March 3, 2008E. Scapparone INSTR081 Particle identification in ALICE E. Scapparone(INFN/CERN) on behalf of the ALICE Collaboration INSTR08, March 3, 2008.

Slides:



Advertisements
Similar presentations
Charm and beauty with ALICE at LHC
Advertisements

CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Dielectron Physics with ALICE Transition Radiation Detector (TRD) Prashant Shukla (for the ALICE TRD Collaboration) Institute of Physics University of.
CMS Heavy Ion Physics Edwin Norbeck University of Iowa.
THE ALICE EXPERIMENT AT CERN LHC: STATUS AND FIRST RESULTS Ermanno Vercellin Università and INFN Torino, Italy On behalf of the ALICE collaboration Outline.
Centauro and STrange Object Research (CASTOR) - A specialized detector system dedicated to the search for Centauros and Strangelets in the baryon dense,
June Physics Performance of ALICE Overview The LHC as Ion collider SPS-RHIC-LHC Global properties in the LHC regime ALICE and its experimental strategy.
Jorge Mercado - I3HP Topical Workshop - St. Andrews The ALICE Transition Radiation Detector (TRD) Read-Out Electronics J. Mercado Physikalisches.
Mini Bang at Big Accelerators Prashant Shukla Institute of Physics University of Heidelberg Presentation at ISA, 30 January 2005, Heidelberg, Germany.
Direct photon measurement at LHC and Korean strength Y. Kwon, J. H. Kang (Yonsei University)
04/11/2008Lijuan Ruan (WWND2008)1 Prototype Performance of Novel Muon Telescope Detector at STAR Outline: Motivation Simulation Intrinsic timing and spatial.
ALICE EMCal Physics and Functional Requirements Overview.
1 ALICE at LHC: getting ready for Physics Christian W. Fabjan, CERN for the ALICE Collaboration Quark Matter 2008, Jaipur
General Trigger Philosophy The definition of ROI’s is what allows, by transferring a moderate amount of information, to concentrate on improvements in.
Cynthia HadjidakisTerzo Convegno sulla Fisica di ALICE Detection of photons and electrons in EMCAL Photons, Electrons and  0 at large p T Identification.
The Physics Potential of the PHENIX VTX and FVTX Detectors Eric J. Mannel WWND 13-Apr-2012.
The BTeV Tracking Systems David Christian Fermilab f January 11, 2001.
THE PHYSICS OF THE ALICE INNER TRACKING SYSTEM Elena Bruna, for the ALICE Collaboration Yale University 24 th Winter Workshop on Nuclear Dynamics, South.
JSPS Research Fellow / University of Tsukuba T. Horaguchi Oct for HAWAII /10/15HAWAII
Sean Kelly, QWG 9/03 Prospects for Quarkonia Physics In Media at the LHC.
Photon physics in ALICE Y.Kharlov D.Peressounko IHEP RRC “Kurchatov Institute” for the ALICE collaboration and.
1 OPEN HEAVY FLAVOUR PRODUCTION IN pp COLLISIONS WITH AT LHC Rosa Romita ( ) for the ALICE Collaboration.
First Physics at the LHC ALICE Bjørn S. Nilsen Creighton University.
Heavy flavour capabilities with the ALICE TRD Benjamin Dönigus ISNP 2008 Erice/Sicily.
LICE The ALICE detector A LargeIonColliderExperiment Gert-Jan Nooren Bachelor Introduction 10 February 2010.
EMCal in ALICE Norbert Novitzky 1. Outline How Electro-Magnetic Calorimeters works ? Physics motivation – What can we measure with Emcal ? – Advantages.
Tracking, PID and primary vertex reconstruction in the ITS Elisabetta Crescio-INFN Torino.
8/18/2004E. Monnier - CPPM - ICHEP04 - Beijing1 Atlas liquid argon calorimeter status E. Monnier on behalf of the Atlas liquid argon calorimeter group.
The 21st International Conference on Ultrarelativistic nucleus-nucleus collisions, March 30 – April 4, Knoxville, TN Results from cosmics and First LHC.
The ALICE Experiment at the CERN LHC P. Kuijer for the Alice collaboration ICHEP 2002.
Prospects in ALICE for  mesons Daniel Tapia Takaki (Birmingham, UK) for the ALICE Collaboration International Conference on STRANGENESS IN QUARK MATTER.
Roberto Barbera (Alberto Pulvirenti) University of Catania and INFN ACAT 2003 – Tsukuba – Combined tracking in the ALICE detector.
Future Possibilities for Measuring Low Mass Lepton Pairs in Christine Aidala for the Collaboration Quark Matter 2002, Nantes.
Particle Identification. Particle identification: an important task for nuclear and particle physics Usually it requires the combination of informations.
Particle ID in ALICE Silvia Arcelli Centro Studi E.Fermi and INFN For the ALICE Collaboration 5 July 2005 Workshop of Hadron Collider Physics, HCP05, Le.
The ALICE Experiment Event by Event fluctuations ALICE TOF Calibration 30th November 2007Chiara Zampolli1.
CP violation in B decays: prospects for LHCb Werner Ruckstuhl, NIKHEF, 3 July 1998.
Feasibility study of Heavy Flavor tagging with charged kaons in Au-Au Collisions at √s=200 GeV triggered by High Transverse Momentum Electrons. E.Kistenev,
CGEM-IT project and beam test program G. Felici for the FE-LNF-TO team Partially supported by the Italian Ministry of Foreign Affairs under the Program.
Christian Lippmann (ALICE TRD), DPG-Tagung Köln Position Resolution, Electron Identification and Transition Radiation Spectra with Prototypes.
HMPiD upgrade variant; simulation status N. Smirnov Physics Department, Yale University, May, 06. CERN visit.
Test Beam Results on the ATLAS Electromagnetic Calorimeters Lucia Di Ciaccio – LAPP Annecy (on behalf of the ATLAS LAr Group) OUTLINE Description of the.
First results from SND at VEPP-2000 S. Serednyakov On behalf of SND group VIII International Workshop on e + e - Collisions from Phi to Psi, PHIPSI11,
July 27, 2002CMS Heavy Ions Bolek Wyslouch1 Heavy Ion Physics with the CMS Experiment at the Large Hadron Collider Bolek Wyslouch MIT for the CMS Collaboration.
P.F.Ermolov SVD-2 status and experimental program VHMP 16 April 2005 SVD-2 status and experimental program 1.SVD history 2.SVD-2 setup 3.Experiment characteristics.
17 December 2009J. Schukraft1 First Physics at the LHC seen through the eyes of ALICE.
SPHENIX Mid-rapidity extensions: Additional Tracking system and pre-shower Y. Akiba (RIKEN/RBRC) sPHENIX workfest July 29,
V. Pozdnyakov Direct photon and photon-jet measurement capability of the ATLAS experiment at the LHC Valery Pozdnyakov (JINR, Dubna) on behalf of the HI.
The BTeV Pixel Detector and Trigger System Simon Kwan Fermilab P.O. Box 500, Batavia, IL 60510, USA BEACH2002, June 29, 2002 Vancouver, Canada.
Axel Drees, SUNY Stony Brook GSI, May January 15 th 2002 PHENIX Upgrade Plans for RHIC II Overview of baseline PHENIX detector Physics goals of RHIC II.
Study of Cherenkov detectors for high momentum charged particle identification in ALICE experiment at LHC Guy Paic Instituto de Ciencias Nucleares UNAM.
Particle Identification of the ALICE TPC via dE/dx
DIS 2011, Newport News, April 2011Joakim Nystrand, University of Bergen 1 Small-x and forward measurements in ALICE Joakim Nystrand University of.
Performance Evaluation for Open Charm and Beauty Measurement at LHC ALICE PID capability from λ and K s 0 measurement at LHC ALICE 筑波大学数理物質科学研究科 Kengo.
Recent Results from ALICE E. Vercellin Dipartimento di Fisica dell’Università di Torino and INFN Torino.
Design and performance of the ALICE Muon Spectrometer
ALICE Commissioning: Getting ready for Physics
Silicon Pixel Detector for the PHENIX experiment at the BNL RHIC
ALICE upgrade plans Paolo Giubellino LHCC Upgrades
Tatia Engelmore, Columbia University
STAR Geometry and Detectors
First physics from the ALICE electromagnetic calorimeters
Open heavy flavor analysis with the ALICE experiment at LHC
Instituto de Ciencias Nucleares UNAM
Simulation study for Forward Calorimeter in LHC-ALICE experiment
Muon Detector Jiawen ZHANG 16 September 2002.
Quarkonium production in p-p and A-A collisions: ALICE status report
STAR Detector Event selection and triggers Corrections to data
Quarkonium production in p-p and A-A collisions: ALICE status report
Presentation transcript:

March 3, 2008E. Scapparone INSTR081 Particle identification in ALICE E. Scapparone(INFN/CERN) on behalf of the ALICE Collaboration INSTR08, March 3, 2008 Outline - Experimental layout and status of the main subdetectors; - Detector performance; - Example of ALICE phsycs potential.

March 3, 2008E. Scapparone INSTR0822 ALICE: A Large Ion Collider Experiment at CERN-LHC Size: 16 x 26 meters Weight: 10,000 tonnes p-p (L=10 31 cm -2 s -1 ), Pb-Pb (L= cm -2 s -1 )

March 3, 2008E. Scapparone INSTR083 Life in Pb-Pb interactions was never easy…. NA49 At RHIC became harder….. ALICE simulated central event !..also more RHIC STAR

March 3, 2008E. Scapparone INSTR084 6 layers, three technologies (keep occupancy at a few % for max multiplicity) SPD: silicon pixels (0.2 m 2, two layers, 9.8 M channels) SDD: silicon drift (1.3 m 2, two layers, 133 k channels) SSD: double-sided silicon strips (4.9 m 2, two layers, 2.6 M channels ) R out =43.6 cm SPD SSD SDD ITS(Inner Tracking System) L out =97.6 cm Material Budget: ≤ 1% X 0 per layer !

March 3, 2008E. Scapparone INSTR085 Challenge: track densities at r = 4 cm (1st layer): up to 100 / cm2 SPD (0.2 m 2 ) Cell size (r  z  : 50  m x 425 µm space resolution(r  ) : 12  m space resolution(z): 100  m ITS SDD (1.3 m 2 ) cell size (r ,z): 294 x 150  m2 space resolution (r , z) : 35  m space resolution(z): 23  m SSD (4.9 m 2 ) cell size (r ,z): 95 x 4200  m2 space resolution (r  ): 20  m space resolution (z); 830  m 40 m m 75 mm 42 mm 6 chips

March 3, 2008E. Scapparone INSTR0866 Inner Tracking System ~ 10 m 2 Si detectors, 6 layers Pixels, Drift, double sided Strips Strips SSD Drift SDD Pixels Inner Silicon Tracker Pixels SPD

March 3, 2008E. Scapparone INSTR087 TPC SSD/SDD SPD

March 3, 2008E. Scapparone INSTR0888 Optimized for dN/dη ≈ 8000 l = 5 m, Ø = 5.6m, 88 m3, 570,000 channels x 500 time bins, up to 80 Mbytes/event (after 0 suppression) Features: lightweight: 3% X 0 total material for perpendicular tracks novel digital electronics (ALTRO) highly integrated, digital shaping; tail cancellation;0-suppression; Baseline restoration Powerful laser calibration system TPC Drift gas:Ne (86) / CO 2 (9.5) / N 2 (4.5) σ(dE/dx) ≈ 5.5 to 6.5 %, depending on multiplicity (measurements and simulations)

March 3, 2008E. Scapparone INSTR0899 ALICE TPC: 5 years construction

March 3, 2008E. Scapparone INSTR0810 Cosmics recorded in Commissioning with Cosmics and Laser tracks Spatial resolution and Electronics noise in experiment according to specifications Status: installed and being commissioned

March 3, 2008E. Scapparone INSTR0811 e/  separation in central barrel p>1 GeV/c fast trigger for high momentum particles (hadrons, electrons)+ tracking 540 detectors ~ 760m 2 18 super modules length: 7m X/X 0 ~ 22 % 28 m 3 Xe/CO 2 (85/15) 1.2 million channels Transition Radiation Detector (TRD) Status: partially installed; being commissioned TRD

March 3, 2008E. Scapparone INSTR0812 TRD - Signal Generation & Processing Average pulse heigth (mV)  e-) = 90 %

March 3, 2008E. Scapparone INSTR0813 TRD Installation

March 3, 2008E. Scapparone INSTR0814 TOF requirements: Large array to cover the ALICE barrel (~150 m 2 ) Time resolution σ < 100 ps High efficiency, ε > 95% High segmentation: few thousands of particles per unit of rapidity expected in Pb-Pb collision at s = 5.5 TeV/nucleon pair ALICE choice: a detector based on MRPC, segmented in ~157,000 channels, (3.5 x 2.5) cm2 area √

March 3, 2008E. Scapparone INSTR0815 TOF 2 crates /side pads, total sensitive area: ~150 m 2 18 Supermodules, each made of 5 modules: 2 external (19 strips), 2 intermediate (19 strips), 1 central (15 strips) 7.4 m Readout performed by two VME Crates/Side

March 3, 2008E. Scapparone INSTR0816 Cross section of a double-stack MRPC strip 2 rows of 48 readout pads (3.5 x 2.5 cm 2 ) Active strip length = 120 cm Differential signal to FEA card 10 gaps 250  m

March 3, 2008E. Scapparone INSTR0817 Test beam of single strips Efficiency Time resolution( ps) ε > 99.9 % average ~ 50 ps Gas mixture: C 2 F 4 H 2 (90%) – SF 6 (5%) – C 4 H 10 (5%) Similar results obtained when strips are inserted inside the modules

March 3, 2008E. Scapparone INSTR0818 M = p ((t2 c2 /L2 )-1)1/2 σ TOF = 80 ps ; B = 0.5 T

March 3, 2008E. Scapparone INSTR SMs installed ; next 4 SMs to be installed next week; being commissioned

March 3, 2008E. Scapparone INSTR0820 December 2007 cosmic run Event display of a muon crossing the TOF detector

March 3, 2008E. Scapparone INSTR0821 Proximity Focused RICH 11 m 2 active detector area 7 modules - 0.6< η < 0.6; Δφ = 58 deg CsI Photocathode read by pads Threshold momentum = 1.21* (Particle Mass) PID optimization for 1 GeV < p < 6 GeV High Momentum Particle Identifier: HMPID

March 3, 2008E. Scapparone INSTR0822 HMPID (Sept ’06) HMPID: Installed; being commissioned

March 3, 2008E. Scapparone INSTR0823 Example of a high multiplicity event as seen by the HMPID dN/d  =6000

March 3, 2008E. Scapparone INSTR stations of high granularity pad tracking chambers, over 1 million channels Complex absorber/small angle shield system (~10 I ) to minimize background (90 cm from vertex) RPC Trigger Chambers MUON spectrometer set-up  0.7 T, bending power 3 Tm  4 MW power, 800 tons  World’s largest warm dipole Trigger pt cut on single  : ~1 GeV/c

March 3, 2008E. Scapparone INSTR0825 Lepton Acceptance ATLAS & CMS present a large lepton acceptance |  |<2.4 ALICE combines muonic and electronic channels - covers the low p T region (quarkonia) - covers the forward region 2.5<  <4.0

March 3, 2008E. Scapparone INSTR0826 Charged Particle Identification ITS kaons pions protons dE/dx (MIP units) TPC All known PID techniques used in ALICE  dE/dx = 6.8% at dN/dy=8000 (5.5% for isolated tracks) HADRON-ID  3  separation power P(GeV/c) dE/dx (MIP units)

March 3, 2008E. Scapparone INSTR0827 Combined PID Performance Efficiency/Contamination Kaon PID (the most difficult case...) ITS TPC TOF(*) (120 ps) p (GeV/c) (C  : C K : C p = 0.75 : 0.15 : 0.1) Higher efficiency & Lower contamination wrt individual detectors p (GeV/c) Combined PID ITS & TPC & TOF (*) very conservative

March 3, 2008E. Scapparone INSTR0828 Extension of PID to higher momenta combining the dE/dX of TRD and TPC Combine TPC and TRD dE/dx capabilities (similar number of samples/track) to get statistical ID in the relativistic rise region 8<p<10 GeV/c

March 3, 2008E. Scapparone INSTR0829 Open Charm Detection in Hadronic Decays Mass GeV/c 2 c  =124  m ~0.55 D 0  K -  + accepted/event important also for J/  normalization

March 3, 2008E. Scapparone INSTR0830 Spectra

March 3, 2008E. Scapparone INSTR0831 Finally … ALICE is becoming reality after almost 15 years in the making 2 nd Commissioning run is going on this week. Further commissioning running until first beams, scheduled for summer 2008 All systems on track for taking first pp collisions ALICE is the general purpose Heavy Ion experiment, designed to address the very rich, expected physics program: particle id will play a central role in this challenging physics.

March 3, 2008E. Scapparone INSTR0832 RISERVE

March 3, 2008E. Scapparone INSTR0833 GIF results No ageing effect measured at PS Working voltage = 13 kV

March 3, 2008E. Scapparone INSTR0834 GIF results: No current increase Source on Source off Source on Source off I (  A) Flow = 1.4 cm 3 /s The gas going to the chamber 2 was bubbled through water for some time of the exposure

March 3, 2008E. Scapparone INSTR0835 Ageing study: Total charge = 14 mC/cm 2 Charge/event = 2 pC 7 *10 9 events /cm 50 Hz/cm 2 T= sec = 1620 days Pb-Pb run Time(min) two MRPC strips irradiated at GIF

March 3, 2008E. Scapparone INSTR0836 ALICE is taking shape All large structures are installed and integration of detector subsystems will start in August The ALICE Collaboration looks forward to first operation of LHC for the expected and the unexpected… Conclusion

March 3, 2008E. Scapparone INSTR0837 PHOton Spectrometer: PHOS PbO 4 W- crystal calorimeter for Photons, neutral mesons, 1 to > 100GeV Crystals: 2.2*2.2 cm 2, 20 X 0, APD R/O Operated at – 25 deg; 5 pe / MeV σ(E) ≈ 3%; σ(x,y) ≈ 4 mm; σ(t) ≈ 1 ns; at 1GeV < η < 0.12; Δφ = 100 deg; at R = 460 cm L0 trigger available at < 900 ns Module tested, calibrated in test beam; 1 or 2 modules to be installed in 04/08 3 rd module during 2008; Ultimately 5 modules with crystals expected by 2010

March 3, 2008E. Scapparone INSTR0838 ElectroMagnetic Calorimeter: EMCAL Pb-Scintillator em calorimeter for Jet physics in conjunction with tracking and PID Approximately opposite to PHOS -0.7 <η < 0.7; Δφ = 107 deg EM resolution σ(E) < 0.1/√E projective towers in ‘Shashlik’ geometry with APD R/O L0 trigger in < 900 ns for high-p T jets, photons, electrons Status: project approved in Dec of 12 supermodules early 2009

March 3, 2008E. Scapparone INSTR0839 Partial view of Muon chambers

March 3, 2008E. Scapparone INSTR0840 TOF Standalone PID (80 ps res. as in the PPR)