DetectorIntro: Difference between revisions
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{| class="wikitable" style="background-color:Gainsboro;" cellpadding="10" | <br> | ||
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The Mu2e Experiment is a search for a muon directly converting to an electron without undergoing standard decay. The experiment will search for this rare process at an unprecedented level of precision. Click on the picture or buttons to learn more about the detector! | |||
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[http://mu2e.fnal.gov/atwork/workgroups/Accelerator/Acronyms.shtml MAD: Mu2e Acronym Dictionary] | |||
([http://mu2e.fnal.gov/atwork/tmp/ static clickable]) | |||
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{| class="wikitable" style="margin: auto; background-color:Gainsboro;" cellpadding="10" | |||
|[[ProtonBeamIntro|Proton Beam]] | |[[ProtonBeamIntro|Proton Beam]] | ||
|[[ProductionSolenoidIntro|Production Solenoid]] | |[[ProductionSolenoidIntro|Production Solenoid]] | ||
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|[[MuonBeamlineIntro|Muon Beamline]] | |[[MuonBeamlineIntro|Muon Beamline]] | ||
|[[ShieldingIntro|Shielding]] | |[[ShieldingIntro|Shielding]] | ||
|[ | |[http://mu2e.fnal.gov/atwork/general/blessed/project_management/index.shtml Project Management] | ||
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|[[ | |[[ComputingTutorials|Computing]] | ||
|[[Detector Control System]] | |||
|} | |} | ||
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File:FullDetector.png|thumb|center|900px|alt=Drawing of the mu2e detector.|The mu2e detector. Click on a detector image to learn more! | |||
poly 77 134 78 150 109 146 103 127 [[ProductionTargetIntro|Production Target]] | |||
poly 37 112 40 185 162 163 161 91 [[ProductionSolenoidIntro|Production Solenoid]] | |||
poly 165 117 165 148 230 138 288 152 326 188 392 203 446 202 433 171 393 172 356 164 315 130 277 113 233 107 191 112 [[TransportSolenoidIntro|Transport Solenoid]] | |||
poly 521 161 520 167 547 163 545 154 [[MuonStoppingTargetIntro|Muon Stopping Target]] | |||
poly 600 124 595 155 608 174 705 156 707 130 695 102 680 107 [[TrackerIntro|Tracker]] | |||
poly 714 102 707 124 715 143 721 150 753 144 758 138 759 120 751 101 744 93 [[CalorimeterIntro|Calorimeter]] | |||
poly 449 137 452 210 818 133 813 68 [[DetectorSolenoidIntro|Detector Solenoid]] | |||
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{| style="margin: auto; width=100%; border-style: none; border-width: 0" cellpadding="10" cellspacing="10" border="0" | |||
|<imagemap> | |||
File:Extinction-Monitor-overview-drawing.png|thumb|center|500px|alt=Drawing of the Production Solenoid, the proton absorber and the Extinction Monitor area.|Overview drawing of the Production Solenoid, the proton absorber and the Extinction Monitor area. Note the proton beam is incident from the left in this picture. Click on a image to learn more! | |||
poly 405 205 510 185 775 165 775 0 582 0 582 78 405 169 [[ExtinctionMonitorIntro|Extinction Monitor]] | |||
poly 400 214 400 275 520 265 520 194 [[ExtinctionMonitorIntro|Proton Dump]] | |||
poly 135 366 209 366 179 240 169 240 [[ProductionTargetIntro|Production Target]] | |||
poly 50 90 50 230 220 220 220 125 280 125 280 90 [[ProductionSolenoidIntro|Production Solenoid]] | |||
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|<imagemap> | |||
File:CRV-overview-drawing.png|thumb|center|500px|alt=Drawing of the Cosmic Ray Veto covering the downstream half of the Transport Solenoid and the Detector Solenoid.|Overview drawing showing the Cosmic Ray Veto that covers the downstream half of the Transport Solenoid and the Detector Solenoid. Click on a image to learn more! | |||
poly 200 0 200 400 800 400 800 0 [[CosmicRayVetoIntro|Cosmic Ray Veto]] | |||
poly 0 150 0 400 200 400 200 0 [[TransportSolenoidIntro|Transport Solenoid (upstream half)]] | |||
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|} | |||
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[[Category:Experiment]] | |||
[[Category:Tutorial]] |
Latest revision as of 16:27, 3 October 2023
The Mu2e Experiment is a search for a muon directly converting to an electron without undergoing standard decay. The experiment will search for this rare process at an unprecedented level of precision. Click on the picture or buttons to learn more about the detector!
MAD: Mu2e Acronym Dictionary
(static clickable)