The Alice Experiment Felix Freiherr von Lüdinghausen

Similar documents
The ALICE Experiment Introduction to relativistic heavy ion collisions

ALICE A Large Ion Collider Experiment

ALICE Commissioning: Getting ready for Physics

PoS(HCP2009)042. Status of the ALICE Experiment. Werner Riegler. For the ALICE Collaboration. CERN

ALICE Detector Status and Commissioning

Heavy Ion Physics Program of CERN: Alice Setup at LHC.

Charged particle multiplicity in proton-proton collisions with ALICE

Particle Detectors A brief introduction with emphasis on high energy physics applications

Federico Antinori (INFN Padova, Italy) on behalf of the ALICE Collaboration

V0 cross-section measurement at LHCb. RIVET analysis module for Z boson decay to di-electron

Charged Particle Production in Proton-Proton Collisions at s = 13 TeV with ALICE at the LHC

Measurements of the dilepton continuum in ALICE. Christoph Baumann Resonance Workshop, Austin

Particle identification at LHC: Alice and LHCb

The ALICE experiment at LHC. Experimental conditions at LHC The ALICE detector Some physics observables Conclusions

ALICE status and early physics prospects. Jean-Pierre Revol The 9 th ICFA seminar Stanford Linear Accelerator Center October 28-31, 2008

Progress of the ALICE experiment

ALICE status and first results

First Run-2 results from ALICE

EP228 Particle Physics

Transverse momentum spectra of identified charged hadrons with the ALICE detector in Pb-Pb collisions at the LHC

Photon and neutral meson production in pp and PbPb collisions at ALICE

High Momentum Particle IDentification (HMPID) in ALICE. Pusan National University In-Kwon Yoo For ALICE / HMPID Collaboration

Recent CMS results on heavy quarks and hadrons. Alice Bean Univ. of Kansas for the CMS Collaboration

Prospective of gamma hadron correlation. study in CMS experiment

Heavy Ion Experiments at

Early physics with ALICE

Heavy Ion Results from the ALICE Experiment

Francesco Barile for the ALICE Collaboration. Università degli Studi di Bari & INFN

The Quark-Gluon Plasma and the ALICE Experiment

D + analysis in pp collisions

Central Meson Production in ALICE

ALICE results on ultraperipheral Pb+Pb and p+pb collisions

The achievements of the CERN proton antiproton collider

In-Medium Energy Loss and Correlations in Pb-Pb Collisions at 2.76 TeV with ALICE

Analyses of the anisotropic flow in Pb-Pb collisions at s NN =2.76 TeV

Information about the T9 beam line and experimental facilities

ATLAS EXPERIMENT : HOW THE DATA FLOWS. (Trigger, Computing, and Data Analysis)

Physics sources of noise in ring imaging Cherenkov detectors

Susanna Costanza. (Università degli Studi di Pavia & INFN Pavia) on behalf of the ALICE Collaboration

IKF. H-QM Quark Matter Studies. Quarkonia Measurements with ALICE. Frederick Kramer. WWND, Ocho Rios, Jan 8, IKF, Goethe-Universität Frankfurt

Particle Detectors. Summer Student Lectures 2007 Werner Riegler, CERN, History of Instrumentation History of Particle Physics

The Fast Interaction Trigger Upgrade for ALICE

Year- 1 (Heavy- Ion) Physics with CMS at the LHC

Theory English (Official)

Detectors in Nuclear and High Energy Physics. RHIG summer student meeting June 2014

Heavy-flavor production in pp and Pb Pb collisions at LHC with ALICE

Some studies for ALICE

7. Particle identification

The ALICE Inner Tracking System Off-line Software

Transverse momentum and pseudorapidity distributions with minimum bias events in CMS at the LHC

What detectors measure

Detectors for Particle Physics. Lecture 2: Drift detectors Muon detectors MWPC, CSC, RPC, TRT, TPC, Cherenkov

PERFORMANCE OF THE ATLAS MUON TRIGGER IN RUN 2

A Very High Momentum Particle Identification Detector for ALICE

Particles and Universe: Particle detectors

Future prospects for the measurement of direct photons at the LHC

Nuclear and Particle Physics 4b Physics of the Quark Gluon Plasma

Status of the LHCb Experiment. Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001

4. LHC experiments Marcello Barisonzi LHC experiments August

Particle Detectors for

First Run II results from ALICE

Muon reconstruction performance in ATLAS at Run-2

Quarkonium results in pp collisions from ALICE

Identifying Particle Trajectories in CMS using the Long Barrel Geometry

Detectors & Beams. Giuliano Franchetti and Alberica Toia Goethe University Frankfurt GSI Helmholtzzentrum für Schwerionenforschung

The Upgrade of the ALICE Experiment at LHC

Recent results in proton-lead collisions with ALICE at the LHC from RUN 2012 and 2013

2 ATLAS operations and data taking

TRIGGER EFFICIENCIES AND DIFFRACTION IN ALICE

PHY492: Nuclear & Particle Physics. Lecture 25. Particle Detectors

Particle Energy Loss in Matter

7 Physics at Hadron Colliders

The physics programme of the ALICE experiment at the LHC

arxiv: v1 [nucl-ex] 29 Feb 2012

The first Z boson measurement in the dimuon channel in PbPb collisions at s = 2.76 TeV at CMS

LHC Detectors and their Physics Potential. Nick Ellis PH Department, CERN, Geneva

arxiv: v1 [hep-ex] 9 Jan 2019

A NEW TECHNIQUE FOR DETERMINING CHARGE AND MOMENTUM OF ELECTRONS AND POSITRONS USING CALORIMETRY AND SILICON TRACKING. Qun Fan & Arie Bodek

Particle Identification: Computer reconstruction of a UA1 event with an identified electron as a candidate for a W >eν event

The HARP Experiment. G. Vidal-Sitjes (INFN-Ferrara) on behalf of the HARP Collaboration

EVENT BY EVENT PHYSICS IN ALICE

PoS(HIGH-pTLHC)022. The VHMPID detector in the ALICE experiment at LHC. Giacomo Volpe. INFN Bari, Italy

Open-charm and J/ψ production at the ALICE experiment

ALICE results on identified particle spectra in p-pb collisions

Tracking at the LHC. Pippa Wells, CERN

Measurement of W-boson production in p-pb collisions at the LHC with ALICE

A progress report on the development of the CsI-RICH detector for the ALICE experiment at LHC

7 Particle Identification. Detectors for Particle Physics Manfred Krammer Institute of High Energy Physics, Vienna, Austria

Performance of the ALICE Muon Trigger system in Pb Pb collisions

TRIGGER EFFICIENCIES AND DIFFRACTION IN ALICE.

Particles and Universe: Particle detectors

Measurement of light mesons at RHIC by the PHENIX experiment

Validation of Geant4 Physics Models Using Collision Data from the LHC

Heavy Ion physics with the ALICE experiment at the CERN LHC

arxiv: v1 [physics.ins-det] 3 Dec 2018 Fast Interaction Trigger for the upgrade of the ALICE experiment at CERN: design and performance

CLAS12 at Jefferson Lab

Photon Physics in ALICE from conversion electrons

Experimental Particle Physics

Electromagnetic Calorimeter Calibration: Getting Rid of the Trash

HARP a hadron production experiment. Emilio Radicioni, INFN for the HARP collaboration

Transcription:

The Alice Experiment Felix Freiherr von Lüdinghausen

Alice, who is Alice? Alice is A Large Ion Collider Experiment. Worldwide hit in 1977 for the band Smokie Alice is the dedicated heavy ion experiment at the LHC. 25.11.2010 Alice 2

Where is Alice? 25.11.2010 Alice 3

The home of Alice This is the former magnet of the L3 experiment at the LEP and now the home of the Alice detectors at the LHC. It provides a magnetic field of 0.5 tesla. 25.11.2010 Alice 4

What is Alice made of? Size: 16x 16x 25m³ Weight: 1000t 25.11.2010 Alice 5

What kind of detector's exist? 25.11.2010 Alice 6

Where is the ITS? 25.11.2010 Alice 7

What is the ITS? The Inner Tracking System is the vertex detector of Alice. It consists of the Silicon Pixel Detector (SPD), Silicon Drift Detector (SDD) and Silicon Strip Detector(SSD). 25.11.2010 Alice 8

What is the ITS? Silicon Pixel Detector (SPD): 3.3M channels first layer + 6.6M channels second layer Silicon Drift Detector (SDD): 43k channels first layer + 90k channels second layer Busy time: ~800μs Samplerate: ~1kHz for whole Alice Detector Silicon Strip Detector(SSD): 1.1M channels first layer + 1.5M channels second layer All three detectors together have a total area of 6,74m². 25.11.2010 Alice 9

What is the ITS doing? Vertex finding in the ITS for an event of a Proton-Proton collision. 25.11.2010 Alice 10

ITS performance 25.11.2010 Alice 11

Where are the Forward Detectors? 25.11.2010 Alice 12

What are the Forward Detectors: FMD, T0, V0? FMD: five rings of silicon strip detectors T0: Two arrays of Cherenkov radiators + detectors V0: Two rings of plastic scintillators Part of Level 0 trigger multiplicity information in forward and backward regions ( η > 1.5) 25.11.2010 Alice 13

Where is the TPC? 25.11.2010 Alice 14

What is the TPC? The Time Projection Chamber is the main tracking device in Alice, which is also used for particle identification. It consist of two chambers with 2,5 m length and 2,8 m radius, which have together a volume of 88m³ filled with a gas micture of 90% argon and 10% carbon-dioxide. 25.11.2010 Alice 15

What is the TPC? 570132 pads in total Drift length: 2,5m Drift velocity 2,7cm/μs Resolution in z: 1100μm ~90μs drift time over the detector length-> ~11kHz 25.11.2010 Alice 16

TPC performance Betheblochformula 25.11.2010 Alice 17

Where is the TRD? 25.11.2010 Alice 18

What is the TRD? The Transition Radiation Detector is the main electron detector in Alice. It will cover a total area of ~736m² in six layers with 1.12 Mio channels when completly installed. The chambers are filled with a gas mixture of 85% Xenon and 15% carbon-dioxide. Size: 7m length x 3,7m radius 25.11.2010 Alice 19

What is the TRD? Electrons and pions are distinguished by the additional Signal from the transition radiation at the end of the pulse. Drift velocity: 1.6cm/μs, timebin: 0.1μs 25.11.2010 Alice 20

TRD performance Here is shown the difference in rejecting pions in the TOFspectra with the TRD compared to without the TRD at 2 GeV/c. 25.11.2010 Alice 21

Where is the TOF? 25.11.2010 Alice 22

What is the TOF? The Time of Flight detector is dedicated to charged particle identification over a very large part of phase space and a rapidity acceptance from 0.5 GeV/c to 2.5 GeV/c with an timeresolution of less than 120 ps, it's radius is roughly 4m. 25.11.2010 Alice 23

What is the TOF? The TOF is coupled with the T0 detector as start trigger and the TOF for the stop signal. While being a gas detector the TOF is not a drift chamber to it's need of high time resolution (~100ps). 25.11.2010 Alice 24

TOF performance 25.11.2010 Alice 25

Where is the HMPID? 25.11.2010 Alice 26

What is the HMPID? The High Momentum Particle Identification detector enhances the PID capability of ALICE beyond the momentum range allowed by ITS, TPC and by the TOF to the range of: up to 3 GeV/c for p and K up to 5 GeV/c for p (on a track-by-track basis) 25.11.2010 Alice 27

What is the HMPID? Cherenkov photons, emitted in the layer of liquid C6F14, are detected by a photon counter onto the pad cathode of a multiwire proportional chamber (MWPC). 25.11.2010 Alice 28

Where is the EMCAL? 25.11.2010 Alice 29

What is the EMCAL? The Electro Magnetic Calorimeter consists out of Pb-scintillators, it's main function is the study of jet quenching (interaction of energetic partons with dense matter). 25.11.2010 Alice 30

Where is the PHOS? 25.11.2010 Alice 31

What is the PHOS? The Photon Spectrometer is used for detection of high energetic photons. It consists of 3584 Leadtungsten crystals which work as calorimeter and cover an area of ~8m². 25.11.2010 Alice 32

Where is the Muon arm? 25.11.2010 Alice 33

What is the Muon arm? The muon spectrometer covers a pseudo-rapidity from -4 < η < -2.5, which corresponds to an polar angular of 171-178. Due to the large Absorber needed to reduce the flux of hadrons only muons with momenta above 4GeV/c could be detected. 25.11.2010 Alice 34

Where is the PMD? 25.11.2010 Alice 35

What is the PMD? The Photon Multiplicity Detector is a forward detector on the opposite side of the Muon arm. It provides charged-particle multiplicity information in the pseudo-rapidity range from -3.4 < η < -1.7 and 1.7 < η < 5. 25.11.2010 Alice 36

Where is the ZDC? 25.11.2010 Alice 37

What is the ZDC? The Zero Degree Calorimeters are used to mesure the energy of the spectator nucleons to determine the centrality of the event. They are located 115 meters away from the interaction point on both sides along the beam line. The ZDCs are made by a stack of heavy metal plates grooved to allocate a matrix of quartz fibres. 25.11.2010 Alice 38

What is this all good for? 25.11.2010 Alice 39

Eventdisplay LHC10e run 130844 In the Eventdisplay you can see all the detected signals combined into tracks with particle-identification, charge, mass, impulse and so on. Than this is used for analysis over a huge number of events by just applying cuts, filters and special criterias just like needed. 25.11.2010 Alice 40

Eventdisplay LHC10e run 130844 25.11.2010 Alice 41

Short look at heavy ions 25.11.2010 Alice 42

Short look at heavy ions 25.11.2010 Alice 43

Centrality in Pb-Pb 25.11.2010 Alice 44

dnch/dη in central Pb-Pb at 2.76Tev dnch/dη = 1584 ± 4 (stat.) ± 76 (syst.) Correction for detector acceptance: dn ch dn = 1 tracklet, with = 2 ; = 0.14 d d 25.11.2010 Alice 45

Bibliography The Alice Experimen at the CERN LHC(http://iopscience.iop.org) Alice Status Report 17.11.2010, Andrea Dainese (http://indico.cern.ch) Physics Performance Report, Volume I+II (http://iopscience.iop.org) http://www.lhc-facts.ch/index.php?page=alice 25.11.2010 Alice 46