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Transcript of PHENIX @ RHIC R.K. CHOUDHURY BARC. Relativistic Heavy Ion Collider at Brookhaven National Laboratory...
PHENIX @ RHIC
R.K. CHOUDHURY
BARC
Relativistic Heavy Ion Collider at
Brookhaven National Laboratory (BNL), USA
World’s First Heavy Ion Collider became operational in 2000
PHENIX, STAR, PHOBOS & BRAHMS
Relativistic Heavy Ion Collider @ BNL
Facts about RHIC
Tunnel: 3.66 m wide under the ground Circumference: 3.84 km Au Beam @200GeV/n speed: 99.995 % of c 1000’s of collisions per second 1000’s of particles produced per collision T ~ 1012 K >> T (centre of the sun) 107 K Spin polarized proton beam upto 500GeV/n
PHENIX: Pioneering High Energy Nuclear Interaction eXperiment. PHENIX is designed specifically to measure direct probes of the
collisions such as electrons, muons, phtons and hadrons.
12 Countries, 58 Institutions, 480 participants: Country: Brazil, China, France, Germany, Hungary, India, Israel,
Japan, Korea Russia, Sweden, USA
International Aspect of PHENIXInternational Aspect of PHENIX
PRIMARY MOTIVATION(Physics Driven)
1. Study of Quark Gluon Plasma(To create a mini universe in the
laboratory what might have existed a few micro seconds after the big
bang)
2. To understand the origin of
Proton Spin
To map out the QCD phase diagram
What happens when two Au ions collide heads on ?What happens when two Au ions collide heads on ?
What happens inside a Detector ?What happens inside a Detector ?
Off Line Analysis BeginsOff Line Analysis Begins
Pattern RecognitionPattern Recognition
BARC CONTRIBUTION
Fabrication of Muon Tracking Stations
Simulation and Reconstruction Software
PHENIX RUN STATISTICS
Run 01 2000 Au+Au @ 65 GeV/n for 5 weeks Run 02 2001 Au+Au @ 100 GeV/n for 16
weeks Run 03 2003 d+Au @ 100 GeV/n for 10
weeks Run 04 2004 Au+Au @ 100 GeV/n for 12
weeks Run 05 2005 Cu+Cu @ 100 GeV/n for 8 weeks Pol. p+p @ 100 GeV/n for 9 weeksRun 06 pol. p+p at 100 GeV/n for 14 weeks
Results from PHENIX (HI runs)
-- Charged particle Multiplicities (stopping) -- Transverse Energy ( ~ 5 GeV/fm3) -- Particle Yield Ratios, energy spectra (thermalisation)
-- Elliptic Flow (v2 scales with eccentricity: high collectivity)
-- Two particle correlations -- Non-statistical Fluctuations -- Suppression of particle production at high pT
-- Jet suppression -- Heavy flavour production (open charm,J/psi) -- Large (anti)baryon to pion ratio at intermediate
pT
1. Heavy flavour cross section:
-->Calculable with QCD also include effects such as Shadowing
-->Measure the cross section in pp, pPb and then extrapolate to Pb-Pb
2. Cold matter effects:
--> Nuclear absorption and Comover scattering, e.g.
J/psi + N --> D + D bar+ X
3. Energy loss in the medium:
4. Quarkonium suppression in QGP:
When screening radius rD < rQQbar, at T > TD
5. Quarkonium Enhancement at LHC:
No. of Q Qbar pairs produced at LHC is large. Possibility of recombination
Heavy Flavour Physics
PHENIX - J/ Suppresion system size dependence
CuCu
200 GeV/c
AuAu
200 GeV/c
dAu
200 GeV/c
AuAuee
200 GeV/c
CuCu
62 GeV/c
J/ muon arm
1.2 < |y| < 2.2
J/ eeCentral arm
-0.35 < y < 0.35
Factor ~3suppression
in central events
CuCuee
200 GeV/c
PHENIX - J/ Suppresion comparison to theory
Models that were successful in describing SPS datafail to describe data at RHIC
- too much suppression -
PHENIX - J/ Suppresion comparison to theory
Implementing regeneration: much better agreement with the data
Suppressed high pSuppressed high pTT hadroproduction in hadroproduction in
Au+Au Au+Au Au+Au 0 X (peripheral) Au+Au 0 X
(central)
Peripheral data agree well with Strong suppression in
p+p (data & pQCD) plus Ncoll-scaling central Au+Au collisions
Suppressed high pSuppressed high pTT hadroproduction hadroproduction
Discovery ofhigh p
T
suppression(one of most significant
results @ RHIC so far)
Ncoll
scaling
(“hard” production)
x5 suppression
Npart
scaling (surface emission)
RAA
<< 1: well below pQCD (collinear factorization) expectations for
hard scattering cross-sections
ppN
AuAuR
binaryAA
Evidence in Favor of QGPJet Tomography
Jet Quenching Data
A Strong Collective Behavior: FLOW
Definition of flow?
Φ: azimuthal angle relative to reaction plane.f (Φ): azimuthal distribution of particles.Make Fourier expansion of f (Φ).1st Fourier coefficient v1 = directed flow2nd Fourier coefficient v2 = elliptic flow vn = <cos (nΦ)>, n = 1,2,…
Central collision: vn=0, n = 1,2,… But one can have a radial flow.
Elliptic Flow for only non-central collisions.
Elliptic Flow & Hydro. Calcs.
Has PHENIX found the Quark Gluon Plasma ?
It is too early to say for sure, but the observation of jet suppression, indication of a very strong amount of flow etc. are very promising.
The collected observations of all of the four RHIC experiments are consistent with a state of matter that has the properties of a perfect fluid comprised of quarks and gluons. fluid comprised of quarks and gluons.
Future Upgrades at RHIC
RHIC Upgrade: Electron beam cooling x10 Luminosity, longer store time
PHENIX Upgrade: Si Vertex Tracking Nose Cone Calorimeter High pT Aerogel Cerenkov Detector
Large Hadron Collider
CMS Detector
Scanned picture of BEL and CEERI Scanned picture of BEL and CEERI Detectors ( Prototype)Detectors ( Prototype)
Detector Micromodule
Si Preshower detector in Endcap ECAL
THANK YOU
1. Heavy flavour cross section:
-->Calculable with QCD also include effects such as Shadowing
-->Measure the cross section in pp, pPb and then extrapolate to Pb-Pb
2. Cold matter effects:
--> Nuclear absorption and Comover scattering, e.g.
J/psi + N --> D + D bar+ X
3. Energy loss in the medium:
4. Quarkonium suppression in QGP:
When screening radius rD < rQQbar, at T > TD
5. Quarkonium Enhancement at LHC:
No. of Q Qbar pairs produced at LHC is large. Possibility of recombination
Heavy Flavour Physics
PHENIX - J/ Suppresion system size dependence
CuCu
200 GeV/c
AuAu
200 GeV/c
dAu
200 GeV/c
AuAuee
200 GeV/c
CuCu
62 GeV/c
J/ muon arm
1.2 < |y| < 2.2
J/ eeCentral arm
-0.35 < y < 0.35
Factor ~3suppression
in central events
CuCuee
200 GeV/c
PHENIX - J/ Suppresion comparison to theory
Models that were successful in describing SPS datafail to describe data at RHIC
- too much suppression -
PHENIX - J/ Suppresion comparison to theory
Implementing regeneration: much better agreement with the data
Suppressed high pSuppressed high pTT hadroproduction in hadroproduction in
Au+Au Au+Au Au+Au 0 X (peripheral) Au+Au 0 X
(central)
Peripheral data agree well with Strong suppression in
p+p (data & pQCD) plus Ncoll-scaling central Au+Au collisions
Suppressed high pSuppressed high pTT hadroproduction hadroproduction
Discovery ofhigh p
T
suppression(one of most significant
results @ RHIC so far)
Ncoll
scaling
(“hard” production)
x5 suppression
Npart
scaling (surface emission)
RAA
<< 1: well below pQCD (collinear factorization) expectations for
hard scattering cross-sections
ppN
AuAuR
binaryAA
Definition of flow?Φ: azimuthal angle relative to reaction plane.f (Φ): azimuthal distribution of particles.Make Fourier expansion of f (Φ).1st Fourier coefficient v1 = directed flow2nd Fourier coefficient v2 = elliptic flow vn = <cos (nΦ)>, n = 1,2,…
Central collision: vn=0, n = 1,2,… But one can have a radial flow.
This talk: only non-central collisions.
Elliptic Flow & Hydro. Calcs.