Heavy Ion results from RHIC-BNL ShinIchi Esumi Univ. of Tsukuba Contents
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Transcript of Heavy Ion results from RHIC-BNL ShinIchi Esumi Univ. of Tsukuba Contents
Hadron Collider Physics 2012, 12/Nov/2012, Kyoto ShinIchi Esumi, Univ. of Tsukuba 1
Heavy Ion results from RHIC-BNL
ShinIchi EsumiUniv. of Tsukuba
Contents
Quark Gluon Plasma Energy loss of parton in QGPCollective expansion of QGPSearch for phase transitionRHIC spin program
Hadron Collider Physics 2012, 12/Nov/2012, Kyoto ShinIchi Esumi, Univ. of Tsukuba 2
Quark Gluon Plasma (QGP)
Early universeNeutron starsQuark-hadron phase transitionDeconfinementProperties of QGP
Hadron Collider Physics 2012, 12/Nov/2012, Kyoto ShinIchi Esumi, Univ. of Tsukuba 3
STAR experiment PHENIX experiment
Relativistic Heavy-Ion Collider (RHIC) at Brookhaven National Laboratory (BNL)
2 large experiments STAR, PHENIX2 small experiments PHOBOS, BRAHMSsqrt(sNN) : 5 ~ 200GeVpp, dAu, CuCu, CuAu, AuAu, UUpolarized proton beam
RHIC andexperiments
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STAR
sqrt(sNN)=200GeV Au+Au central collisions
large acceptance lepton, photon, PID
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jet
p p
Au Au
Energy loss of high energy parton in QGP
- strong suppression of high pT hadrons in A+A with respect to a geometrical superposition of p+p collisions- no-suppression and slight enhancement in d+A (cold nuclear matter effect)
Phys. Rev. Lett. 91, 072303 (2003)
Phys. Rev. Lett. 91, 072304 (2003)
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Suppression of hadronsNo-suppression of direct-photons
PRL109, 152302 (2012)arXiv: 1208.2254
- strong suppression of hadrons- no suppression of direct photons at high pT
peripheral Au+Au central Au+Au
q
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hadrons
“- hadron”correlation
measurement
PHENIX Preliminary, QM12
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Collective expansion of QGP
- elliptic (2nd order) and higher order event anisotropic collectivity and its Nquark scaling - hydro-dynamic properties of QGP
PHENIX Preliminary, QM12
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Thermal photon radiation and collective flow
arXiv: 1105.4126Phys. Rev. Lett. 109, 122302 (2012)
Phys. Rev. Lett. 104, 132301 (2010)
- significant low pT photon excess- comparable v2 with hadrons
elliptic expansion
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Heavy quark energy loss and collective flow
u,d,s
c,b c,b
u,d,s
STAR Preliminary, QM12
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J/ suppression and collective flow(azimuthal dependence of suppression)
“suppression vs enhancement”- color screening- cold nuclear matter effect- recombination, quark coalescence
Auspectators
Cuspectatorsparticipants
PHENIX Preliminary, QM12
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PHENIX Preliminary, QM12
Transverse shape of QGP (at the end of freeze-out) via 2-parcle interferometry measurement RT-side, RT-out vs (), ()RT-side
oscill. < RT-outoscill.
for n=2,3 (central)
pT1
pT2
side view sizeqT-side : RT-side
depth + time durationqT-out : RT-out
together with vn(pT)PID
fitting with Blast Wave
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- strong 2 dependence and left/right asymmetry (coupled with energy loss and flow)- broad out-of-plane correlation enhanced more in central (redistribution and expansion)- weak 3 dependence
2-particle correlation relative to 2 and 3 plane
central 0-10%mid-central 40-50%
central 0-10%
PHENIX Preliminary, QM12Au+Au 200GeV, hadron-hadronpT : (2~4)Trig x (1~2)Asso (GeV/c)
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Testing the phase diagramwith beam energy scan
FAIR / J-PARC
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Beam energy dependence of RCP
and shape of net-proton distribution
from enhancement to suppressionwith increasing the beam energy AGS-SPS-RHIC
net-Baryon number fluctuation is expected to reflect the critical point as a non-monotonic behavior
STAR Preliminary, QM12
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v2 v3
Beam energy dependence of v2 and v3
Smooth trend (not not?) of v2 and v3 with beam energy
STAR Preliminary, QM12
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Directed flow v1
- strong anti-flow of pion (and p-bar)- small but significant anti-flow of proton- sign change of v1 slope around 10GeV- minimum around 20GeV
STAR Preliminary, QM12
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Charge asymmetry with respect to reaction planeas a possible indication of local parity violation in QGP with strong B-field at non-central heavy ion collisions
L or B
1s
2s
1c2c1
2 X
Y
dN/d ~ 1+ 2vncos(n(-)) + 2asin(-) + …<cos(1+2-2)> ~ -<a1a2>
STAR Preliminary, QM12
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Gluon Polarization G(x)
Integrated Gluon Polarization
Non zero ! ~ 0.1
- gluons can make a very significant contribution to the spin of the proton- Need to extend the measurements to low-x region where abundant gluons exist
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Sea Quark Polarization Measurements
- Direct sea quark measurement- Fragmentation function free (no model dependence)- Improve knowledge from semi-inclusive DIS measurements significantly.- x10 statistics in Run 2013
Polarized Sea-Quark Distribution
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Summary
Quark Gluon Plasma Energy loss of parton in QGPCollective expansion of QGPSearch for phase transitionRHIC spin program
Hadron Collider Physics 2012, 12/Nov/2012, Kyoto ShinIchi Esumi, Univ. of Tsukuba 22
backup slides
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Hadron Collider Physics 2012, 12/Nov/2012, Kyoto ShinIchi Esumi, Univ. of Tsukuba 24
PHENIX, QM12
extracted by BW fitting with spectra + v2,3,4 of ,K,p
extracted from RTside by HBT
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Hadron Collider Physics 2012, 12/Nov/2012, Kyoto ShinIchi Esumi, Univ. of Tsukuba 26
PHENIX, QM12
- strong 2 dependence and left/right asymmetry coupling with geometry and/or expansion- almost no 3 dependence (poor 3 resolution)
mid-central collisions
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- out-of-plane correlation enhanced (strong jet quenching and collective expansion)- some weak 3 dependence
central collisions
PHENIX, QM12