The ALICE e xperiment at LHC
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Transcript of The ALICE e xperiment at LHC
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The ALICE experiment at LHC
Domenico Di BariDipartimento Interateneo di Fisica
INFN-Bari
4th Summer School on THE PHYSICS OF LHC 14-19 jun 2010 Martignano, Grecìa Salentina (Lecce, Italy)
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P. Giubellino
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PLC 20J. Schukraft3
HI @LHC: Constraints and Solutions
Extreme particle density : dNch/dh ~ 2000 – 8000 x 500 compared to pp@LHC; x 30 compared to 32S@SPS
high granularity, 3D detectors Silicon pixels and drift detectors, TPC with low diffusion gas mixture (Ne-CO2)
conservative & redundant tracking up to ~200 space points per track
large distance to vertex e.g. emcal at 4.5 m (typical is 1-2 m !)
Large dynamic range in pt: from very soft (0.1 GeV) to fairly hard (100 GeV)
very thin detector, modest field 0.5 T (low pt), ALICE: ~ 10%X0 in r < 2.5 m (typical is 50-100%X0) vertex detector works as ‘standalone low pt spectrometer’ (tracking & PID)
large lever arm + good hit resolution (large pt) B= 0.5T, tracking L ~ 3.5m, BL2 ~ like CMS !
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PLC 20J. Schukraft4
HI @LHC: Constraints and Solutions
Both partons & hadrons matter: fragmentation (i.e. hadrons) is part of the signal, not of the problem
partons (heavy quarks): secondary vertices, lepton ID hadrons: use of essentially all known PID technologies
dE/dx, Cherenkov & transition rad., TOF, calorimeters, muon filter, topological
Modest Luminosity and interaction rates; short runs 10 kHZ (Pb-Pb), (< 1/10000 of pp@1034) ~ 1 month/year
allows slow detectors (TPC, SDD), moderate radiation hardness moderate trigger selectivity, no pipelines (mostly ‘track & hold’ electronics)
large event size (~ 100 MB) + short runs => high throughput DAQ (> 1GB/s)
Single dedicated heavy ion experimentcombine capabilities of a handful of more specialized HI expts at AGS/SPS/RHIC 18 detector technologies, several smaller ‘special purpose’ detectors (HMPID, PHOS, PMD, FMD, ZDC..) central barrel (~ STAR) + forward muon arm (~PHENIX)
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5
Detector:Size: 16 x 26 metersWeight: 10,000 tons
Collaboration:> 1000 Members> 100 Institutes > 30 countries
ALICEACORDEV0T0ZDCFMDPMD
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Are you asking me if QGP was here? I
don’t know. Please, call the CSI experts…
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AHA, AHA, here is the
Higgs!!!
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21/4/2010 28th RRB J. Schukraft8
ALICE StatusComplete: ITS, TPC, TOF, HMPID,FMD, T0, V0, ZDC, Muon arm, Acorde PMD , PHOS(3/5), DAQ
Partial installation: 7/18 TRD 4/10 EMCAL
~ 60% HLT
ALICE Detector Installation mid 2009
New (‘post Chamonix’) LHC schedule: Likely configuration until end 2011
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Material budget distribution in ALICE
Radial distance from beam line
X/X0<10% up to 250 cm
from IP
Good precision for
e/ measurement
s
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Photon convertion
point distrib. @7TeV
Actual agreement of data with MC
< 8%
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some anxious minutes waiting for collisions..
~ 16:35
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The first ‘event’ pops up in the ACR
~ 16:41
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Relief and jubilation.. Collisions in ALICE !!
.. and some celebration..~ 16:42
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‘First Physics’ in the making
After years of looking at simulated data, there was no holding back:First physics results examined,
ca 1 hour after data taking finished (284 events !)..
~ 18:00
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12/3/2010 Yale J. Schukraft15
A few days later…
TPC trackTRD track HMPID
Cherenkov Ring
Muon Spectrometer
ITS
TPC, TRD, TOF, HMPID
On 6th December, ‘stable beams’ were declared & we could switch onall ALICE detectors for the first time..
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Data Taking Summary
30/03/2010 09/04/2010 19/04/20100
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ALICE efficiency
ALICE PHYSICS RUN TIME
cum
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LHC STABLE BEAMS
efficiency (%)
>15 Million interactions
> 150 kMuon triggers
Inter. rate~ 30 – 90 Hz
Integrated Data taking efficiencysince 30.3 ~ 85%
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12/3/2010 Yale J. Schukraft17
Tracking works beautifully
Beam spot at 2.36 TeV
TPC pt spectrumPreliminary
preliminary alignment !
SPD Vertex resolution versus # tracks
Plots as shown on 18 Dec ‘LHC’ jamboree
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alignment with cosmics only
s=181 mmafter alignment
before alignment
DataMC
pT = 1 – 1.5 GeV/c
DataMC
Impact parameter DCA
pT = 1 – 1.5 GeV/c
cosmics + pp ( = 0 and π)
Getting to know ALICE: Shape
18
SPD
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21/4/2010 28th RRB J. Schukraft19Results shown on 17 Febr LHCC
PID (or 6 ways to measure Kaons)
ALICE - Work in Progress
ALICE - Work in Progress
ALICE - Work in ProgressK ® mn
ALICE Work in Progress
K0s ® pp
# 6:HMPID Cherenkov
p
K p
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12/3/2010 Yale J. Schukraft20
Plots as shown on 18 Dec ‘LHC’ jamboree
The Particle Zoo Revisited:
PDG: 1115.7 MeV
L ® pp
PDG: 497.6 MeV
K0s ® pp
PDG: 1115.7 MeV
L ® pp
… National Geographic was sort of correct..
F ® K+K- PDG: 1019.5 MeV
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21/4/2010 28th RRB J. Schukraft21W(sss) ® LK ® pp K
April 2010
More Particle Appearances
K* ® Kp
February 2010
Work in progress
h ® ® e+e- e+e-
X(ssd) ® Lp ® pp pApril 2010
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12/3/2010 Yale J. Schukraft22
Plots as shown on 18 Dec ‘LHC’ jamboree
More Particles..
p0 ® ® e+e- e+e-
p0 ® 1 < pt < 1.5 GeV
PHOS (9 m2)
X ® Lp ® pp p
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Reconstruction from conversion
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12/3/2010 Yale J. Schukraft24
Plots as shown on 18 Dec ‘LHC’ jamboree
ALICE special: Particle Identification (very important for heavy ion physics later in 2010)
15/2/2006 LHCC Status Report J. Schukraft
.. ‘lots’ of data..
ITS
‘Good pp interactions’: (rate few Hz) - 300 k : √s = 900 GeV - 30 k : √s = 2.36 TeV
TRD
Electrons
Pions
velocity v/c
TOFProtons
Kaons
Pions
all plots:preliminary calibration & alignment !
TPCNo vertex cut !
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(Anti)Nuclei
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P. Giubellino
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Event Classess = 0.9 and 2.36 TeV
Inelastic (INEL) = Single-diffractive (SD) + Double-diffractive (DD) + Non-diffractive (ND);
Non-single diffractive (NSD) = ND+DDUse measured cross sections for diffractive processes
Change MC generator fractions (SD/INEL, DD/INEL) such that they match these fractions
s = 7 TeVDiffraction is quite unknownHadron-level def. of evts to minimize model
dependenceAll events that have at least one charged primary particle
in |η| < 1: “INEL>0”27
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Physics exploitation of ALICE has started for good !
Phase 1: rediscovering the standard model(QCD in the case of ALICE)
The average number of charged particlescreated perpendicular to the beam
in pp collisions at 900 GeV is:dN/dh = 3.10 ± 0.13 (stat) ± 0.22 (syst)
This is the first (and easiest) ofmany numbers we need to (re)measure toget confidence in our detectors, tune thesimulations, study background, ....Phase 2 is still a long way to go..
last time measured at the ISR for pp
» p
National Geographic News (4 Dec.) ‘….a machine called ALICE....
found that a (!) proton-proton collision recorded on November 23 created the precise ratio
of matter and antimatter particles predicted from theory..’
submitted to EPJC 28 Nov 2009
Physics exploitation of ALICEhas started for good !
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dN/dh: comparison to exp.
NSD 2.36 TeV NSD 900 GeV INEL 900 GeVALICE preliminary 4.43 ± 0.01 ± 0.16 3.58 ± 0.01 ± 0.12 3.02 ± 0.01 ± 0.07ALICE EPJC 65 111 (2010) 3.51 ± 0.15 ± 0.25 3.10 ± 0.13 ± 0.22CMS JHEP 02 (2010) 041 4.47 ± 0.04 ± 0.16 3.48 ± 0.02 ± 0.13 UA5 Z. Phys. C33 1 (1986) 3.43 ± 0.05 ± ? 3.09 ± 0.05 ± ?
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Multiplicity distributions @ 0.9,2.36,7 TeV
0.9 TeV: consistent with UA5Fit with NBD (Negative Binomial Distrib.) ok in a limited h-regions
7 TeV: NBD fit slightly deviate at highest multiplicities
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Life starts getting interesting..Increase .9 to 2.3 TeV (%) NSD
ALICE preliminary* 23.7 ± 0.5 +4.6-1.1 %
CMS 28.4 ± 1.4 ± 2.6 %
Pythia D6T (109) 18.7 %
Pythia ATLAS CSC (306) 18.3 %
Pythia Perugia-0 (320) 18.5 %
Phojet 14.5 %
QGSM 19 %
Larger increase of multiplicity at mid-rapidity than in MC generators
Tail grows faster !
Good news for the Heavy Ion program:More charged particles will create
a denser and hotter system !
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Physics Analysis Papers published ‘First Physics’, EPJC 65 (2010) 111
Papers submitted Detailed analysis of charged particle multiplicity (0.9 & 2.36 TeV) EPJC, 18.4 First look at multiplicity at 7 TeV
Papers almost ready (900 GeV Data) Charged particle pT
Identified particles pT (π, K, p) Strangeness production (K0, Λ, Ξ, Φ) Baryon-antibaryon asymmetry Bose-Einstein correlations
Other ongoing Analysis π0 spectra, event structure, azimuthal correlations, h-φ correlations, high multiplicity events, ………
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P. Giubellino
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P. Giubellino
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P. Giubellino
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Charmed Mesons
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m+ m- invariant mass as measured by the Muon
Spectrometer
2.5 < h < 4
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Femtoscopy (HBT correlation)0-9 TeV
By correlating two (or more) particles (i.e. Bose-Einstein enhancement for pairs of pions at low pT), the ALICE experiment will probe the space-time substructure of the dynamic matter at the femtometer (10 -15 m) scale.These measurements are of great interest both for heavy ion and for proton-proton collisions. Indeed, the space-time substructure of the "system" created in proton collisions is not well understood, and may reveal information on the confinement process inaccessible through momentum-space probes alone
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In 1956, Robert Hanbury Brown and Richard Q. Twiss published A test of a new type of stellar interferometer on Sirius, in which two photomultiplier tubes (PMTs), separated by about 6 meters, were aimed at the star Sirius. Light was collected into the PMTs using mirrors from searchlights. An interference effect was observed between the two intensities, revealing a positive correlation between the two signals, despite the fact that no phase information was collected. Hanbury Brown and Twiss used the interference signal to determine the apparent angular size of Sirius, claiming excellent resolution.
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P. Giubellino
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Thanks for your patience…
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Backup slides
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Rapidity Rapidity Rapidity
Single Diffraction (SD) Double Diffraction (DD)Double Pomeron Exch. (DPE)