exploring superdense matter at rhic
DESCRIPTION
Exploring superdense matter at RHIC. Barbara V. Jacak Stony Brook June 12, 2002. Goals of experiments at RHIC. Collide Au + Au ions at high energy 130 GeV/nucleon c.m. energy in 2000 s = 200 GeV/nucleon in 2001 Achieve highest possible temperature and density - PowerPoint PPT PresentationTRANSCRIPT
Exploring superdense matter at RHIC
Goals of experiments at RHIC
Collide Au + Au ions at high energy130 GeV/nucleon c.m. energy in 2000s = 200 GeV/nucleon in 2001
Achieve highest possible temperature and densityas existed ~1 sec after the Big Banginter-hadron distances comparable to
that in neutron starsheavy ions to achieve maximum volume
Study the hot, dense matter do the nuclei dissolve into a quark gluon
plasma?do partons/hadrons thermalize?characteristics of the phase transition?transport properties of the quark gluon
plasma? equation of state?
Use RHIC to study QCD
Hadron properties governed by QCDforce between quarks: exchange of
colored gluons
How does confinement work? What are the properties of deconfined
matter?
QCD is non-abelian:gluons can interact with gluonscalculations challenging
at short distance:force is weak(probe w/ high Q2, perturbative)
at large distance:force is strong(probe w/ low Q2,non-perturbative)
Deconfinement temperature, energy density?
QCD on the lattice predicts:
Karsch, Laermann, Peikert ‘99
/T4
T/Tc
Tc ~ 170 ± 10 MeV (1012 °K)
~ 3 GeV/fm3
101044 gluons, q, q’s gluons, q, q’s
Initial collision probability given by nuclear structure functionsfollowed by parton cascade
Evolution of a heavy ion collision
Experiments ask:did something new happen?
Collision dynamics (via hadronic final state)
Probe the early (hot) phase
Equilibrium?hadron spectra, yields
Collective behaviori.e. pressure and expansion?elliptic, radial flow
matter box
vacuum
QGP
Particles created earlyin predictable quantityinteract differently withQGP and normal matterfast quarks, J/fast quarks, J/, strange, strangequark content, quark content, thermal radiation
RHIC at Brookhaven National Laboratory
RHIC is first dedicated heavy ion collider10 times the energy previously available!
4 complementary experiments
STAR
Address via experiment:
Temperatureearly in the collision during plasma phase
Densityalso early in the collision, at maximum
Are the quarks confined or in a plasma?Use probes of the medium to investigate
Properties of the quark gluon plasma:equation of state (energy vs. pressure)how is energy transported in the plasma?
Density: a first look
summing particles under the curve, find ~ 5000 charged particles in collision final state
initial volume ~ Vnucleus
(~ longitudinal velocity)
Central Au+Aucollisions
Is energy density high enough?
4.6 GeV/fm3
YES - well above predicted transition!50% higher than seen before
PRL87, 052301 (2001)
dy
dE
cRT
Bj 22
11
02
R2
2c
Colliding system expands: Energy tobeam direction
per unitvelocity || to beam
elliptic flow as “barometer”
Origin: spatial anisotropy of the system when created followed by multiple scattering of particles in evolving system spatial anisotropy momentum anisotropy
v2: 2nd harmonic Fourier coefficient in azimuthal distribution of particles with respect to the reaction plane
y2 x2 y2 x2
2cos2 v
x
y
p
patan
Almond shape overlap region in coordinate space
Large v2: the matter can be modeled by hydrodynamics
STARPRL 86 (2001) 402
Hydro. CalculationsHuovinen, P. Kolb and U. Heinz
v2 = 6%: larger than at CERN or AGS!
pressure buildup explosionpressure generated early! early equilibration !first hydrodynamic behavior seen
mT2 = pT
2 + m02
mT - m0 = transverse kinetic energy
Protons are flatter velocity boost
charged hadron spectra
Many high pt baryons!
hydrodynamicalcalculation agrees with data
Teaney, Lauret, Shuryaknucl-th/0110037
nucl-ex/0203015
As many baryons as pions at pT> 2 GeV/c
Conditions in hadronic phase at RHIC
Collisions atRHIC approachzero net baryondensity
¯
_
s
B---B
Braun-Munzinger, Magestro, Redlich, Stachel, hep-ph/0105229
Tch = 175 MeVB = 51 MeV
Analyze with Grand Canonical Ensemble: fit particle ratios for mB, T
pde
pde
p TE
TE
B 3)(
3
Locate RHIC on phase diagram
Baryonic Potential B [MeV]
0
200
250
150
100
50
0 200 400 600 800 1000 1200
AGS
SIS
SPS
RHIC
quark-gluon plasma
hadron gas
neutron stars
early universe
thermal freeze-out
deconfinementchiral restauration
Lattice QCD
atomic nuclei
At the time of chemical equilibrium amonghadrons
Mystery #1
How come hydrodynamics does so well on elliptic flow and momentum spectra of mesons & nucleons emitted
… but FAILS to explain correlations between meson PAIRS?
pT (GeV)
Possible explanations:non-uniform particle density distribution!(i.e. Hydrodynamics is not explosive enough
middle not depopulated)Shape of correlation function different at RHIC
Hard scattered partons as probeof early collision stage
hadrons
q
q
hadronsleadingparticle
leading particle
schematic view of jet production
Probe: Jets from hard scattered quarks
Observed via fast leading particles orazimuthal correlations between the leadingparticles
But, before they create jets, the scatteredquarks radiate energy (~ GeV/fm) in thecolored medium
decreases their momentum fewer high momentum particles beam “jet quenching”
hadron pT spectra
PHENIX data STAR data
Baseline: inclusive pt distribution in p+p collision
Fit power law: pp =
d2N/dpt2 = A (p0+pt)
-n
Should be dominatedby leading hadronsfrom jets
Both h & 0 below p+p
Peripheral (60-80% of geom):
<N binary collisions> = 20 6
central (0-10%): <N bin coll> = 905 96
PRL 88, 022301 (2002)
Jet quenching in central Au + Au collisions?
Charged deficit seen by both STAR & PHENIX
charged
central coll central
pp
/Yield N
Yield
transverse momentum (GeV/c)
Phys. Rev. Lett. 88, 022301 (2002)
STARpreliminary
0 loweras h ½ baryons
A closer look at high pT
PHENIX preliminaryYield scales with Nbin.coll?
NO
Yield scales with Npart?
high pT : should be from hardprocesses, but see scaling with # of binaryNN collisions decrease with increasingcollision centrality (quenching effect!?)
Can we confirm jets?
STAR preliminary
Correlation of 4 GeV/c trigger hadronWith particle of pT > 2 GeV/c(v2 effect removed)
= 0.27 0.9 rad (as for jets in pp)
How much energy loss at RHIC?
<dE/dx> = 0.25 GeV/fm
scaled pp
shadowing +initial mult. scattering
but we know system is not static!
With expansion:<dE/dx> 7.3 GeVfor 10 GeV/c jets
X.N. Wang & E. Wang, hep-ph/0202105
energyloss
EM probes at RHIC
PHENIX looks for J/ e+e- and
There is the electron.
A needle in a haystack
must find electron without mistaking a pion for an electron at the level of one in 10,000
Ring ImagingCherenkovcounter to tagthe electrons“RICH”
See cherenkovlight in CO2
vpart. > cmedium
We do find the electrons
Energy/Momentum
PHENIX sees some “extra” electrons
they come from charm quarks c D meson
e + K +
J/ analysis is underway now
0 ee
ee, ee
0ee, 3
0ee, ee
conversion
ee
ee
Electron enriched sample (using RICH)
All tracks p=0.8-0.9 GeV
Mystery #2
If jets from light quarks are quenched, shouldn’t charmed quarks be suppressed too?
nucl-ex/0202002
Theorists: yes (some), no (others)Enhancement balanced by e loss?
Unprecedented energy density! > crit
Early thermalizationvery explosive collisions matter at early
time has a stiff equation of statehydrodynamics works (mostly)
Chemical equilibration with Tch ~ Tc
Probe early phase with hard partonssee a deficit energy loss!
Some mysteriesHydro misses 2 particle correlationsNo energy loss by c,cbar quarksJ/ to come (from higher L data)
QGP? Most likely… pA reference needed
Conclusions
Gluon saturation at RHIC?
Wavefunction of low x partons overlap and the self-coupling gluons fuse,
thus saturating the density of gluons in the initial state
treat as classical field!
In nucleus rest frame
r/ggg
The saturation scale:
pT2 ~ sNc 1/A2/3 dNg/dy (G(x,pT
2))
(A, b dependent) mT scaling of hadrons & suppressed gluon jet production
expect saturation effects at higher x than at HERA effect present in initial state at RHIC?
1 J.P Blaizot, A.H. Mueller, Nucl. Phys. B289, 847 (1987).
Venugopalan, McLerran, Kharzeev, etc.
What’s next?
To rule out conventional explanations extend reach of Au+Au data measure p+p reference p+Au to check effect of cold nuclei on
observables study volume & energy dependence
• are jets quenched & J/ suppressed???
Measure momentum & flight time;calculate particle mass
(dE/dx) = .08 dE/dx
pions
e
kaons
protons
STARSTAR
or measuremomentum+ energy loss in gas detector
also
Identify hadrons
PHENIX measures 0 in PbSc and PbGl calorimeters
0’spT >2 GeV, asym<0.8
in PbSc
excellentagreement!
PRL 88, 022301 (2002)
J/ suppression observed at CERN
Fewer J/ in Pb+Pb than expected!
But other processes affect J/ tooso interpretation is still debated...
J/yield
Something new at RHIC?
Compare to a baseline, or controluse nucleon-nucleon collisions at the same energy
To zero’th order Au + Au collisionsa superpositionof N-N reactions(modulo effect ofnuclear binding andcollective excitations)
Hard scattering processes scale asnumber of N-N binary collisions <Nbinary>
so expect: YieldA-A = YieldN-N . <Nbinary>
nucleons
PHENIX at RHIC
2 Central spectrometers2 Forward spectrometers3 Global detectors
Philosophy: optimize for signals / sample soft physics
Thermal Properties
PCM & clust. hadronization
NFD
NFD & hadronic TM
PCM & hadronic TM
CYM & LGT
string & hadronic TM
measuring the thermal history
, e+e-,
+Kpn
d,Real and virtual photons from quark scattering is most sensitive to the early stages. (Run II measurement)
Hadrons reflect thermal properties when inelastic collisions stop (chemical freeze-out).
Hydrodynamic flow is sensitive to the entire thermal history, in particular the early high pressure stages.
Known effects
tppA ppA
X.N.Wang, nucl-th/0104031
pA and AA data at lower energy showexcess above unity:“Cronin effect”
(multiple scattering)
From compilation of X.N. Wang
RA
A(p
T)
parton energy loss, if any, is overwhelmed by initial state soft multiple scattering!
In Pb + Pb at CERN
Crossing at ~ 1.5 GeV/c
Is SPS-RHIC comparison fair?
Same pt implies different x!
RHIC
if pT(had) / pT(jet) ~ 1 then xT ~ x(parton) at y=0
xT =
Nuclear shadowing at RHIC?Zheng Huang, Hung Jung Lu, Ina Sarcevic: Nucl.Phys.A637:79-106,1998 (hep-ph/9705250 )
Shadowingof structure functions small in RHIC x range!!
Gluon shadowingshould be even less
pt comparison OKdeficit shadowing!
quark structure function
Effect of flow + quenching?
hydro boosts baryons to higher pT
Jet quenching should reduce yield (by ~3-5)baryons less depleted as less likely to be
leading particles in fragmenting jet
Vitev & Gyulassy Phys. Rev. C65 (2002) 041902 pbar/
pi-
Correlations at high pT
jet correlations weak or missing!Reaction plane results a mystery...
Hydrodynamicsno longer dominates
Correlation method on HIJING picks out back-to-back particles from jets
For datacorrelation & reaction plane methods agree
J. Rak