Title: Recent Results from STAR
1Recent Results from STAR
14th Topical Conference on Hadron Collider Physics
Munich, Germany
For the STAR Collaboration
2Outline
- RHIC
- STAR
- Analyses
- Anisotropic Flow
- Jets at RHIC
- Ultra-Peripheral Collisions
- Summary
- Outlook
3The Relativistic Heavy Ion Collider
- Two independent accelerator rings
- 3.83 km in circumference
- Accelerates everything from p to Au
- Running conditions Au-Au 2001
- 55-56 bunches per ring (tested up
to 110) - 7.5?108 Au/bunch _at_ storage energy
- Storage energy 100 GeV/A
- Peak luminosity 5?1026 cm-2 s-1
- Running conditions p?p? 2001
- 55 bunches per ring
- 0.8?1011 p?/bunch
- Energy/beam 100 GeV
- Peak luminosity 1.5?1030 cm-2 s-1
- Beam polarization 25 (? AGS)
Long Island
4The STAR experiment at RHIC
STAR uses the worlds largest Time Projection
Chamber
5One of the first Au on Au Events at CM Energy of
200 GeV?A
6Anisotropic Flow
- Look at peripheral collisions
- Overlap region is not symmetric in coordinate
space - Almond shaped overlap region
- Easier for particles to emerge in the direction
of x-z plane - Larger area shines to the side
- Spatial anisotropy ? Momemtum anisotropy
- Interactions among constituents generate a
pressure which transforms the initial spatial
anisotropy into the observed momentum anisotropy
- Perform a Fourier decomposition of the momentum
space particle distributions in the x-y plane - vn is the n-th harmonic Fourier coefficient of
the distribution of particles with repsect to the
reaction plane - v1 directed flow
- v2 elliptic flow
7v2 vs. Centrality (130 GeV)
- v2 is large
- 6 in peripheral collisions
- Smaller for central collisions
- Hydro calculations are in reasonable agreement
with the data - In contrast to lower collision energies where
hydro over-predicts anisotropic flow - Anisotropic flow is developed by
rescattering - Data suggests early time history
- Quenched at later times
Anisotropic transverse flow is large at RHIC
8v2 vs. pt and Particle Mass (130 GeV)
- The mass dependence is reproduced by hydrodynamic
models - Hydro assumes local thermal equilibrium
- At early times
- Followed by hydrodynamic expansion
D. Teaney et al., QM2001 Proc.P. Huovinen et
al., nucl-th/0104020
Hydro does a surprisingly good job
9v2 for High pt Particles (130 GeV)
- pQCD inelastic energy loss parameterized hydro
component (M. Gyulassy, I. Vitev and
X.N. Wang, PRL 86 (2001) 2537) - value of v2 at high pt sensitive to the initial
gluon density - saturation and decrease of v2 as a function of pt
at higher pt - data starts to deviate from hydrodynamics at pt gt
2 GeV/c
Adler et al., nucl-ex/0206006
Data is in qualitative agreement with
jet-quenching scenario
10Centrality dependence of v2(pt)
130 GeV
- v2 is saturated at high pt and it does not come
back down as rapidly as expected - What does v2 do at very high pt ?
200 GeV (preliminary)
11v2 up to 12 GeV/c
v2 seems to remain saturated
12Hard Probes in Heavy-Ion Collisions
- New opportunity using Heavy Ions at RHIC ? Hard
Parton Scattering - ?sNN 200 GeV at RHIC
- 17 GeV at CERN SPS
- Jets and mini-jets
- 30-50 of particle production
- High pt leading particles
- Azimuthal correlations
- Extend into perturbative regime
- Calculations reliable (?)
- Scattered partons propagate through matter
- radiate energy (dE/dx x) in colored medium
- Interaction of parton with partonic matter
- Suppression of high pt particles jet quenching
- Suppression of angular correlations
13Jets in Hadronic Collisions
AuAu ???? (STAR_at_RHIC)
pp ?jetjet (STAR_at_RHIC)
14Identifying jets on a statistical basis in Au-Au
STAR Preliminary AuAu _at_ 200 GeV/c, 0-5 most
central 4 lt pt(trig) lt 6 GeV/c, 2 lt pt(assoc.) lt
pt(trig)
- Given a trigger particle with pt gt pt (trigger),
associate particles with pt gt pt (associated) - AuAu
- flow
- pp and AuAu collisions
- dijets
- momentum conservation
- jets
- resonances
All ??
Small ??
15Peripheral AuAu data vs. ppflow
- Ansatz
-
- A high pt triggered AuAu event is a
superposition of a high pt triggered - pp event plus anisotropic transverse flow
- v2 from reaction plane analysis
- A is fit in non-jet region (0.75 lt ?? lt
2.24)
16Central AuAu data vs. ppflow
17Jets at RHIC
- The backward going jet is missing in central
Au-Au collisions when compared to p-p data flow - Other features of the data
- High pt charged hadrons dominated by jet
fragments - Relative charge
- Azimuthal correlation width
- Evolution of jet cone azimuthal correlation
strength with centrality
Surface emission?
- Other explanations for the disappearance of
back-to-back correlations in central Au-Au? - Investigate nuclear kT effects
- Experiment pAu or dAu
- Theory Add realistic nuclear kT to
the models
?
Suppression of back-to-back correlations in
central AuAu collisions
18Ultra-Peripheral Collisions
- b gt 2RA
- no hadronic interactions
- ltbgt 20-60 fermi at RHIC
- Ions are sources of fields
- Fields couple coherently to ions
- pt lt h/RA, 30 MeV/c for heavy ions
- p lt gh/RA 3 GeV/c at RHIC
- Photonuclear (Photon-Pomeron) Interactions
- gA r0, w, f, J/y, A
- Vector Meson Dominance
- gA qqA (elastic scattering) VA
- s(r) 350 mb at 130 GeV/nucleon
- 5 of sAuAu(had.)
- Electromagnetic particle production
- gg leptons, mesons
- Strong Field (nonperturbative?) QED
-
19Exclusive r0
200GeV
- Trigger on low multiplicity events
- veto on cosmic rays
- 2 track vertex w/ charge 0
- reject (coplanar) cosmic rays
- peak for pt lt 150 MeV/c
- pp and p-p- give background shape
- scaled up by 2.1
Signal region ptlt0.15 GeV
r0 pt
ptlt0.15 GeV
M(pp-)
20Minimum Bias Data
200 GeV
- 800,000 triggers neutron signals in ZDCs
- Nuclear excitation tags small b interactions
- excitation and r0 are independent
- Analysis same as in peripheral
Signal region ptlt0.15 GeV
Preliminary
r0 pt
200 GeV
Preliminary
- Normalized to 7.2 b hadronic cross section
- Systematic uncertainties luminosity, overlapping
events, vertex tracking simulations, single
neutron selection, etc.
ds/dMpp (mb/GeV)
M(pp-)
21Summary of Analyses
- Results
- Large anisotropic flow, consistent with
hydrodynamical picture - Saturation of v2 at high pt
- Jet quenching?
- Suppression of back-to-back jets
- Surface emission?
- r0 cross sections measured in ultra-peripheral
Au-Au collisions, good agreement to theory
- shown
- Anisotropic Flow
- Jets at RHIC
- Ultra-Peripheral Collisions
- not shown
- Particle yields / ratios / spectra
- Interferometry (HBT)
- Fluctuations
- Gluon density saturation
- Spin physics program
22RHIC Performance Goals for 2003
- 29 weeks of d-Au (including cooldown)
- 8 weeks of p?p?
- (We wont have Si-Si nor Au-Au next year.)
-
More interesting physics to come ...
23STAR Institutions
- U.S. Labs
- Argonne, Brookhaven, and Lawrence Berkeley
National Labs - U.S. Universities
- UC Berkeley, UC Davis, UCLA, Carnegie Mellon,
Creighton, Indiana, Kent State,
Michigan State, CCNY, Ohio State, Penn State,
Purdue, Rice, - UT Austin, Texas AM, Valparaiso, Washington,
Wayne State, Yale - Brazil
- Universidade de Sao Paolo
- China
- IPP - Wuhan, IMP - Lanzhou USTC, SINR,
Tsinghua University, IHEP - Beijing
England University of Birmingham France
IReS - Strasbourg SUBATECH -
Nantes Germany Max Planck Institute - Munich
University of Frankfurt India Institute of
Physics - Bhubaneswar IIT - Mumbai, VECC -
Calcutta Jammu University, Panjab
University University of Rajasthan The
Netherlands NIKHEF Poland Warsaw
University of Technology Russia MEPHI -
Moscow, IHEP - Protvino LPP LHE JINR - Dubna