601:2 1599:/ 1597:1 1595:/ 1578:2 1576:/ 1564:2 1562:/ 1515:3 1513:/ 1511:2 1509:/ 1492:2 1490:/ 1403:2 1401:/ 1389:2 1387:/ 1193:e 1186:t 1179:v 938:S 936:p 575:e 568:t 561:v 531:" 472:, 464:, 456:, 444:,

Index


UA1
UA2
NA31
NA32
COMPASS
SHINE
NA62
Linear accelerators
protons
Lead
Proton Synchrotron Booster
Proton Synchrotron
fixed-target experiment
SPS
CERN
spectrometer

nucleon spin structure
hadron spectroscopy
LHC
MicroMegas
GEM

Quark transverse momentum distribution

Drell-Yan

particle beams
dilution refrigerator

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