particle detection - rhigrhig.physics.wayne.edu/reu/new_talks/detectors2016.pdf · what is...
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ParticleDetectionHowtoseetheinvisible
RobertHarr
WhatIsDetection?• Howcanwe“see”asubatomicparticle?
o Byitsinteractionswithordinarymatter.
• Whatkindofinteractionsdoesasubatomicparticlehavewithordinarymatter?o Ordinarymatteriscomposedofatoms.Interactionscanoccurwiththe:• bulkmaterial,• molecularbonds,• atomicelectrons,and• nuclei.
o Theatomicpictureisveryuseful!13 May 2016 R. Harr 2
AGeneralPurposeDetector
13 May 2016 R. Harr 3
Detection• Requirescreatingameasurablesignal:
o somethingthatcanbeseenbyeyeo anelectricsignalthatcanberegisteredo achemicalchangetosomethingthatcanbemadevisibleafterachemicalreaction
• Wenormallyconsiderthedetectormaterialtobeatresto incidentparticleonfixedtargetgeometry
13 May 2016 R. Harr 4
WheretoBegin?• Somanypossibledetectormaterials:o gas,liquid,solido atomicormolecularo HtoU
• Andsomanypossiblesignals:o heat,light,electric
• Canwesimplifythis?
13 May 2016 R. Harr 5
• Therearehundredsofparticles:o leptons,quarkso bosons:γ,W,Z,Ho combinationsofquarks:mesonsandbaryons
o deuterons,alphas,...o newparticles:axions,SUSY,darkmatter,...
• Canwewinnowthislistdown?
WhichParticles?• Whichparticlesaredirectlydetectable?
o Thosethatlivelongenoughtotraversedetectormaterial
• Enumeratethem(it’sasmallnumber):o photonγo electronandpositrone±
o muonandanti-muonµ±
o chargedpions π±
o chargedkaons K±
o protonandanti-protonp±
o neutronsn andanti-neutronsn,andneutralkaon K0
o afewofthestrangebaryons,inspecialcaseso somespeculativeparticleslikedarkmatterormag.monopoles
13 May 2016 R. Harr 6
hadrons
WhatAboutOtherParticles?• Detectionofallotherparticlesisviatheirdecayproducts,forexample:o K0Sà π+π−
o D+(s) à φ π+ à K+K-π+ (seeplot)
o Z0 à e+e-,µ+µ-,bb• b quarksareseenasjetswithadisplacedvertex• jetsareacollectionofdetectableparticlesinanarrowcone
oW± à e±νe ,µ±νµ• neutrinosaren’tseensomuchasinferredfromanimbalanceofmomentumperpendiculartothecollisionaxisreferredtoasmissingtransverseenergyorMET.
13 May 2016 R. Harr 7
WhatCanBeMeasured?• Firstistodetectthataparticleispresent.
o Forlowenergyphotons,darkmatter,and[lowenergy]neutrinos,thatisaboutallthatcanbemeasured
• Forotherparticleswewouldliketoknow:o chargeo typeofparticle(mass)o energyandmomentumo spin(?!)
• Thesearedeterminedfromthewayparticlesinteractwithamacroscopicdetector(matter).
13 May 2016 R. Harr 8
TheInteractions• Thebasicinteractionscanbefurthersubdividedintoasurprisinglyshortlist.
• Iwillnotdiscussinteractionsthateffectmolecularbonds.o Thesearenotusedinelectronicdetectorssincechemicalprocessingisneeded(uptonow).
o Thesecomeintoplaywithphotographicemulsionsandsometypesofplasticdetectors.
o Otherfamousexample:RayDavis’solarneutrinoexpt.o Consultreferencesifyouneedmoreinformation.
13 May 2016 R. Harr 9
Interactions(cont’d)1. Interactionswith(orrequiring)atomicnuclei-
- maybefamiliarfrommodernphysicscourses:
a) Pairproductionb) Bremstrahlungc) Nuclear(hadronic)interaction
• Thefirstappliestophotons,thesecondtoelectrons(mostly),andthelasttohadrons.
13 May 2016 R. Harr 10
Interactions(cont’d)2. Interactionswithatomicelectronsarewidely
used:a) ComptonScatteringb) Photoelectriceffectc) Ionizationofatomsd) Excitationofatoms
• Thefirsttwoapplyonlytophotons,thelasttwoapplytoallparticles.
13 May 2016 R. Harr 11
Interactions(cont’d)3. Interactionswithbulkmaterialmaybethe
leastfamiliar:a) Cerenkovradiationb) Transitionradiation
• Iwillnotbeabletocoverthesetoday.o Checkthebackupslidesforsomeinformationonthese.o AgoodintroductioncanbefoundinJackson’sClassicalElectrodynamics.
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ThePhysicsofDetection
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14
InteractionswithElectrons• Interactionswithatomicelectronsmaybethesinglemostimportantdetectionprocessforparticleexperiments.o Primaryprocessfor“tracking” particleso Alsoimportantforproducinglargenumbersoffreeelectronsforadetectablecurrent.
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15
ThePhotoelectricEffectFamiliarfromModernPhysicsclass.Einstein’sexplanationrequiresquantizedenergyforphotons.
Energyofliberatedelectronsdependsonthefrequencyoflight(photons).
Rateofelectrons(current)dependsontheintensityofthelight(rateofincidentphotons).
Photomultipliertubesusethephotoelectriceffecttoconvertincomingphotonstoelectrons(singlephotondetection).Silicondetectors(strips,pixels,CCD’s)usethephotoelectriceffecttocreateanelectron-holepair.13 May 2016 R. Harr 15
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ComptonScatteringAsecondtypeofphoton-matterinteraction.Usuallyappearswhendiscussingrelativity.
Importantforintermediateenergyphotons.
Incidentphotonlosesenergywhenejectinganelectronfromanatom.
Processisimportantto“breakdown” ahighenergyphotonintoelectrons.Theenergyofthephotondeterminesthefinalnumberofelectronsproduced.(Seecalorimetry)
13 May 2016 R. Harr 16
The Bethe-BlochFormula• Semi-classicalcalculationofenergyloss
• Notethecompetitionbetweenln(β2γ2)and–β2o Causesaminimumintheenergylosso MinimumenergylossscalesroughlyasZ/Aofthematerial.
• 4MeVcm2/gforHtoabout1MeVcm2/gforheavyelementso Minimumenergylosswhenβγ ≈3to3.5o Dependsonkinematics,independentofparticletype
• δ termrepresentsdensityeffect13 May 2016 R. Harr 17
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18
Energy Loss
13 May 2016 R. Harr 18
DependenceonMaterialEnergylossdependsonthetypeofmaterialandparticle.AtomswithhigherZhavelessenergylossperg/cm2
Buttheirhigherdensity(g/cm3)morethanmakesupforthis.
13 May 2016 R. Harr 19
ScintillationManymaterialsemitlightwhenatomsormoleculesareexcitedbyachargedparticlepassingnearbyEmittedlightiscalledscintillationScintillatingmediumusuallytransparentLight(onetoa fewphotons)detectedbyaphotomultiplier
13 May 2016 R. Harr 20
InteractionswithNuclei• Twotypesofinteractionarepossible
o Electromagnetico Strong
• Detailsareinthebackupslides
13 May 2016 R. Harr 21
(1)Electromagnetic• Mostlysinglephotonexchange
o elasticinteractions
• Whenalightobject(particle)scatterselasticallyfromaheavyobject(nucleus):o littlelossofenergyo canchangedirectionsignificantly
• thinkoftheRutherfordscatteringexperiment• mostscatteringissmallangle• largenumberofsmallanglescatterscanbetreatedstatistically
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23
PairProductionAthirdtypeofphoton-matterinteraction.Exampleofconversionofenergyintomass.
Importantforhighenergyphotons.
Incidentphotonconvertsintoanelectron-positronpair.
Processisimportantto“breakdown” ahighenergyphotonintoelectrons.Theenergyofthephotondeterminesthefinalnumberofelectronsproduced.(Seecalorimetry.)
Presenceofmatterisrequiredtoconserveenergy-momentum.
13 May 2016 R. Harr 23
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BremstrahlungAGermanwordfor“brakingradiation”.
Importantforhighenergyelectrons.
Incidentelectronemitsaphoton(usuallyx-ray),whenacceleratedintheelectricfieldofanucleus.
Processisimportantto“breakdown” ahighenergyelectronintolowenergyelectrons.Theenergyoftheincidentelectrondeterminesthefinalnumberofelectronsproduced.(Seecalorimetry.)
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SynchrotronRadiationLikeBremstrahlung,butaccelerationduetoa
magneticfield.
13 May 2016 R. Harr 25
(2)StrongInteractionsImportantformeasuringtheenergyofprotons,neutrons,pions,andkaons(calorimetry).
13 May 2016 R. Harr 26
ATypicalDetector
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BuildinganExperimentIdeallywewanttoidentifyeverything(particletype,charge,spin,pointoforigin,momentumatpointoforigin)emergingfromacollisioninordertoreconstructexactlywhatoccurred.
Webuildadetectorthatcomesasclosetoachievingthisgoalasmoneyallows.
Interestingcollisionscontainshortlivedparticles(top,bottom,orcharmquarks,WorZbosons,Higgsparticles,oradeconfined quarkstate)thatcannotbedirectlyseen,andmustbeinferredfromtheproductstheyleavebehind.
13 May 2016 R. Harr 28
CollideParticles
• atveryhighenergiesandconvertenergyintomass(i.e.otherparticles)
13 May 2016 R. Harr 29
DetectorLayout• Colliderdetectorshaveconvergedonastandardconfiguration.Movingoutwardfromthecollisionwehave:o precisiontrackingo trackingtomeasurecurvatureinasolenoidal magneticfield
o Cerenkovdetector,TOF,transitionradiationdet.(optional)o electromagneticcalorimetero hadronic calorimetero muondetector(alwaysoutermost)
13 May 2016 R. Harr 30
AGeneralPurposeDetector
13 May 2016 R. Harr 31
Tracking• measuretheorigin(vertex)ofchargedtracks• measurethemomentumofchargedtracks• requires:
o amagneticfieldofsufficientstrengthandextent(tomeasureradiusofcurvature)
o largevolumetracking(drivenbycost)o highprecisionmeasurementsnearthecollisionpt.o possiblysomeparticleID(dE/dx,TOF,Cerenkov,TRD)
13 May 2016 R. Harr 32
MeasuringMomentum• Inauniformmagneticfield
o p cosλ =0.3zBRo whereB isinTesla,R inmeters,z inmultiplesoftheprotoncharge,p inGeV/c.
• Theuncertaintyonp comesfrom2sources:i. resolutionoftrackpositionmeasurementsii. multiplescatteringofmaterialinthedetectoro Thesecondsourceleadsustousethinsilicondetectorsorgaseousdetectors
13 May 2016 R. Harr 33
Calorimetry• Measuretheenergyinchargedandneutralparticles
• Hadronsinteractdifferentlyfromphotonsandelectrons.EMcalorimeterplacedbeforehadronic calorimeter
13 May 2016 R. Harr 34
MeasuringEnergy• Converttheenergyofhighenergyparticlesinton lowenergyparticleso n ~E/E0 whereE0 istheaverageenergytoproducealowenergyparticle.
o ThenumberofparticlesisstochasticquantitywithPoissonfluctuationsà wewillmeasuren ± √n particles
o ThemeasuredenergyisE ± √E,sotherelativemeasurementuncertaintyis1/√E
13 May 2016 R. Harr 35
PhotonDetection• Detectingphotonsisimportantinmanysituations:astronomy,calorimetry,TOF,...
• Commondetectorsareo photomultipliers
• fastsignals,highsensitivity,lowgranularityo CCDs
• highgranularity,timeintegrating
13 May 2016 R. Harr 36
CCD• Thesensorsfordigitalcameras• Semiconductordevices,usuallysilicon• CanbecustomizedforsensitivityinIR,visible,orUV.
13 May 2016 R. Harr 37
MuonDetector• Muons are200timesheavierthanelectrons.• Muons bremstrahl with(200)2 smallerprobability
• Theresultisthattheycanpassthroughmuchmorematerialwithoutinteractingthanotherchargedparticles.
• Muondetectorisbasicallyachargedparticletrackerlocatedbehindlotsofmaterial.
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Backup
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(1)Electromagnetic(cont’d)• MultipleCoulombscattering(MCS)
o yieldsaroughlyGaussiandistributionofscatteringangles
o X0 iscalledtheradiationlengthofthematerial• characterizeselectromagneticinteractionswithnucleiinamaterial
o Scatteringindependentofparticletype(excepte-)
13 May 2016 R. Harr 41
P (q)dq =1p
2pq0eq2/2q2
0dq
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bpc
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42
TransitionRadiationRadiationproducedwhenahighlyrelativisticelectronpassesthroughmaterialswithdifferentindicesofrefraction.
13 May 2016 R. Harr 42
CerenkovRadiationEmittedwhenaparticleexceedsthespeedoflightinamediumLiketheshockwavefromasupersonicplaneConeangleisrelatedtoparticlevelocity
13 May 2016 R. Harr 43
ElectromagneticShowers• Tomeasuretheenergyofanincomingparticle
o Convertasinglehigh-energyparticleintomanylow-energyparticles,andcountthenumberofparticles.
o Theconversioniscalledashower.o pairproduction:1photonà 2electronso Comptonscattering:1photonà 1photon+1electrono bremstrahlung:1electronà 1electron+1photon
• AftertraversingdistanceXofamedium,theaverageenergyofanelectron/photonis:
13 May 2016 R. Harr 44
hEi = E0e�X/X0
Hadronic Showers• Sameideaasforelectromagneticshowers
o incomingparticleisahadrono interactionswithmaterialcharacterizedbyinteractionlengthλI
o radiationlengths<<interactionlengthso therefore,electromagneticcalorimetersprecedehadroniccalorimetersinadetector
13 May 2016 R. Harr 45
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