=GHU]HQLDSURWRQSURWRQZ/+&
|
|
- Gary Wright
- 6 years ago
- Views:
Transcription
1 =GHU]HQLDSURWRQSURWRQZ/+& paczki HQHUJLD Proton-Proton REZyG Protons/bunch SROHPDJ Beam energy Luminosity ZLHWOQRü SDF]HN Crossing SSDF]ND rate 7H9 NP 7 FP V protony partony (kwarki, gluony) SU]HFLFLDSDF]HN Collisions F]VWRü 0+] RGVWS QV F]\OL P l produkty zderzenia jet l jet e + e - Higgs Z o Z o e + e - 3U]\QRPLQDOQHMZLHWOQRFLZND*G\PSU]HFLFLX SDF]HN]DMG]LH]GHU]HSURWRQSURWRQ
2 σ LHC s=14tev L=10 34 cm -2 s -1 rate ev/year barn σ inelastic LV1 input GHz mb bb MHz µb max LV2 input max LV1 output nb W Z W lν Z l + l - tt max LV2 output khz gg H SM SUSY q ~ q ~ +q ~ g ~ +g ~ g ~ tanβ=2, µ=m ~ ~ g =m q tanβ=2, µ=m ~ g =m ~ q /2 Hz pb qq qq H SM 10 5 H SM γγ h γγ tanβ=2-50 Z ARL l + l - mhz fb H SM ZZ ( * ) 4l µhz Z SM 3γ scalar LQ Z η l + l particle mass (GeV)
3 6HOHNFMDSU]\SDGNyZ :FLJXODWSUDF\/+&]DMG]LH ]GHU]HSS =DREVHUZRZDQLH³HJ]RW\F]Q\FK SU]\SDGNyZPR*H VWDQRZLüHSRNRZHRGNU\FLH³QRZHMIL]\NL 1DOH*\MHGQDNXPLHüRGV]XNDüRZHSU]\SDGNyZ ZUyGZV]\VWNLFK 6]XNDQLHLJá\ZVWRJXVLDQD" W\SRZDLJáD²PP W\SRZ\VWyJVLDQD²P LJáDVWyJ 3RV]XNLZDQLH³QRZHMIL]\NL Z/+& WRV]XNDQLHLJá\ZPLOLRQLHVWRJyZVLDQD
4 àdpljáyznd QDáR*RQ\FK]GHU]HSS ZLG]LDQ\FKSU]H]ZHZQWU]QF]üNU]HPRZHJRGHWHNWRUD PLNURSDVNRZHJR :UyGQLFKUR]SDGF]VWNL+LJJVDQDPLRQ\ =QDMG(SURVWHODG\
5 5R]ZL]DQLHáDPLJáyZNL =UHNRQVWUXRZDQHODG\RS W!*H9 :UyGQLFKGREU]HZLGRF]QHPLRQ\]UR]SDGX+LJJVD 5R]ZL]DQLHPR*OLZHMHOL]DMWRüGHWHNWRUDa SRZLHU]FKQLDPLNURSDVNDaPP! NDQDáyZRGF]\WX
6 &06DLQQHHNVSHU\PHQW\ GHWHNWRU ONDQDáyZ ]DMWRü SU]\SDGHN PR]DLNRZ\ N% PLNURSDVNRZ\ N% wczesnych kaskad N% NDORU\PHWU\ N% PLRQRZ\ N% FDáNRZLWDZLHONRüSU]\SDGNX 0% SPS Lear 40 MHz LHC CMS ATLAS CDF 330 KHz HERA 10 MHz UA1/2 250 KHz LEP 45 KHz /LF]EDNDQDáyZ WUXPLHGDQ\FKNRQWUROQ\FK&06WHPSHUDWXUD QDSLFLH LWS MHVW SRUyZQ\ZDOQ\ ]H VWUXPLHQLHP ZV]\VWNLFK GDQ\FK MHGQHJR ]H ZVSyáF]HVQ\FK HNVSHU\PHQWyZ/(3N%V
7 6\VWHPZ\]ZDODQLDWU\JHU 1RZRF]HVQHV\VWHP\SDPLFLPDVRZHMSR]ZDODM ]DSLV\ZDüa0%V 6SRUyGa SU]\SDGNyZ]DREVHUZRZDQ\FKZFLJX ND*GHMVHNXQG\MHG\QLHPR*HE\ü]DSLVDQ\FK :\ERUXGRNRQXMHV\VWHPZ\]ZDODQLD]ZDQ\WU\JHUHP 75<*(5MHVWWRGZXZDUWRFLRZDIXQNFMD ]DUHMHVWURZDQ\FKGDQ\FK VWDQXGHWHNWRUD EDGDQHMIL]\NL T( ) RGU]XFLü ]DSLVDü 3RQLHZD*QLHZV]\VWNLHGDQHVQDW\FKPLDVWGRVWSQH DIXQNFMDMHVWVNRPSOLNRZDQD7.MHVWREOLF]DQH ZNROHMQ\FKSU]\EOL*HQLDFK]ZDQ\FK VWRSQLDPLWU\JHUD 'RRGU]XFHQLDSU]\SDGNXZ\VWDUF]\RJUDQLF]RQD GRNáDGQRüGRQDVWSQHJRVWRSQLDSU]HFKRG]ZLF W\ONRSU]\SDGNL]GHF\]M]DSLVDü
8 6HOHNFMDSU]\SDGNyZ F]VWRü 10 G*HW\ 8 OHSWRQ\ 10 6 := WRS 'HWHNWRU 1 µs 3LHUZV]\VWRSLH²0+] VSHFMDOLVW\F]QHSURFHVRU\$6,&)3*$ LEVEL 1 Trigger 40 MHz Hardwired UyZQROHJáHSU]HWZDU]DQLHSRWRNRZH processors (ASIC, FPGA) MASSIVE PARALLEL Pipelined Logic Systems :\*V]HVWRSQLH N+] IDUPDVWDQGDUGRZ\FK HIGH LEVEL TRIGGERS 100 khz Standard processor SURFHVRUyZ FARMs sec +LJJV DPLüPDVRZD²+] 25 ns µs ms sec F]DVSU]HWZDU]DQLD>V@ /LF]ED SURFHVRUyZ Z IDUPLH &06 MHVW SRUyZQ\ZDOQD ] OLF]E ZV]\VWNLFK VWDFML URERF]\FK L NRPSXWHUyZ RVRELVW\FKZ&(51LHZURNXa
9 3U]HWZDU]DQLHSRWRNRZH 7U\JHUPXVL]DQDOL]RZDüGDQH]ND*GHJR]GHU]HQLD FRQVPXVL]DSDüGHF\]MDF]\MH]DSLVDü -HMZ\SUDFRZDQLHZ\PDJDMHGQDNGáX*V]HJRF]DVX 5R]ZL]DQLHSUREOHPX SU]HWZDU]DQLHSRWRNRZHF]\OL³WDPDSURGXNF\MQD DOJRU\WPSRG]LHORQ\MHVWQDNURNLZ\NRQ\ZDOQHZQV SURFHVRUVWDQRZLáDFXFKHOHPHQWyZ ]NWyU\FKND*G\Z\NRQXMHMHGHQNURNDOJRU\WPXZQV LSU]HND]XMHZ\QLNQDVWSQHPX ZWHQVSRVyESU]HWZDU]DQHGDQHSá\QSU]H]SURFHVRU aµvdz\qlnlsrmdzldmvlqdmhjrz\mflxfrqv SHáQHGDQHF]HNDMQDGHF\]MWU\JHUD Sá\QFV\QFKURQLF]QLHZSDPLFLSRWRNRZHM czas przetwarzania 3µs procesor potokowy 25 ns detektor pamiü potokowa C C B B A A bufor synchroniczny przepáyw danych asynchr.
10 Track finding Associate hits in a 2-D plane in order to identify segments, circles, etc... Pattern recognition on global 2-D data - Combinatorial logic - Lookup table - Associative memories x y Track following. Find segments built by a couple of points aligned in a given direction - Coincidence matrix - Lookup table - Mean timer S. Cittolin CERN/ECP CMS-TriDas. CERN School of Computing, Egmond aan Zee/NL.96 46
11 CMS level-1 muon trigger Primitive generators (segments, hits) Segment EXTRAPOLATION (DT,CSC) Segment recognition - Cone coincidence (RPC) - Mean timer (Tube) Pattern RECOGNITION (RPC) Track momentum - Coincidence matrix - Logic mask DT,CSC RPC LVL-1 Global Content addressable memories Matrix logic (ASIC, Gate array...) S. Cittolin CERN/ECP CMS-TriDas. CERN School of Computing, Egmond aan Zee/NL.96 47
12 Coincidence matrix (ATLAS level-1 muon trigger) Segment identification within a given angles and segments combination 0 x i 0 32 y y i u ij x c a 32 b a b c z i = x i u ij y j Two planes low occupancy detectors Tree logic for more plane/segments (and pipeline) S. Cittolin CERN/ECP CMS-TriDas. CERN School of Computing, Egmond aan Zee/NL.96 51
13 CMS calorimeter level-1. Isolated electron (sliding window algorithm) Hadron Electromagnetic HAD calorimeter Hit E T 4032 cells φ η EM calorimeter E t cut + Max ( ) > Threshold AND Longitudinal cut / < 0.05 AND HAD transverse cut < 2 GeV AND EM isolation One of (,,, ) < 2 GeV ISOLATED ELECTRON Trigger granularity (Dh * Df) No.of trigger towers ECAL : h * * 72 = 4032 h > * as ECAL HCAL : as ECAL 162 S. Cittolin CERN/ECP CMS-TriDas. CERN School of Computing, Egmond aan Zee/NL.96 41
14 CMS calorimeter level-1. Isolated electron (peak finding algorithm) Hadron Electromagnetic E T HAD calorimeter 4032 cells φ η EM calorimeter w i E i > 0 Peak finding E t cut > Threshold AND EM isolation / > 0.9 AND HAD longitudinal and transverse cut < 4 GeV ISOLATED ELECTRON Trigger granularity (Dh * Df) No.of trigger towers ECAL : h * * 36 = 4032 h > * HCAL : * S. Cittolin CERN/ECP CMS-TriDas. CERN School of Computing, Egmond aan Zee/NL.96 42
15 3U]HSá\ZGDQ\FKZ&06 GHWHNWRU 0+] MHz LLISION RATE 16 0NDQDáyZ Million channels 3 Gigacell buffers *%EXIRUyZ HQHUJLD Energy Tracks ODG,VWWU\JHUD 100 khz N+] EL-1 TRIGGER 1 Terabit/s NDQDáyZ A CHANNELS) 7HUDELWV Charge Time Pattern ádgxqhn F]DV NV]WDáW 1 0%SU]\SDGHN Megabyte EVENT 200 Gigabyte BUF 500 *%EXIRUyZ Readout memorie ZPRGXáDFK G\VWU\EXWRU *LJDELWV 0 Gigabit/s,,VWWU\JHUD 100 Hz +] TERED EVENT *LJDELWV Gigabit/s 7%G]LH SERVICE LAN 3%URN DYSTRYBUTOR SDPLüPDVRZD EVENT BUILDER. A large switching network ( ports) w throughput of approximately 500 Gbit ZHMü the interconnection between the sour (Readout Dual Port Memory) and the destinations (switch Z\Mü to Farm Interface Event Manager collects the status an request of event filters and distributes building commands (read/clear) to RD 5 TeraIPS SURFHVRUyZ EVENT FILTER. It consists of high RPRF\*,36 performance commercial proc organized into many farms convenien on-line and off-line applications. 7,36The architecture is such that a single CPU processes one event QSG]LHQQLH Petabyte NDVHW'/7 ARCHIVE SR*%ND*GD 7% WHUDEDMW EDMWyZ 3% SHWDEDMW EDMWyZ *,36 LQVWUXNFMLV 7,36 LQVWUXNFMLV
16 '\VWU\EXWRU '\VWUXEXWRU WRJyUNDUR]U]GRZDV\VWHPX]ELHUDQLDGDQ\FK -HJR]DGDQLHPMHVW]HEUDQLHGDQ\FKGRW\F]F\FK GDQHJRSU]\SDGNX]HZV]\VWNLFKF]FLGHWHNWRUD LSU]HVáDQLHLFKGRRNUHORQHJRSURFHVRUD PRGXá\RGF]\WXUy*Q\FKF]FLGHWHNWRUD IDUPDSURFHVRUyZ SU]HSXVWRZRü *LJDELWV MHVWUyZQRZD*QDLORFLGDQ\FKSU]HV\áDQ\FKSU]H]FDá G]LVLHMV]WHOHNRPXQLNDFMHXURSHMVN
17 (ZROXFMDV\VWHPyZ]ELHUDQLDGDQ\FK (1 MHz) el-1 F]VWRü e WU\JHUD (Hz) >+]@ LHCB 10 5 F]VWRü WU\JHUD 0+] ATLAS CMS High OLF]EDNDQDáyZ No. Channe SU]HSXVWRZRü High Bandwidth *ELWV ( 500 Gbit/s) KLOE HERA-B H1 ZEUS CDF ALICE High LORü Data Archive GDQ\FK (PetaByte) SHWDEDMW\ 10 2 NA Event Size (byte UR]PLDUSU]\SDGNX>EDMW@,ORü GDQ\FK SU]HSá\ZDMF\FK SU]H] V\VWHP RGF]\WX &06 Z FLJX PLQXW SUDF\ /+& MHVW SRUyZQ\ZDOQD ]FDáRFL GDQ\FK SU]HVáDQ\FK SU]H] ZV]\VWNLH VLHFL Z &(51LHZFLJXFDáHJRURNX
18 5R]ZyMWHFKQRORJLL Gbit MEMORIES MIPS CPU POWER DISK RISC 1 DRAM SRAM Year Ggate TECHNOLOGY Gate/Chip µm MByte/s MIPS Year DATA ACQUISITION DAQ MIPS Technology Rates Mbyte/s 0.12 Year SPS 70' SPSC 80' LEP 90' DESY 90' TEV 00' LHC 04' 0RFREOLF]HQLRZDSURFHVRUyZZ]UDVWDUD]\FRODW 3RMHPQRüSDPLFLZ]UDVWDUD]\FRODWD &DáDPRFREOLF]HQLRZD&(51XZURNXE\áD PQLHMV]DQL*MHGQHJRZVSyáF]HVQHJRNRPSXWHUD RVRELVWHJR
19 +DUPRQRJUDPSUDF SURMHNWWHFKQLF]Q\ RFHQDGRVWSQ\FKWHFKQRORJLL WHVW\SURWRW\SyZ Z\EyUWHFKQRORJLL LILQDOQDVSHF\ILNDFMD SURGXNFMDLWHVW\ LQVWDODFMD URN 6NDODSU]HGVLZ]LFLDZ\PDJDDE\SURMHNWWHFKQLF]Q\ E\áJRWRZ\QDODWSU]HGXUXFKRPLHQLHP HNVSHU\PHQWX $E\ XU]G]HQLH QLH E\áR SU]HVWDU]DáH MX* ZPRPHQFLH RGGDQLD GR X*\WNX Z F]DVLH SURMHNWRZDQLD QDOH*\ SU]HZLG]LHüLXZ]JOGQLüPR*OLZ\UR]ZyMWHFKQRORJLL &Dá\V\VWHPZ\]ZDODQLDL]ELHUDQLDGDQ\FK&06]DZLHUD SRQDGPRGXáyZHOHNWURQLF]Q\FK -H*HOLPRGXáSVXáE\VLUHGQLRUD]QDODWDFRG]LHQQLH QDOH*DáRE\Z\PLHQLDüPRGXáyZ
20 3RGVXPRZDQLH :VSyáF]HVQDIL]\NDF]VWHNRFLHUDVLRJUDQLFH OXG]NLHJRSR]QDQLDSUyEXMF]XQLILNRZDüZV]\VWNLH ]QDQHREHFQLHRGG]LDá\ZDQLD 3UyEDRGSRZLHG]LQDS\WDQLDSU]H]QLVWDZLDQH Z\PDJDVLJQLFLDGREDUG]RZ\VRNLFKHQHUJLL 7H9 LSRV]XNLZDQLDQLH]Z\NOHU]DGNLFK]MDZLVN σaie 3RáF]HQLHW\FKGZyFKZ\PDJDVWDQRZLZ\]ZDQLH GOD QDMQRZRF]HQLHMV]\FKWHFKQRORJLLLQIRUPDW\F]Q\FK L WHOHNRPXQLNDF\MQ\FK Z\VRNDHQHUJLD GX*DOLF]EDSURGXNRZDQ\FKF]VWHN asu]\sdghn SUHF\]\MQ\SRPLDUZV]HURNLP]DNUHVLH G\QDPLF]Q\P aµp SRV]XNLZDQLHU]DGNLFK]MDZLVN ROEU]\PLDF]VWRüRGG]LDá\ZD QDNáDGDQLHVLRGG]LDá\ZD PDá\VWRVXQHNV\JQDáXGRWáD a*+] Z\QLNDMFH]SRZ\*V]HJRZ\PDJDQLDWHFKQRORJLF]QH VWHURZDQLHSU]HSá\ZHPROEU]\PLHMLORFLGDQ\FK *ELWVV DQDOL]DSU]\SDGNyZZF]DVLHU]HF]\ZLVW\P VHOHNFMD JLJDQW\F]QDPRFREOLF]HQLRZD VXSHUSRMHPQDSDPLüPDVRZD 7,36 3%URN
Higgs Boson Physics. Analysis Techniques. Günter Quast, Roger Wolf, Andrew Gilbert Master-Kurs SS
Higgs Boson Physics Analysis Techniques Günter Quast, Roger Wolf, Andrew Gilbert Master-Kurs SS 2015 Institut für Experimentelle Kernphysik KIT Universität des Landes Baden-Württemberg und nationales Forschungszentrum
More informationq Z0 q W W H q p p q Z0 Fig.2
Fig.1 q Z 0 p q W Z 0 H W q q p Fig.2 Fig.3 Fig.4 Fig.5 Training Quenches at 1.8K - first runs Training Quench 10.00 No Quench 9.75 9.50 Provoked Quench Magnetic Field at Quench B [Tesla] 9.25 9.00 8.75
More informationParticles and Universe: Particle detectors
Particles and Universe: Particle detectors Maria Krawczyk, Aleksander Filip Żarnecki March 31, 2015 M.Krawczyk, A.F.Żarnecki Particles and Universe 5 March 31, 2015 1 / 46 Lecture 5 1 Introduction 2 Ionization
More informationParticles and Universe: Particle detectors
Particles and Universe: Particle detectors Maria Krawczyk, Aleksander Filip Żarnecki April 12, 2016 M.Krawczyk, A.F.Żarnecki Particles and Universe 5 April 12, 2016 1 / 49 Lecture 5 1 Introduction 2 Ionization
More informationTrigger di primo livello per gli esperimenti ATLAS & CMS ad LHC
Trigger di primo livello per gli esperimenti ATLAS & CMS ad LHC F.Pastore INFN Sezione di Roma II Workshop sulla fisica di ATLAS e CMS Napoli, 13-15 Ottobre 2004 Outline LHC Physics Program Requirements
More informationThe ATLAS trigger - commissioning with cosmic rays
Journal of Physics: Conference Series The ATLAS trigger - commissioning with cosmic rays To cite this article: J Boyd 2008 J. Phys.: Conf. Ser. 119 022014 Related content - The ATLAS Level-1 Central Trigger
More information2 ATLAS operations and data taking
The ATLAS experiment: status report and recent results Ludovico Pontecorvo INFN - Roma and CERN on behalf of the ATLAS Collaboration 1 Introduction The ATLAS experiment was designed to explore a broad
More informationIdentifying Particle Trajectories in CMS using the Long Barrel Geometry
Identifying Particle Trajectories in CMS using the Long Barrel Geometry Angela Galvez 2010 NSF/REU Program Physics Department, University of Notre Dame Advisor: Kevin Lannon Abstract The Compact Muon Solenoid
More informationLHC State of the Art and News
LHC State of the Art and News ATL-GEN-SLIDE-2010-139 16 June 2010 Arno Straessner TU Dresden on behalf of the ATLAS Collaboration FSP 101 ATLAS Vulcano Workshop 2010 Frontier Objects in Astrophysics and
More informationTriggering. Example: Suppose you d like to take an exceptional photograph of the CN-tower.
Triggering Example: Suppose you d like to take an exceptional photograph of the CN-tower. Poor strategy: Take pictures continuously until your film is used up or camera memory is full Better strategy:
More informationThe ATLAS muon and tau triggers
Journal of Physics: Conference Series OPEN ACCESS The ATLAS muon and tau triggers To cite this article: L Dell'Asta and the Atlas Collaboration 2014 J. Phys.: Conf. Ser. 523 012018 View the article online
More informationLHC Detectors and their Physics Potential. Nick Ellis PH Department, CERN, Geneva
LHC Detectors and their Physics Potential Nick Ellis PH Department, CERN, Geneva 1 Part 1 Introduction to the LHC Detector Requirements & Design Concepts 2 What is the Large Hadron Collider? Circular proton-proton
More informationAlexei Safonov Lecture #18
Methods of Experimental Particle Physics Alexei Safonov Lecture #18 1 Presentations: Trigger Today Lecture D0 calorimeter by Jeff 2 Collisions at LHC 14 000 x mass of proton (14 TeV) = Collision Energy
More informationFlavour Physics at LHC
Flavour Physics at LHC ICFP2009, Hanoi, September 2009 Tatsuya Nakada LPHE/EPFL Introduction (I) There exist solid observations for physics beyond the Standard Model T. Nakada ICFP2009 Hanoi September
More informationATLAS HLT Steering. Andrey Belkin Johannes Gutenberg Universität Mainz
ATLAS HLT Steering Johannes Gutenberg Universität Mainz 36. Herbstschule für Hochenergiephysik Maria Laach, Overview ATLAS detector Trigger system Steering Performance tests Status and outlook Johannes
More informationATLAS EXPERIMENT : HOW THE DATA FLOWS. (Trigger, Computing, and Data Analysis)
ATLAS EXPERIMENT : HOW THE DATA FLOWS (Trigger, Computing, and Data Analysis) In order to process large volumes of data within nanosecond timescales, the trigger system is designed to select interesting
More information7 Physics at Hadron Colliders
7 Physics at Hadron Colliders The present and future Hadron Colliders - The Tevatron and the LHC Test of the Standard Model at Hadron Colliders Jet, W/Z, Top-quark production Physics of Beauty Quarks (T.
More informationAccelerators and Colliders
Accelerators and Colliders References Robert Mann: An introduction to particle physics and the standard model Tao Han, Collider Phenomenology, http://arxiv.org/abs/hep-ph/0508097 Particle Data Group, (J.
More informationDr. Andrea Bocci. Using GPUs to Accelerate Online Event Reconstruction. at the Large Hadron Collider. Applied Physicist
Using GPUs to Accelerate Online Event Reconstruction at the Large Hadron Collider Dr. Andrea Bocci Applied Physicist On behalf of the CMS Collaboration Discover CERN Inside the Large Hadron Collider at
More informationTrigger in ATLAS and CMS
Trigger in ATLAS and CMS Christos Leonidopoulos CERN-PH On behalf of the ATLAS and CMS collaborations LHC New Physics Signatures Workshop January 5-11, 2008, Ann Arbor What are we trying to do? Find the
More informationAtlas Status and Perspectives
Atlas Status and Perspectives Bruno Mansoulié (IRFU-Saclay) On behalf of the Topics The hot news: Heavy Ion analysis Data taking in 2010 Luminosity, Data taking & quality, trigger Detector performance
More informationLast Friday: pp(bar) Physics Intro, the TeVatron
Last Friday: pp(bar) Physics Intro, the TeVatron Today: The Large Hadron Collider (LHC) The Large Hadron Collider (LHC) 7 TeV + 7 TeV Protons Protons 10 11 Protons per bunch Bunch Crossings 4x10 7 Hz Proton
More informationA glance at LHC Detector Systems. Burkhard Schmidt, CERN PH-DT
A glance at LHC Detector Systems Burkhard Schmidt, CERN PH-DT The Enter LHC a New accelerator Era in Fundamental and the detectors Science Start-up of the Large Hadron Collider (LHC), one of the largest
More informationIntroduction of CMS Detector. Ijaz Ahmed National Centre for Physics, Islamabad
Introduction of CMS Detector Ijaz Ahmed National Centre for Physics, Islamabad Layout of my Lectures: 1) Introduction of CMS Detector 2) CMS sub-detectors 3) CMS Trigger System Contents Introduction of
More informationTriggering at the Frontier: Top Quark Physics at ATLAS
Triggering at the Frontier: Top Quark Physics at ATLAS Institutskolloquium Technisch Universität Dresden 23. April 2009 Martin zur Nedden, Humboldt-Universität zu Berlin 1 Content Open Questions The Large
More informationCMS Trigger Simulation
CMS Trigger Simulation Sridhara Dasu University of Wisconsin Outline: Calorimeter Level- Trigger Algorithms Rates and Efficiencies Physics Performance Muon Level- Trigger Algorithms Rates and Efficiencies
More information4. LHC experiments Marcello Barisonzi LHC experiments August
4. LHC experiments 1 Summary from yesterday: Hadron colliders play an important role in particle physics discory but also precision measurements LHC will open up TeV energy range new particles with 3-5
More informationThe LHCb Experiment II Detector XXXIV SLAC Summer Institute, July, 2006
The LHCb Experiment II Detector XXXIV SLAC Summer Institute, 17-28 July, 2006 Tatsuya NAKADA CERN and Ecole Polytechnique Fédérale de Lausanne (EPFL) 1) Introduction Physics requirements for the detector
More informationEfficient Implementation of High- Energy Physics Processing Using Modified Jet Reconstruction and Active Size Partitioning
Efficient Implementation of High- Energy Physics Processing Using Modified Jet Reconstruction and Active Size Partitioning Tony Gregerson University of Wisconsin Tony Gregerson, U. Wisconsin, 13 April
More informationCMS Status and the US-CMS DAQ projects
CMS Status and the US-CMS DAQ projects Ichiro Suzuki Fermi National Accelerator Laboratory KEK Seminar, 2003/03/24 1 Contents What am I talking about? Introduction What are we going to do? Physics topics
More informationRare B decays in ATLAS and CMS
Rare B decays in ATLAS and CMS University Dec. 14 th 2006 Makoto Tomoto Nagoya University on behalf of CMS and ATLAS collaborations Makoto Tomoto (Nagoya University) Outline B physics in ATLAS and CMS
More informationUpgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential
IL NUOVO CIMENTO 4 C (27) 8 DOI.393/ncc/i27-78-7 Colloquia: IFAE 26 Upgrade of ATLAS and CMS for High Luminosity LHC: Detector performance and Physics potential M. Testa LNF-INFN - Frascati (RM), Italy
More informationFirst physics with the ATLAS and CMS experiments. Niels van Eldik on behalf of the ATLAS and CMS collaborations
First physics with the ATLAS and CMS experiments Niels van Eldik on behalf of the ATLAS and CMS collaborations Content Status of the LHC and the ATLAS and CMS experiments Event production rates First physics
More informationHow and Why to go Beyond the Discovery of the Higgs Boson
How and Why to go Beyond the Discovery of the Higgs Boson John Alison University of Chicago http://hep.uchicago.edu/~johnda/comptonlectures.html Lecture Outline April 1st: Newton s dream & 20th Century
More informationStatus of the LHCb Experiment. Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001
Status of the LHCb Experiment Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001 1 P b b P Number of pp inelastic interactions in one bunch crossing (σ inelastic = 80 mb): b b correlation
More informationFuture and Prospects for Heavy Flavour Physics at LHC
15 October 2010 Future and Prospects for Heavy Flavour Physics at LHC Pascal Perret LPC Clermont On behalf of the ATLAS, CMS & LHCb Collaboration The present: Content LHC & Detector performances highlight
More informationMojtaba Mohammadi Najafabadi School of Particles and Accelerators, IPM Aban 22- IPM Workshop on Electroweak and Higgs at the LHC
Electroweak studies for the LHC Mojtaba Mohammadi Najafabadi School of Particles and Accelerators, IPM Aban 22- IPM Workshop on Electroweak and Higgs at the LHC 1 Why accelerator? We live in a cold and
More informationTHE ATLAS TRIGGER SYSTEM UPGRADE AND PERFORMANCE IN RUN 2
THE ATLAS TRIGGER SYSTEM UPGRADE AND PERFORMANCE IN RUN 2 S. Shaw a on behalf of the ATLAS Collaboration University of Manchester E-mail: a savanna.marie.shaw@cern.ch The ATLAS trigger has been used very
More informationElementary Particle Detectors and Data Handling Systems: A historical perspective
Elementary Particle Detectors and Data Handling Systems: A historical perspective Prof. Manuel Delfino, UAB and IFAE, Director of PIC Dialogues on the boundaries of knowledge: Big Data 2 Why Experimental
More informationCollider physics. Introduction Some e + e - collider physics. Hadronic machines. R(e + e - hadrons/ e + e - µ - µ + ) Z 0 and W at LEP
Collider physics Introduction Some e + e - collider physics R(e + e - hadrons/ e + e - µ - µ + ) Z 0 and W at LEP Hadronic machines Total cross sections Hard and soft collisions Triggers An example: LHCb
More informationPhysics at Hadron Colliders
Physics at Hadron Colliders Part 2 Standard Model Physics Test of Quantum Chromodynamics - Jet production - W/Z production - Production of Top quarks Precision measurements -W mass - Top-quark mass QCD
More informationRisultati dell esperimento ATLAS dopo il run 1 di LHC. C. Gemme (INFN Genova), F. Parodi (INFN/University Genova) Genova, 28 Maggio 2013
Risultati dell esperimento ATLAS dopo il run 1 di LHC C. Gemme (INFN Genova), F. Parodi (INFN/University Genova) Genova, 28 Maggio 2013 1 LHC physics Standard Model is a gauge theory based on the following
More informationCMS Trigger Simulation Sridhara Dasu University of Wisconsin
CMS Trigger Simulation Sridhara Dasu University of Wisconsin Outline: Calorimeter Level- Trigger Algorithms Rates and Efficiencies Muon Level- Trigger Algorithms Rates and Efficiencies Combined Rates Physics
More informationCommissioning of the CMS Detector
Commissioning of the CMS Detector Marina Giunta INFN Bologna On behalf of the CMS Collaboration XLIVth Rencontres de Moriond on QCD and High Energy Interactions La Thuile,14-21 March 2009 2008: very busy
More informationHow and Why to go Beyond the Discovery of the Higgs Boson
How and Why to go Beyond the Discovery of the Higgs Boson John Alison University of Chicago http://hep.uchicago.edu/~johnda/comptonlectures.html Lecture Outline April 1st: Newton s dream & 20th Century
More informationHL-LHC Physics with CMS Paolo Giacomelli (INFN Bologna) Plenary ECFA meeting Friday, November 23rd, 2012
@ HL-LHC Physics with CMS Paolo Giacomelli (INFN Bologna) Plenary ECFA meeting Friday, November 23rd, 2012 Many thanks to several colleagues, in particular: M. Klute and J. Varela Outline Where we stand
More informationChamonix XII: LHC Performance Workshop. Requirements from the experiments in Year 1*
Chamonix XII: LHC Performance Workshop Requirements from the experiments in Year 1* 3-8 March, 2003 Experiments: Foreseen Status in April 2007 Physics Reach in the First Year Requirements from the Experiments
More informationDiscovery of the W and Z 0 Bosons
Discovery of the W and Z 0 Bosons Status of the Standard Model ~1980 Planning the Search for W ± and Z 0 SppS, UA1 and UA2 The analyses and the observed events First measurements of W ± and Z 0 masses
More informationRecent Results on New Phenomena and Higgs Searches at DZERO
Recent Results on New Phenomena and Higgs Searches at DZERO Neeti Parashar Louisiana Tech University Ruston, Louisiana U.S.A. 1 Outline Motivation for DØ Run II Detector at Fermilab The Fermilab Tevatron
More informationLHC. John Huth Harvard University. 16, Aug, 05 J.Huth, NEPSR
LHC John Huth Harvard University Outline The Accelerator General purpose detectors: ATLAS, CMS Specialized detectors: ALICE, LHCb Physics Motivation Symmetry Breaking sector: Higgs, Technicolor other Standard
More informationLHCb Discovery potential for New Physics
Beam induced splash in LHCb Imperial College London LHCb Discovery potential for New Physics Introduction Physics with LHCb Flavour physics can provide unique input on the type of New Physics If we express
More informationStatus and prospects of the LHCb experiment
Status and prospects of the LHCb experiment Overview Spectrometer Vertex Detector RICH Physics Program Trigger Strategy Status and Outlook U. Straumann, Uni Zuerich Geneva, 13. April 2005 pt vs for detected
More informationb Physics Prospects For The LHCb Experiment Thomas Ruf for the LHCb Collaboration Introduction Detector Status Physics Program
b Physics Prospects For The LHCb Experiment Thomas Ruf for the LHCb Collaboration Introduction Detector Status Physics Program b Primary goal of the LHCb Experiment Search for New Physics contributions
More informationFlavor Physics beyond the SM. FCNC Processes in the SM
Flavor Physics beyond the SM 48 FCNC Processes in the SM A SM ( B ΔF = ΔF = 1 W q W b b u, c, t q b u, c, t q 0 q B ) ~ ( V V 0 q ) tb tq g m 16π m t W A SM ( b q) = V V tb tq g 16π m m t W FCNC in SM
More informationThe ATLAS Silicon Microstrip Tracker
9th 9th Topical Seminar on Innovative Particle and Radiation Detectors 23-26 May 2004 Siena3 The ATLAS Silicon Microstrip Tracker Zdenek Dolezal, Charles University at Prague, for the ATLAS SCT Collaboration
More informationCMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS NOTE 22/? The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-2 GENEVA 23, Switzerland xxxx Study of a High Level b-trigger selection of
More informationNon-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC
WDS'12 Proceedings of Contributed Papers, Part III, 142 146, 212. ISBN 978-8-7378-226-9 MATFYZPRESS Non-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC I. Chalupková, Z.
More informationHiggs Searches at CMS
Higgs Searches at CMS Ashok Kumar Department of Physics and Astrophysics University of Delhi 110007 Delhi, India 1 Introduction A search for the Higgs boson in the Standard Model (SM) and the Beyond Standard
More informationStatus of the LHCb experiment and minimum bias physics
Status of the LHCb experiment and minimum bias physics Sebastian Bachman Heidelberg University on behalf of the LHCb collaboration 6/19/2010 Sebastian Bachmann 1 Beauty and Charm at the LHC LHC is a factory
More informationPhysics with Jets at the LHC
XXXIV Int. Symp. on Multiparticle Dynamics, Sonoma County, July 29, 2004 ISMD Rohlf p.1/50 Physics with Jets at the LHC Jim Rohlf Boston University Outline Introduction Detectors and expected performance
More informationFuture prospects for the measurement of direct photons at the LHC
Future prospects for the measurement of direct photons at the LHC David Joffe on behalf of the and CMS Collaborations Southern Methodist University Department of Physics, 75275 Dallas, Texas, USA DOI:
More informationIntroduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production.
Introduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production. Early discoveries? Conclusions. 2 First collisions
More informationWalter Hopkins. February
B s µ + µ Walter Hopkins Cornell University February 25 2010 Walter Hopkins (Cornell University) Bs µ + µ February 25 2010 1 / 14 Motivation B s µ + µ can only occur through higher order diagrams in Standard
More informationTriggering on Long-lived neutral particles in ATLAS
Triggering on Long-lived neutral particles in ATLAS Our theoretical friends tell us that many extensions of the Standard Model that address the hierarchy problem contain new sectors These new sectors decouple
More informationThe Collider Detector at Fermilab. Amitabh Lath Rutgers University July 25, 2002
The Collider Detector at Fermilab Amitabh Lath Rutgers University July 25, 2002 What is Fermilab? A user facility with the Tevatron: 4 mile ring with superconducting magnets. Collides protons with antiprotons.
More informationEarly physics with the LHCb detector
XXVIII PHYSICS IN COLLISION - Perugia, Italy, June, 25-28, 2008 Early physics with the LHCb detector Dirk Wiedner CERN for the LHCb collaboration 27 June 2008 Dirk Wiedner at PIC2008 Perugia 1 Outline
More informationDario Barberis. Physics with 2 nd Generation Pixel Detectors. Pixel 2002, Carmel (Ca), Sept Dario Barberis Genova University/INFN 1
Dario Barberis Physics with 2 nd Generation Pixel Detectors Pixel 2002, Carmel (Ca), Sept. 2002 Dario Barberis Genova University/INFN 1 Pixel Detector Evolution First generation (developed in early 90
More informationHiggs Searches and Properties Measurement with ATLAS. Haijun Yang (on behalf of the ATLAS) Shanghai Jiao Tong University
Higgs Searches and Properties Measurement with ATLAS Haijun Yang (on behalf of the ATLAS) Shanghai Jiao Tong University LHEP, Hainan, China, January 11-14, 2013 Outline Introduction of SM Higgs Searches
More informationATLAS Run 2 Higgs Prospects
ATLAS Run 2 Higgs Prospects Jessica Levêque LAPP Annecy-le-Vieux CNRS/IN2P3 on behalf of The ATLAS Collaboration Outline ATLAS Upgrades during LS1 ATLAS readiness First physics results with Run 2 data
More informationChapter 2 The CMS Experiment at the LHC
Chapter 2 The CMS Experiment at the LHC The Large Hadron Collider (LHC) [1] is designed to collide proton beams at a center-of-mass energy of s = 14 TeV and a nominal instantaneous luminosity of L = 10
More informationYear- 1 (Heavy- Ion) Physics with CMS at the LHC
Year- 1 (Heavy- Ion) Physics with CMS at the LHC Edwin Norbeck and Yasar Onel (for the CMS collaboration) University of Iowa For the 26 th Winter Workshop on Nuclear Dynamics Ocho Rios, Jamaica 8 January
More informationA Search for the Higgs
A Search for the Higgs The Four Muon Channel Author: Alexander Burgman Supervisor: Oxana Smirnova Division of Particle Physics Lund University Content Background Facts Some theoretical background Machines
More informationThe ATLAS C. Gemme, F.Parodi
The ATLAS Experiment@LHC C. Gemme, F.Parodi LHC physics test the Standard Model, hopefully find physics beyond SM find clues to the EWK symmetry breaking - Higgs(ses)? Standard Model is a gauge theory
More informationA-Exam: The Rare B s µ + µ decay and tanβ
A-Exam: The Rare B s µ + µ decay and tanβ Walter Hopkins Physics Department, Cornell University. The rare B decay of B s µ + µ is a promising decay channel to find beyond the Standard Model (BSM) physics
More informationLight Charged Higgs Discovery Potential of CMS in. A. Nikitenko, M. Hashemi, Imperial College, IPM & Sharif Univ. of Tech.
Light Charged Higgs Discovery Potential of CMS in the H ± τν Decay A. Nikitenko, M. Hashemi, Imperial College, IPM & Sharif Univ. of Tech. London Tehran Outline: Signal and background identification Signal
More informationLuminosity measurement at LHC
Luminosity measurement at LHC Corsi di Dottorato congiunti BO-FE-PD Corso di Fisica delle Alte Energie Aprile 2012 Per Grafstrom CERN Che cosa è la luminosita? Organizzazione Perche misurare la luminosita?
More informationATLAS Level-1 trigger studies for the invisibly decaying Higgs boson produced in vector boson fusion
ATLAS Level-1 trigger studies for the invisibly decaying Higgs boson produced in vector boson fusion Guilherme Nunes Hanninger Markus Schumacher (Uni Siegen) Maria Laach, Sept. 2007 Invisibly decaying
More informationPoS(HCP2009)042. Status of the ALICE Experiment. Werner Riegler. For the ALICE Collaboration. CERN
Status of the ALICE Experiment CERN E-mail: Werner.Riegler@cern.ch For the ALICE Collaboration ALICE is a general-purpose heavy-ion experiment designed to study the physics of strongly interacting matter
More informationRecent CMS results on heavy quarks and hadrons. Alice Bean Univ. of Kansas for the CMS Collaboration
Recent CMS results on heavy quarks and hadrons Alice Bean Univ. of Kansas for the CMS Collaboration July 25, 2013 Outline CMS at the Large Hadron Collider Cross section measurements Search for state decaying
More informationPHYS 5326 Lecture #23
PHYS 5326 Lecture #23 Monday, Apr. 21, 2003 Dr. Backgrounds to Higgs Searches Requirement on Experiments for Higgs Searches 1 Announcement Semester project presentation 1:00 4:00pm, Wednesday, May 7 in
More informationA search for heavy and long-lived staus in the LHCb detector at s = 7 and 8 TeV
A search for heavy and long-lived staus in the LHCb detector at s = 7 and 8 TeV Trần Minh Tâm minh-tam.tran@epfl.ch on behalf of the LHCb Collaboration LHCb-CONF-2014-001 EPFL, Laboratoire de Physique
More informationPhysics potential of ATLAS upgrades at HL-LHC
M.Testa on behalf of the ATLAS Collaboration INFN LNF, Italy E-mail: marianna.testa@lnf.infn.it ATL-PHYS-PROC-207-50 22 September 207 The High Luminosity-Large Hadron Collider (HL-LHC) is expected to start
More informationREADINESS OF THE CMS DETECTOR FOR FIRST DATA
READINESS OF THE CMS DETECTOR FOR FIRST DATA E. MESCHI for the CMS Collaboration CERN - CH1211 Geneva 23 - Switzerland The Compact Muon Solenoid Detector (CMS) completed the first phase of commissioning
More informationSearch for the Higgs at the LHC
Search for the Higgs at the LHC 1. The Large Hadron Collider 2. The General Purpose Detectors 3. Tools and Algorithms 4. Search for the SM Higgs 5. Search for the Supersymmetric Higgs 6. Conclusions Tejinder
More informationSearches for new Physics at HERA
Peter Schleper, Hamburg University LHC 2008 Searches at HERA 1 Searches for new Physics at HERA HERA data & experiments Model independent Search Single top & lepton + P T,miss Supersymmetry Contact Interactions
More informationModern experiments - ATLAS
Modern experiments - ATLAS, paula.eerola [at] hep.lu.se,, 046-222 7695 Outline Introduction why new experiments? The next generation of experiments: ATLAS at the Large Hadron Collider Physics basics luminosity,
More informationZ boson studies at the ATLAS experiment at CERN. Giacomo Artoni Ph.D Thesis Project June 6, 2011
Z boson studies at the ATLAS experiment at CERN Giacomo Artoni Ph.D Thesis Project June 6, 2011 Outline Introduction to the LHC and ATLAS ((Very) Brief) Z boson history Measurement of σ Backgrounds Acceptances
More informationALICE Commissioning: Getting ready for Physics
ALICE Commissioning: Getting ready for Physics Christian Lippmann, CERN for the ALICE Collaboration Moriond QCD and High Energy Interactions March 14th - March 21st 2009 1 Outline Introduction to ALICE
More informationATLAS-CONF October 15, 2010
ATLAS-CONF-2010-096 October 15, 2010 Data-driven background estimation for the H τ + τ τ h search at 7 TeV with the ATLAS detector Ian Howley 7 December 2010 1 Motivation One of the primary LHC physics
More informationPERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2
PERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2 M.M. Morgenstern On behalf of the ATLAS collaboration Nikhef, National institute for subatomic physics, Amsterdam, The Netherlands E-mail: a marcus.matthias.morgenstern@cern.ch
More informationATLAS Searches for Higgs Bosons Beyond the Standard Model
ATLAS Searches for Higgs Bosons Beyond the Standard Model Trevor Vickey University of the Witwatersrand, South Africa University of Oxford, United Kingdom on behalf of the ATLAS Collaboration July 28,
More informationLHCb Status and Physics
LHCb Status and Physics Tatsuya Nakada CERN and EPFL SUSY in 2010 s 20-22.06.07, Sapporo 1 1) Introduction Contents 2) LHC(b) Experiments 3) Physics with 2008 data 4) Flavour Physics >2008 also ATLAS/CMS
More informationBoosted searches for WW/WZ resonances in
Boosted searches for WW/WZ resonances in the lνj final state BILLIE LUBIS COLUMBIA UNIVERSITY REU 2016 CERN Founded in 1954 by 12 Western European countries Now 22 member countries Aims to conduct cutting-edge
More informationPhysics at the LHC. Academic Training, Part 3: Experiment and Standard Model
Physics at the LHC Academic Training, Part 3: Experiment and Standard Model Dr. Sven Moch, DESY Zeuthen (Theory) Dr. (Experiment) June 2007 DESY Zeuthen, based on a lecture in WS 06/07 at Humboldt University
More informationSome studies for ALICE
Some studies for ALICE Motivations for a p-p programme in ALICE Special features of the ALICE detector Preliminary studies of Physics Performances of ALICE for the measurement of some global properties
More informationLHC experiment. Summer student lectures, DESY Zeuthen 2011 Elin Bergeaas Kuutmann. DESY summer student lectures 25 July 2011
LHC experiment. Summer student lectures, DESY Zeuthen 2011 Elin Bergeaas Kuutmann 1 Some recent news... Presented at the EPS conference, Friday 22 July Is this a discovery of the Higgs boson? If not, what
More informationThe long road to understanding LHC data
The long road to understanding LHC data Philip Bechtle January 15th and 22nd 2010 P. Bechtle: The long road to understanding LHC data SFB Lecture 01/2010 1 Disclaimer I m by far not an expert on all of
More informationLHCb status. Raluca Mureşan EPFL. p.1/20
LHCb status Raluca Mureşan EPFL p.1/20 Disclaimer too many things going on 8 meetings to attend per week, days with over 100 e-mails very dinamic evolution - the most of the plots shown in a meeting are
More informationLuminosity measurement and K-short production with first LHCb data. Sophie Redford University of Oxford for the LHCb collaboration
Luminosity measurement and K-short production with first LHCb data Sophie Redford University of Oxford for the LHCb collaboration 1 Introduction Measurement of the prompt Ks production Using data collected
More informationStatus and Performance of the ATLAS Experiment
Status and Performance of the ATLAS Experiment P. Iengo To cite this version: P. Iengo. Status and Performance of the ATLAS Experiment. 15th International QCD Conference (QCD 10), Jun 2010, Montpellier,
More information