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Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University of California at Riverside

Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

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Page 1: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Study of Charged Hadrons Spectra with the Time Expansion

Chamber of the PHENIX Experiment at the Relativistic

Heavy Ion Collider

Dmitri KotchetkovUniversity of California at Riverside

Page 2: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

The Relativistic Heavy Ion Collider (RHIC)

Project objectives:To detect and study a

newstate of matter, quark-gluon plasma (QGP)from Au-Au collisions:in 2000 at C.M. energy

of 130 GeV;in 2001 at C.M. energy

of 200 GeV (design);To understand the spinstructure of the nucleonfrom proton-proton collisions:in 2001 at C.M. energy

of 200 GeV.N

S

Page 3: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Pioneering High Energy Nuclear Interaction eXperiment (PHENIX)

To study signatures of QGPthrough kinematical and dynamicproperties of electrons, muons,hadrons, and photons coming outof the collision point.Array of 11 subsystems forunbiased research.2000: 4 million Au-Au minimumbias (all impact parameters)events recorded;2001: 170 million Au-Au

minimumbias events recorded (with 92million minimum bias and 14million rare events available foranalysis) and 190 million p-pevents. N

SW

E

The TimeExpansionChamber

Page 4: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Passage of a Track through the PHENIX East Central Arm

Mult

iplic

ity V

ert

ex D

ete

ctor

Dri

ft C

ham

ber

Pad

Ch

am

ber

1

Rin

g Im

ag

ing C

here

nko

v D

ete

ctor

Tim

e E

xpansi

on C

ham

ber

Pad

Ch

am

ber

3

Tim

e o

f Fl

ight

Ele

ctro

magneti

c C

alo

rim

ete

r

East

Beam

Lin

e

5 cm205 cm

245 cm410 cm

260 cm

480 cm500 cm 510 cmDistances are closest to the vertex, not scaled

400

Page 5: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Functions of the Time Expansion Chamber (TEC) in the PHENIX

A) Measures charged particle ionization energy losses (dE/dx): Separation of electrons from pions: 1) over a momentum range 0.25 -3 GeV

(e/ is 5% at 500 MeV), 2) after upgraded to the Transition

Radiation Detector (TRD), over a momentum range 0.25-50 GeV via transition X-radiation detection (e/is 1.5% at 500 MeV).

B) Tracks all charged particles and produces direction vectors that match tracking information from the Drift and Pad Chambers to complete track determination in the PHENIX. Single point track resolution of 250 m and two track separation of 2 mm.C) Measuring the transverse momentum of a charged particle. PHENIX East Central Arm

TEC

Page 6: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Geometry of the TEC

2000

2001

Page 7: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Design Parameters of the TEC

1) Arranged in 6-plane 4 sectors (in 2000

and 2001 only 4 planes wereinstrumented electronically).2) Covers 900 of the PHENIX azimuthal angle and 0.35 units of pseudorapidity(approximately 400 of the polar angle ).

3) Distance from the collision vertexapproximately R = 410-457 cm.4) 64,080 wires and 20,480 readout channels.

5) Filled with Ar-CH4 (P-10) gas (90% of

argon and 10% of methane) with theeffective gas gain of 10000 (in 2000and 2001 the effective gas gain was2000-5000). (Gain is the number of electrons produced in a signal wire

by one electron knocked out by a

chargedtrack).6) Dimensions of the planes:3.00 m x 1.69 m for the smallest

and3.49 x 1.90 m for the largest.7) 320 Front-End Modules (FEM) and

640 Preamplifier/Shaper Boards (PS)(in 2001 216 FEMs and 432 PS

Boards).

TEC six-plane sector

Page 8: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Mechanical Design of the Plane

68 mm

30 mm

4 mm

Electric field

Filled withAr-CH4 (P-10) gas

Cu-Mylarwindows

8 mm

cathode (Au-Cu-Be)

anode(Au-W-Re)

To be filled with TRD fiber radiator

Drift velocity15-50 mm/s

beamdirection

East

chargedparticle

6 mm

Page 9: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Electronics chain

Fromanode

95 ns preamplifier Tail cancellation

Gain x25

Gain x5

dE/dx

TR32 channel Preamp/Shaper board

Flash Analog-Digital

Converter

Digital MemoryUnit

Data Delay andBuffering

Data Formatter PHENIXformat To PHENIX

DataCollectionModuleFPGA

Data format

Timing and mode bits

ArcNETBoard configurationDigital parameters

Communication

64 channelFront-EndModule

Page 10: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Signal sampling

28 level ADC (dE/dx)

3 level ADC (TR)

Analogvoltage

Gain x25dE/dx

Gain x5TR

Enco

der

3 bits

28 bits

5 bits

To DigitalMemory

UnitFADC

dE/dx signal: 0.2-0.3 keV (MIP in Xe)TR signal: 3-10 keV (X-rays in Xe)

Timing distributionsfor reconstructed

chargedparticles

Page 11: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Track reconstruction

y

x (East)azimuthalangle

inclination angle

charged particle

TEC

reference circleR = 450 cm

beamdirection

Hit pairs on the same track have the same and A peak in the space indicates the track.

Transverse momentum as a function of :pt = 1/(21.5*.

In 2000 the transverse momentum resolution is 4.8%+5.5%*pt

*Studied by A.Lebedev, S. Bhagavatula, and M. Rosati

Page 12: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Analysis motivations

1. Third paper published by PHENIX deals with suppression of hadrons at high pt. Analysis was done on Run-2000 data with tracks reconstructed exclusively in the PHENIX Drift Chamber.

2. It is reasonable to do similar analysis of high pt hadrons reconstructed exclusively from the TEC tracks.

3. That makes cross-check and correctness estimate on the PHENIX published result.

4. Estimate how well the Time Expansion Chamber can perform as a tracking device.

Page 13: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Data Sample from the Run-2000

PHENIX East Central Arm

Time Expansion Chamber

Electromagnetic Calorimeter

Time of Flight

Pad Chamber 3

Pad Chamber 1

Tracks reconstructed in the Time Expansion Chamber in association with hits in the Pad Chamber 1 (PC1), Pad Chamber 3 (PC3), Time of Flight (TOF), and Electromagnetic Calorimeter (EMC). No Drift Chamber Tracks.

Page 14: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

TEC Tracks in 2000

Sector 2(4 planes)

Sector 1(4 planes)

Data taken

Data in analysis

Analysis centrality selection:1) Minimum bias;2) 0-5%;3) 5-15%;4) 15-30%;5) 30-60%;6) 60-92%.;7) 0-10%.

Analysis is performed separately for positive and negative particles for each centrality bin.

1.3 million minimum bias events and

11 million tracks

Page 15: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Corrections

1. Ghost tracks, i. e. “unphysical” background is found though Z-flip method of subsystem’s hit and performing track association with flipped hit.2. Association cut efficiency.3. Acceptance.4. Surviving probability.5. Physical background.6. Momentum resolution 4.8%+5.5*pt%.7. Tracking efficiency.8. Track splitting and merging (negligible in TEC, found as ratio of angles Phi between two tracks from mixed events and the same events.

Page 16: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Acceptance

Fiducial area

Fiducial area

Vertex range:-30cm<Z<30cm

Hardware acceptance:dead areas are 8%

Page 17: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Track association and tracking efficiency

Background

Signal + background

Measure closest distances between TECtracks and associated hits in PC1, PC3, TOF, EMC, and between projection of the tracks to the collision vertex and the vertex for 60-80% peripheral events.

Tracking efficiency found as a ratio of the number of found simulated tracks embedded into data tracks to the total number of embedded tracks. Function of the number of data tracks.

Page 18: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Relative spatial resolution

Page 19: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Track association efficiency

Efficiency of association cuts asfunction of transverse momentumfor 60-80% peripheral events

no cut

cut on allsubsystems

Plot the distributions of TEC trackassociation with the collision vertex: 1) without making any association cut on any subsystem; 2) making 3- (or 2- ) cuts on all subsystems. Find the ratio of the maxima of these distributions, which will be the association cut efficiency.

Page 20: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Surviving probability and physical background

Physical background correction function is found through simulationas ratio of the total number of particlesfound in the TEC to the number of primary particles found in the TEC.

Pions

Kaons

Probability that hadrons woulddecay prior reaching the TEC

Page 21: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Transverse momentum spectra

2

hh

PHENIX preliminary

0-5%5-15%15-30%30-60%60-80%80-92%

Page 22: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Comparison with the Drift Chamber results

0-10% central events 60-80% peripheral events

Drift Chamber(nucl-ex/0109003)Time Expansion Chamber

2

hh

2

hh

Drift Chamber(nucl-ex/0109003)Time Expansion Chamber

PHENIX preliminary PHENIX preliminary

Page 23: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Presentations by UCR

Hardware:1. “Front-End Electronics for the PHENIX Time Expansion Chamber”,

2001 Nuclear Science Symposium and Medical Imaging Conference, November 4-10, 2001, San Diego (published proceedings). 2. “The Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider”, 2002 Spring Meeting of the California Section of the American Physical Society, March 29-30, Davis, California

Analysis: 1. “Study of charged hadrons with the PHENIX Time Expansion Chamber”, XIV National Nuclear Summer School, July 28 – August 10, 2002, Santa Fe, New Mexico. 2. “Study of charged hadrons with the PHENIX Time Expansion Chamber”, poster presentation at XV International Conference on Ultra-Relativistic Nucleus-Nucleus Colli

Page 24: Study of Charged Hadrons Spectra with the Time Expansion Chamber of the PHENIX Experiment at the Relativistic Heavy Ion Collider Dmitri Kotchetkov University

Upgrade

1. Ongoing upgrade into the Transition Radiation Detector (capable of pion/electron separation for momenta beyond 50 GeV) by:a) electronically instrumenting from 4 to 6 planes,b) installing polypropelene fiber radiators in front of each wire plane, c) use xenon-helium-methane (Xe-He-CH4) gas mixture.

(All work to be finished by the middle of December 2002)2) Possible construction of the TEC in the PHENIX West

Central Arm (2005).