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L0/L1 trigger development of ALICE PHOS detector PDF

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L0/L1 trigger generation by the ALICE PHOS detector Lijiao Liu (cid:6) (cid:7) (cid:5) (cid:8) (cid:4) (cid:4) (cid:3) (cid:9) (cid:10) (cid:2) (cid:8) (cid:8) (cid:11) (cid:4) (cid:8) (cid:6) (cid:3) (cid:7)(cid:12)(cid:6) Dissertation for the degree philosophiae doctor (PhD) at the University of Bergen October 2011 Contact: LijiaoLiu InstituteofPhysicsandTechnology UniversityofBergen Allégaten55 5007Bergen Norway Email: [email protected] Privateemail: [email protected] Acknowledgements I started my PHD program in spring 2008, now it comes to the end with the submission of the thesis. Working on the interesting and challenge project brings me to a large group of internationalcolleagues,withwhomIenjoyedverynicecooperationandfruitfulexchangeof ideas. WhenIthinkback, mystudyinBergeniswonderful, exciting, andworthcherishing, even though there have been moments of hard work and exhaust. I appreciate that I have experiencedalotduringthework. Attheveryfirst, IwouldliketothankmysupervisorDieterRöhrichandKjetilUllaland for giving me the chance to work in the group and guiding me on both my work and life. DieteralwayssupportsmeandgivesmehelpwheneverIneed. AndIalwaysadmirehisway of explaining complicated physics in easily understandable and short words. His relax and kind personality deeply impresses me too. Kjetil has been a main source of knowledge and inspiration for me. He has had many long and priceless discussions with me, both on work and life, which greatly help me get through my PHD period. I’m always influenced by his intelligence,optimisticandhappiness. DiscussingwithhimhighlightsmydaywhenI’mlack of motivation or unhappy. Dieter and Kjetil, thanks a lot! I appreciate deeply being your studentandIwishIcouldbeyourstudentagain! IowemyspecialthankstoprofessorsGuangmingHuangandDaicuiZhou,whogaveme thechancetoapplythepositionofworkingontheproject. Daicuifirstlyprovidedthechance oftheposition.WhenIhesitated,Guangmingencouragedandconvincedmetoapply,making me experienced a wonderful life in Bergen. Moreover, I appreciated a lot of dinner time at CERNwithDaicui. WhenI’minBergen,youtwostillcareaboutmeverymuch,treatmeas astudent,afriendandadaughter. IwouldalsoliketothankJohanAlmeandKetilRøed,whohelpedmealotatthebegin- ningofmywork. ItwasunforgettablethatJohansentmethedocumentationformyworkon Chinese New Year and regards for my birthday the same day on 2008. Ketil was a nice of- ficemate,gavemeinvaluablehelp. Youtwoalwaysgavemedetailedandpatientanswers,no matterhowstupidmyquestionswereandhowbusyyouwerewithyourthesis. Iappreciated alot!Thanksagain! IwouldliketothankHongyanYang,LiangSunandYunCheng,whohelpedmestartthe i ii Acknowledgements studylifeinBergen.Withoutyou,IcouldnotgetusedtomylifeinBergenassoonaspossible. IhavehadthepleasureofworkingcloselywithDongWang,whohasbeenmyfriendfor 10years. Wehavesharednotonlyalotoftasks, butalsoalotofnicemomentsofcooking, havingdinnerandhiking. Hehasbeenanimportantmotivatorinmyworkandanicefriend inmylife. ThesamethankgoestoMeidanaHuang, whoisaniceroommate, anintelligent colleagueonmyworkandthebestfriendinmylife.Wewenttogetherforconferences,shared a lot of nice moments at CERN. Dana, thank you! You have made my life enjoyable and colorful.Iwon’tfeellonelybecauseofyou! ThanksalsogotoJoakimNystrand,Per-ThomasHille,ØysteinDjuvsland,SveinLindal, HenrikQvigstadandKyrreSkjerdalforansweringmyquestionsnicelyandgivingmecount- less ride at CERN. I appreciated a lot! Jiri Kral deserves a lot of thanks for answering my stupid questions with great patience and helping with my work. So does Yuri Kharlov, who answerspatientlymyemailingreatdetail,helpingmeunderstandeasily.Aspecialthankgoes toHåvardHelstrupalso,whohelpedmewiththesetupoftheDAQsystematthelabefficiently. MygratefulthanksgotoDominikFehlkertoo,withwhomIsharedalotoffunnytimeand havingfruitfuldiscussionaboutwork. I’mimpresseddeeplybyhispatienceandconsiderate- ness. Iwon’tforgetthefirsttimeheshowedmeandDanathesetupatthelabatCERN,the nice invitation for fishing and the computer games during rest time, the nice accompany for walkingushome,nottomentioncountlessrideaftergroupparties.DagToppeLarsendeserves muchofmyappreciationforencouragingmewhenI’mdepressed,forhelpingmewithLatex, Aliroot,andforreadingthroughmythesisandcorrectinginabettershape. Specialthanksgo toShimingYang,whohasgivenmealotofhelponwork,wehavealotofnicediscussionon both life and work. Thanks also go to Kalliopi Kanaki, Sebastian Bablok, Gaute Øvrebekk, ØysteinSennesetHaaland,HegeErdal,CamillaHanquistStokkevåg,YngveSkogseide,Njål Brekke,ArildVelure,EivindLarsen,Per-IvarLønne,KristianYtre-Hauge,ThomasChristoph Solem,andAndreasSamnøy. Thanksyouallwithyourgreathelponbothworkandlife. Ad- ditionally,IwouldliketothankmyothercolleaguesinPHOSgroup,microelectronicsgroup andNuclearPhysicsgroupwhohavecontributedthehelpinonewayoranother. AlthoughI havenottalkedmuchwithsomeofyou,thesmilesonyourfacesencouragemealot.Working togetherwithyouisalwaysinterestingandenjoyable. MydeepgratitudegoestoBiancaRossforalwayscaringmuchaboutme,invitingmeto her many nice dinner parties. Your concern could not mean more to me. I won’t forget the words she encourages me every time she meets me. I won’t forget the regards when I was at CERN for work and Spring Festival. I won’t forget the electronic card for my Birthday. Bianca, thanks you very much, I love you! I have never met a lady with such a broad and goldenheartasyoubeforeever,yourfascinatingpersonalityinfluencesme. IalsohadchancetomeetalotofcolleaguesandfriendsfromHuazhongNormalUniversity iii atCERN,thankyouall,alotofdinnertimewithyoumademystaysatCERNveryenjoyable andmemorable! ManythanksgotomyChinesefriends(toomanytobelistedhere)inBergen,weshared alotofwonderfultimeinBergen. Thanksallofyoutokeepmehappyinaforeigncountry. AlsothanksmyfriendsinChinaforencouragingmeandsupportingme. Finally,Iowethankstomyparents,sisters,brothers-in-law,brothers,nephewsandniece, yourloveandconstantsupportaregreatstrengthformetogothroughtheseyears.Ihavebeen farawayfromyouforfouryears,Imissedalotoffamilyactivitiesinthepast10years. You alwaysunderstandmewithoutcomplaining.Thanks,Iloveyou! Abstract Quark-GluonPlasma(QGP)isaphasethatexistsaboveacriticaltemperatureandcorrespond- ingenergydensityaccordingtothetheoryofQuantumChromo-Dynamics(QCD).Thestudies oftheQGPhelpustounderstandtheearlyevolutionofouruniverseandtheStandardModel. A large Ion Collider Experiment (ALICE) aims to study the properties of the QGP. A QGP cannotbeobserveddirectlybecauseitisashortlivedstate.Signaturessuchasjetquenching, flowpatternandhigh p suppressionindicatetheexistenceofaQGP.Varioussub-detectors T are designed for detecting these signatures. The PHOton Spectrometer (PHOS), one of the sub-detectors, isahigh-resolutionelectromagneticcalorimeterdedicatedtotheprecisemea- surementofdirectphotonandneutralmesonyieldsina p rangeupto100GeV/c. T Four online systems are developed to monitor, control and read out the different sub- detectors. The trigger system is one of them. The task of the trigger system is to select events of interest and to reduce the overall data flow in the ALICE experiment. Three lev- elsoftriggersandaHighLevelTrigger(HLT)aredesignedtomakeoptimaluseofdifferent sub-detectors, which vary in readout time. The PHOS detector generates two levels of trig- gers: i) the Level-0 (L0) trigger selects high p clusters in Pb+Pb and in p+p collisions; ii) T theLevel-1(L1)triggercorrespondstoamoresophisticatedshoweranalysiswhichrefinesthe eventselection. The main objective of the thesis has been to develop the PHOS trigger firmware, to im- plementitinanFPGAandtocommissionit. TheALICEL0triggerhasalatencyof1.2μs, limitingthetimeforgeneratingL0triggersinthePHOSdetector.Thealgorithmsarebasedon thedigitizedsignalfromAvalanchePhoto-Diodes(APDs). Asliding-windowclusterrecon- structoristhecriticalpart. Alotofeffortshavebeenmadetofulfillthetimingrequirement. TheALICEL1triggerhasalatencyof6.5μs,leavingmoretimetorefinetheeventselection. TherearethreetypesofL1triggersforPHOS:onebasicL1triggerandtwoadvancedones: total energy trigger and isolated photon trigger. The firmware development focuses on the L0generation(chapter5). Thetiminganalysis(chapter5),testingandcommissioningofthe PHOSL0trigger,whichisthemaineffortduringthePhDprojectaswell,havebeenperformed (chapter 7). The generation of L1 triggers is discussed in chapter 6, where the firmware for the basic L1 trigger is implemented. The algorithms and related resource consumption for v vi Abstract theadvancedL1triggersareanalyzed, buttheyhavenotbeencommissionedyet. Addition- ally,simulationshavebeendonetoanalyzehowseveralfactorsaffectthetriggerperformance (chapter6). The outline of this thesis is given as follows: After a very brief overview of the physics goal,thesub-detectorsandtheonlinesystemsoftheALICEexperimentaredescribedinchap- ter1.ThePHOSdetectorisspecifiedthoroughlyinchapter2.Chapter3introducesthetrigger and readout electronics, based on which the firmware for the triggers (chapter 5) is imple- mented for the PHOS detector. In chapter 4, the requirements of the ALICE PHOS triggers are given in detail. The principle of issuing triggers is discussed elaborately based on the layoutofthedetector,irrespectiveofthetriggerelectronics.Chapters5and6discussthegen- erationofL0andL1triggersrespectively.Chapter7givesthecommissioningresults.Finally, theconclusionandanoutlookaregiveninchapter8. The trigger firmware is implemented by two types of electronics boards, Trigger Region Unit(TRU)andTrigger-OR(TOR),I’mresponsiblefortheTORsince2008. TheL0trigger commissioning has started in Oct. 2008, and it is still ongoing. In addition, I performed the timing analysis, the energy and trigger channel correlation analysis and the L0 trigger performance analysis. Because the L1 algorithm was implemented in the TOR, I analyzed algorithms,resourceandtimingconsumptionofallthreetypesL1triggers,andsimulatedthe L1triggerperformance. Contents Acknowledgements i Abstract v Contents vii ListofFigures xiii ListofTables xvii 1 TheALICEexperiment 1 1.1 Quark-GluonPlasma . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1 1.2 TheLargeHadronCollider . . . . . . . . . . . . . . . . . . . . . . . . . . . 2 1.3 TheALICEexperimentalsetup . . . . . . . . . . . . . . . . . . . . . . . . . 4 1.4 TheALICEdetectorsystems . . . . . . . . . . . . . . . . . . . . . . . . . . 5 1.4.1 InnerTrackingSystem . . . . . . . . . . . . . . . . . . . . . . . . . 5 1.4.2 TimeProjectionChamber . . . . . . . . . . . . . . . . . . . . . . . 7 1.4.3 TransitionRadiationDetector . . . . . . . . . . . . . . . . . . . . . 7 1.4.4 Time-Of-Flight . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 7 1.4.5 PhotonSpectrometer . . . . . . . . . . . . . . . . . . . . . . . . . . 8 1.4.6 HighMomentumparticleidentificationdetector . . . . . . . . . . . . 8 1.4.7 Electro-MagneticCalorimeter . . . . . . . . . . . . . . . . . . . . . 8 1.4.8 ALICECosmicRayDetector . . . . . . . . . . . . . . . . . . . . . 8 1.4.9 Forwardmuonspectrometer . . . . . . . . . . . . . . . . . . . . . . 9 1.4.10 Forwarddetectors. . . . . . . . . . . . . . . . . . . . . . . . . . . . 9 1.5 TheALICEonlinesystems . . . . . . . . . . . . . . . . . . . . . . . . . . . 10 1.5.1 ExperimentControlSystem . . . . . . . . . . . . . . . . . . . . . . 10 1.5.2 TriggerSystem . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10 1.5.3 DataAcquisitionSystem . . . . . . . . . . . . . . . . . . . . . . . . 13 1.5.4 HighLevelTriggerSystem . . . . . . . . . . . . . . . . . . . . . . . 15 vii viii CONTENTS 1.5.5 DetectorControlSystem . . . . . . . . . . . . . . . . . . . . . . . . 15 2 ThePHOSDetector 17 2.1 Photonphysics . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 18 2.2 ThecomponentsofthePHOSdetector . . . . . . . . . . . . . . . . . . . . . 19 2.2.1 PWOcrystals . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19 2.2.2 AvalanchePhotoDiode. . . . . . . . . . . . . . . . . . . . . . . . . 20 2.2.3 ChargeSensitivePre-Amplifier . . . . . . . . . . . . . . . . . . . . 21 2.2.4 TheLEDSystem . . . . . . . . . . . . . . . . . . . . . . . . . . . . 22 2.2.5 ThelayoutofPHOS . . . . . . . . . . . . . . . . . . . . . . . . . . 22 2.3 IntrinsicperformanceofthePHOSdetector . . . . . . . . . . . . . . . . . . 22 3 ThePHOStriggerandreadoutelectronics 27 3.1 PHOSelectronicstopologyanddataflow . . . . . . . . . . . . . . . . . . . . 27 3.2 FrontEndCard . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28 3.2.1 Shapers . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29 3.2.2 ALTRO . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 31 3.2.3 Analog-sum. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 31 3.2.4 BoardController(BC) . . . . . . . . . . . . . . . . . . . . . . . . . 32 3.3 TriggerRegionUnit . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33 3.3.1 TheTRUoverview . . . . . . . . . . . . . . . . . . . . . . . . . . . 33 3.3.2 TheTRUresources . . . . . . . . . . . . . . . . . . . . . . . . . . . 34 3.4 TriggerOR . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 34 3.4.1 TheTORoverview . . . . . . . . . . . . . . . . . . . . . . . . . . . 34 3.4.2 TheTORresources . . . . . . . . . . . . . . . . . . . . . . . . . . . 35 3.5 DCSboard . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 36 3.6 ReadoutControlUnit . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38 3.7 BusyBOX . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 42 4 ThePHOStriggerrequirementsanddesign 45 4.1 ThePHOStriggerrequirement . . . . . . . . . . . . . . . . . . . . . . . . . 45 4.2 Triggergeneration. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 46 4.2.1 TheprincipleofissuingL0triggers . . . . . . . . . . . . . . . . . . 47 4.2.2 TheprincipleofissuingL1triggers . . . . . . . . . . . . . . . . . . 49 4.2.3 HardwareRequirements . . . . . . . . . . . . . . . . . . . . . . . . 50 5 ThegenerationofPHOSLevel-0trigger 55 5.1 ThefirmwaredevelopmentofLevel-0trigger . . . . . . . . . . . . . . . . . 55 5.1.1 TechnicalrequirementsofL0 . . . . . . . . . . . . . . . . . . . . . 56

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5.10 An analog-sum signal from an oscilloscope and its fitting function According to the QCD theory, quarks can not exist alone naturally. Lattice calculations of QCD predict that at a critical temperature and corresponding energy
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