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Particle Identification @ ALICE - IRTG Heidelberg

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Partcile Production from<br />

<strong>Particle</strong> <strong>Identification</strong> @ <strong>ALICE</strong>,<br />

SIS to the LHC<br />

Techniques and physics interpretation<br />

Helmut Oeschler<br />

Darmstadt University of Technology<br />

and<br />

CERN<br />

May 11 th , 20010


Melting Matter<br />

smooth crossover


Size: 16 x 26 meters<br />

Weight: 10,000 tons


<strong>Particle</strong> identification using three detectors:<br />

Some steps in building the time projection chamber TPC<br />

Calibration, cosmic rays, pp collisions<br />

Time of Flight<br />

Inner Tracker System<br />

Results from the various detectors,<br />

Final spectra and their understanding<br />

Measuring particle yields and<br />

what we can learn from it


October 2006


The <strong>ALICE</strong> Time Projection Chamber (TPC)<br />

• main tracking and particle identification detector of Alice<br />

• delivers almost complete picture of the collision:<br />

tracking, particle momentum (pT = 0.3 B r), and particle ID<br />

⋅ ⋅ 7<br />

07.10.2009 | A.Kalweit@GSI.de<br />

5 m


The time projection chamber (TPC)<br />

largest ever<br />

88 m3, l = 5 m, d = 5.6m<br />

570 k channels<br />

lightweight,<br />

powerful FEE<br />

Radius 2.5 m<br />

Length: 5 m<br />

Volume: 95 m 2<br />

Gas: Ne CO 2 N 2


TPC


energy-loss formula<br />

• energy loss per unit path length is described by the Bethe-<br />

Bloch formula<br />

(depends only on charge and rest mass for a fixed<br />

momentum)<br />

• parameterization is fitted to the data (Aleph-<br />

Parameterization):<br />

07.10.2009 | A.Kalweit@GSI.de


<strong>Particle</strong> identification via specific energy loss<br />

• energy loss per unit path length is described by Bethe-Bloch formula:<br />

• depends only on charge<br />

and rest mass for a fixed<br />

momentum<br />

-> particle ID<br />

• scaling variable:<br />

βγ<br />

= p/m<br />

07.10.2009 | A.Kalweit@GSI.de<br />

11<br />

MC


TPC Krypton calibration<br />

• Prerequisite for precise PID: Gain of 557568 pads has to be equalized<br />

• Injection of radioactive Krypton: Rb -> Kr* -> Kr<br />

A. Matyja, Cracow<br />

07.10.2009 | A.Kalweit@GSI.de<br />

41.6 keV<br />

C side Gain Map


Field defining potential network


Calibration with laser beams


Calibration with cosmics<br />

• <strong>ALICE</strong> TPC started cosmic data taking in February 2008, long run during 2009<br />

• Almost all necessary calibrations were carried out with this data.<br />

cosmic event<br />

07.10.2009 | A.Kalweit@GSI.de<br />

15<br />

dE/dx spectrum<br />

from 7 million<br />

cosmic ray events


With magnetic field


First TPC pp event<br />

6 Dec 2009


900 GeV pp data


Parametrize the dE/dx<br />

for the various particles<br />

Slices in pt<br />

Difference between<br />

measured value and<br />

parametrized one<br />

For charged particles:<br />

pi, K and p


Secondary vertex studies:<br />

+PId<br />

Basis of topological identification<br />

Weak decay of strange particles<br />

displaced vertices (cτ ~cm)<br />

charged decay daughters<br />

K 0 s , Λ, Ξ- and Ω -<br />

high branching ratio (>64%)<br />

Reconstruction from charged tracks<br />

tracking inward<br />

secondary track selection<br />

displaced vertex finder<br />

<strong>Identification</strong> of secondary vertices<br />

quality selection (ITS clusters…)<br />

daughter PId (dE/dx, TOF, etc…)


Changes in the Reconstruction and the<br />

ESD


Λ → πp<br />

<strong>ALICE</strong> in full glory


Results from 900 GeV pp data<br />

Λ → πp<br />

PDG: 1115.7 MeV<br />

Λ → πp<br />

PDG: 1115.7 MeV<br />

K 0 s<br />

→ ππ<br />

PDG: 497.6 MeV<br />

φ → Κ + Κ −<br />

PDG: 1019.5 MeV


Lambda analysis with and without PID<br />

With PID:<br />

PID cut at 3 sigma<br />

Without PID:


Secondary vertex studies:<br />

simulation<br />

Multi-strange particle analysis ?<br />

3 prong decays for Ξ and Ω<br />

association of 3 tracks<br />

High multiplicity environment<br />

dNch /dy ~2000 (?)<br />

2 units of rapidity<br />

2 tracks: 2000 pos x 2000 neg<br />

3 tracks: …<br />

compromise efficiency / purity<br />

Candidate quality evaluation<br />

kinematical variables<br />

distances of closest approach<br />

χ 2 calculations


Ξ reconstruction


Kaon/pion ‘identification’ from their<br />

weak decay inside <strong>ALICE</strong> TPC detector<br />

24/05/10 28<br />

<strong>ALICE</strong> Week, PWG2, MSS<br />

K<br />

K<br />

K<br />

K<br />

K<br />

→<br />

μν<br />

→ ππ<br />

→ eπ<br />

→<br />

μπ<br />

→ ππ<br />

K- kinks<br />

0<br />

ν<br />

0<br />

0<br />

0<br />

ν<br />

π<br />

0<br />

π- - kinks<br />

π →<br />

μ ν<br />

63.<br />

43%<br />

21.<br />

13%<br />

4.<br />

87%<br />

3.<br />

27%<br />

1.<br />

73%<br />

99%


<strong>ALICE</strong> Data pp interactions at 900 GeV, KinkAngle VRS Mother Mom.<br />

All Kinks<br />

Blue:π Limit, Red:K Limit<br />

24/05/10 29<br />

<strong>ALICE</strong> Week, PWG2, MSS<br />

Selected Kaon-kinks


<strong>ALICE</strong> MC (left) and Data(right) pp interactions at 900 GeV, K-kinks<br />

MC<br />

24/05/10 30<br />

<strong>ALICE</strong> Week, PWG2, MSS<br />

<strong>ALICE</strong> Data


<strong>ALICE</strong> Data pp interactions at 900 GeV, K-kinks Pt, Raw and corrrect<br />

MC<br />

24/05/10 31<br />

<strong>ALICE</strong> Week, PWG2, MSS<br />

Data, 3σ cut


<strong>ALICE</strong> MC pp interactions at 900 GeV, K-kinks correction factors<br />

24/05/10 32<br />

<strong>ALICE</strong> Week, PWG2, MSS<br />

Blue->K+, Red->K-<br />

Fraction of decaying<br />

kaons in the given<br />

volume<br />

Probability of finding the<br />

kink decays


<strong>ALICE</strong> Data pp interactions at 900 GeV, K-kinks Pt, Raw and corrrect<br />

24/05/10 33<br />

<strong>ALICE</strong> Week, PWG2, MSS


Time-of-flight Detector


Time difference between measured t TOF and<br />

calculated (based on pass length)


TPC<br />

SPD cone<br />

SSD/SDD<br />

IT<br />

S<br />

SPD barrel<br />

SPD<br />

Inner Tracking System<br />

~ 10 m 2 Si detectors, 6 layers<br />

Pixels, Drift, double sided Strips


Inner Tracking System (II)<br />

• Design goals<br />

– Optimal resolution for primary vertex and track<br />

impact parameter<br />

• Minimize distance of innermost layer from beam axis<br />

(≈ 3.9 cm) and material budget<br />

– Maximum occupancy (central PbPb) < few %<br />

– 2D devices in all the layers<br />

– dE/dx information in the 4 outermost layers for<br />

particle ID in 1/β 2 region<br />

Layer Det.<br />

Type<br />

Radius<br />

(cm)<br />

Length<br />

(cm)<br />

Resolution<br />

(μ m)<br />

PbPb dN/dy=6000<br />

rφ Z Part./cm 2 Occupancy<br />

(%)<br />

1 SPD 3.9 28.2 12 100 35 2.1<br />

2 SPD 7.6 28.2 12 100 12 0.6<br />

37


ITS role in <strong>ALICE</strong> physics (II)<br />

• Vertexing<br />

– Reconstruction of primary (interaction) vertex<br />

Resolution [μ m]<br />

• From tracks: ITS crucial to obtain resolution better than 100 μm<br />

• From SPD tracklets: done before tracking and used as a starting point (seed) in the<br />

tracking phase. Allows for pileup tagging based on multiple vertices<br />

– <strong>Identification</strong> of secondary vertices from decays of hyperons and open charm and<br />

beauty hadrons<br />

Primary vertex resolution vs.<br />

multiplicity in p-p<br />

Vertex from tracks<br />

Interaction diamond:<br />

σ x,y =50 μm<br />

D + → K - π + π + decay vertex<br />

resolution<br />

38


SDD<br />

Central<br />

Cathode<br />

at -HV<br />

70.2 mm<br />

Voltage divider<br />

E drift<br />

E drift<br />

v d (e - )<br />

v d (e - )<br />

Modules mounted<br />

on ladders<br />

Anodes<br />

HV supply<br />

Front-end electronics (4 pairs of ASICs)<br />

-> Amplifier, shaper, 10-bit ADC, 40 MHz<br />

sampling<br />

LV supply<br />

Commands<br />

Trigger<br />

Data <br />

Cooling (H 2 O) tubes<br />

Cables to power<br />

supplies and DAQ<br />

Carbon fiber support<br />

Layer # ladders Mod./ladde<br />

r<br />

SDD layers<br />

into SSD<br />

# modules<br />

3 14 6 84<br />

4 22 8 176<br />

39


Pid via Energy loss


Same procedure as for TPC


Kaon analysis via the different methods


What do we learn from<br />

the spectra?


Thermallyshaped<br />

Soft<br />

Production<br />

Hard<br />

Scattering<br />

hep-ex/0305013 S.S. Adler et al.<br />

RHIC<br />

PHENIX<br />

p+p->π 0 + X


a first glimpse of mini-<br />

jets<br />

ITS-TPC matching and tracking


a first glimpse of mini-<br />

<strong>ALICE</strong> TPC Di-jet<br />

jets<br />

angular distribution of<br />

particles in TPC relative to<br />

a high p t trigger particle<br />

(single event!)


Spectra from RHIC p+p and Au+Au<br />

exponential low-energy<br />

part with a pronounced<br />

tails towards high<br />

momenta<br />

How to compare p+p with<br />

Au+Au?<br />

Volume?<br />

Bulk, N part<br />

Number of NN collisions?<br />

Hard collisions, N coll


Deuterons and anti-deuterons selection<br />

Natasha Sharma, PWG2 Meeting,<br />

March 23rd, 2010<br />

Thanks to Alexander<br />

Kalweit<br />

48


Anti deuteron<br />

Natasha Sharma, PWG2 Meeting,<br />

March 23rd, 2010<br />

49


Outlook for 7 TeV


Statistical Model<br />

Strangeness Suppression in pp<br />

Resonance Suppression in HI<br />

− In pp particle ratios are well described using canonical description<br />

− In Au+Au only stable particle ratios are well described<br />

Observed strangeness enhancement NOT signal for a QGP!


• Chemical decoupling<br />

conditions extracted<br />

from SIS up to RHIC<br />

feature common<br />

behavior<br />

• parametrisation e.g.<br />

T - μ B – systematics<br />

Nucl. Phys. A 697 (2002)<br />

902<br />

J. Cleymans, HO, K. Redlich, S. Wheaton,<br />

Phys. Rev. C 73 (2006) 034905


Chemical Freeze Out<br />

Data points:<br />

T μ B<br />

Hadronization<br />

Towards LHC!<br />

T ≈ 170 MeV<br />

μ B ≈ 1 MeV


Freeze-out parameters using the anti p/p ratio<br />

pp 900 GeV<br />

<strong>ALICE</strong><br />

pp 200 GeV<br />

STAR<br />

I. Kraus, et al., PRC 79 (2009) 014901


Predictions for pp and HI at LHC<br />

Prediction for<br />

heavy ions:<br />

Grand can.<br />

I. Kraus et al.,<br />

PRC 74 (2007)<br />

034903


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