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Baryons’10, Dec. 9, 2010, Osaka U. Third Moments of Conserved Charges in Phase Diagram of QCD. Masakiyo Kitazawa (Osaka Univ.) M. Asakawa, S. Ejiri and MK, PRL 103 , 262301 (2009). ?. Phase Diagram of QCD. RHIC, LHC. Quark-Gluon Plasma. T. lattice. Hadrons. Color SC. m. 0.

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third moments of conserved charges in phase diagram of qcd

Baryons’10, Dec. 9, 2010, Osaka U.

Third Moments of Conserved Chargesin Phase Diagram of QCD

Masakiyo Kitazawa

(Osaka Univ.)

M. Asakawa, S. Ejiri and MK,

PRL103, 262301 (2009).

phase diagram of qcd

?

Phase Diagram of QCD

RHIC, LHC

Quark-Gluon Plasma

T

lattice

Hadrons

Color SC

m

0

qcd critical point
QCD Critical Point

And, how many?

Where is the QCD critical point?

MK, et al.,2002

Stephanov, ’07

qcd critical point1

Yamamoto, et al. ’06

MK, et al.,2002

Zhang, et al., ’09

Basler, Buballa, ’10

GL analysis

induced by axial anomaly

QCD Critical Point

And, how many?

Where is the QCD critical point?

Stephanov, ’07

phase diagram of qcd1

?

Phase Diagram of QCD

RHIC, LHC

Quark-Gluon Plasma

T

  • non-uniform states?
  • quarkyonic state?
  • BEC/pseudogap region?

lattice

Hadrons

Color SC

m

0

qcd thermodynamics on the lattice
QCD Thermodynamics on the Lattice

Phase diagram for m=0

Equation of States

physical?

Hot QCD, 2009

ultra relativistic heavy ion collisions
Ultra-Relativistic Heavy Ion Collisions

from PHENIX collaboration

Observables:

  • collective flow
  • photon / dilepton production rates
  • jet / particle correlations
  • event-by-event fluctuations and higher order moments
  • and etc…

NOTE: Experimental data @ LHC is available! ALICE, 1011.3913/3914

dilepton production rate
Dilepton Production Rate

g

e+

e-

PHENIX, 2009

  • Most direct probes of the QGP.
  • They are produced in all stages of time evolution.
phase diagram of qcd2

RHIC energy scan

Phase Diagram of QCD

RHIC, LHC

T

lattice

?

Hadrons

Color SC

m

0

fluctuations at qcd critical point

However,

  • Region with large fluctuations may be narrow.
  • Fluctuations may not be formed well due to critical slowing down.
  • Fluctuations will be blurred by final state interaction.
Fluctuations at QCD Critical Point

Stephanov, Rajagopal, Shuryak ’98,’99

2nd order phase transition at the CP.

baryon # susceptibility

divergences of fluctuations of

  • pT distribution
  • freezeout T
  • baryon number,
  • proton, chage, …
net charge fluctuations
(Net-)Charge Fluctuations

Asakawa, Heinz, Muller, ’00

Jeon, Koch, ’00

D-measure:

NQ

NQ: net charge # / Nch: total #

Dy

hadrons:

quark-gluon:

values of D:

D ~ 3-4

largesmall

D ~ 1

When is experimentally measured D formed?

  • Conserved charges can remember fluctuations
  • at early stage, if diffusions are sufficiently slow.
experimental results for d measure
Experimental Results for D-measure

RHIC results: D ~ 3

PHENIX ’02, STAR ’03

  • hadron gas: D ~ 3-4
  • free quark-gluon gas: D ~ 1

STAR, ’10

experimental results for d measure1
Experimental Results for D-measure

RHIC results: D ~ 3

PHENIX ’02, STAR ’03

  • hadron gas: D ~ 3-4
  • free quark-gluon gas: D ~ 1

STAR, ’10

  • Failure of QGP formation?
  • Is the diffusion so fast?

NO!The result does not contradict these statements.

Large uncertainty in Nch.

Bialas(’02), Nonaka, et al.(’05)

take a derivative of c b

Dy

Take a Derivative of cB

cB has an edge along the phase boundary

changes the sign at

QCD phase boundary!

: third moment of

fluctuations (skewness)

  • m3(BBB) can be measured by event-by-event
  • analysis if NB in Dy is determined for each event.

NB

impact of negative third moments

No dependence on any specific models.

  • Just the sign! No normalization (such as by Nch).
Impact of Negative Third Moments

Once negative m3(BBB) is established, it is evidences that

(1) cB has a peak structure in the QCD phase diagram.

(2) Hot matter beyond the peak is created in the collisions.

third moment of electric charge

mQ : chemical potential

associated to NQ

Third Moment of Electric Charge

Experimentally,

  • net baryon # in Dy : difficult to measure
  • net charge # in Dy : measurable!
third moment of electric charge1

mQ : chemical potential

associated to NQ

Third Moment of Electric Charge

Experimentally,

  • net baryon # in Dy : difficult to measure
  • net charge # in Dy : measurable!

cB

cI/9

Under isospin symmetry,

isospin susceptibility

(nonsingular)

singular @CEP

Hatta, Stephanov ’02

the ridge of susceptibility
The “Ridge” of Susceptibility

Region with m3(BBB)<0 is limited near the critical point:

= 0 at mB=0 (C-symmetry)

m3(BBB) is positive for small mB (from Lattice QCD)

~ mB at mB>>LQCD (since W~mB4 for free Fermi gas)

T

m

the ridge of susceptibility1

m3(BBB)<0

m3(QQQ)<0

The “Ridge” of Susceptibility

Region with m3(BBB)<0 is limited near the critical point:

= 0 at mB=0 (C-symmetry)

m3(BBB) is positive for small mB (from Lattice QCD)

~ mB at mB>>LQCD (since W~mB4 for free Fermi gas)

Analysis in NJL model:

T

m

derivative along t direction

E : total energy in a subvolume

measurable experimentally

Signs of m3(BBE) and m3(QQE)

change at the critical point, too.

Derivative along T Direction

T

m

more third moments

“specific heat” at constant

  • diverges at critical point
  • edge along phase boundary
More Third Moments

T

m

more third moments1

“specific heat” at constant

  • diverges at critical point
  • edge along phase boundary
More Third Moments

T

m

Signs of these three moments change, too!

model analysis

2-flavor NJL;

G=5.5GeV-2, mq=5.5MeV, L=631MeV

Model Analysis
  • Regions with m3(*EE)<0 exist even on T-axis.
  •  This behavior can be checked
  • on the lattice
  • at RHIC and LHC energies
trails to the edge of mountains
Trails to the Edge of Mountains

m3(EEE) on the T-axis

  • Experimentally: RHIC and LHC
  • On the lattice:
trails to the edge of mountains1

c4

c6

Cheng, et al. ‘08

Trails to the Edge of Mountains

m3(EEE) on the T-axis

  • Experimentally: RHIC and LHC
  • On the lattice:

m3(QQQ), etc. at mB>0

  • Experimentally: energy scan at RHIC
  • On the lattice: ex.) Taylor expansion
summary
Summary

Seven third moments

m3(BBB), m3(BBE), m3(BEE), m3(EEE),

m3(QQQ), m3(QQE), and m3(QEE)

all change signs at QCD phase boundary near the critical point.

To create a contour map of the third moments on the QCD

phase diagram should be an interesting theoretical subject.

Negative moments would be measured and confirmed both

in heavy-ion collisions and on the lattice. In particular,

(1)m3(EEE) at RHIC and LHC energies,

(2)m3 (QQQ)=0 at energy scan,

are interesting!

proton skewness @star
Proton # Skewness @STAR

STAR, 1004.4959

Measurement of the skewness

of proton number @STAR

shows that

for 19.6-200GeV.

proton skewness @star1
Proton # Skewness @STAR

STAR, 1004.4959

Measurement of the skewness

of proton number @STAR

shows that

for 19.6-200GeV.

Remark: Proton number, NP, is not a conserved charge.

No geometrical connection b/w 2nd & 3rd moments.

higher order moments
Higher Order Moments

Ratios between higher order moments (cumulants)

RBC-Bielefeld ’09

Ejiri, Karsch, Redlich, ’05

Gupta, ’09

4th/2nd at m=0 reflects the charge of quasi-particles

Quarks:1/32

Hadrons:1

Higher order moments increase much faster near the CP.

Stephanov, ’09

Rajagopal, et al., ’10

derivative along t direction1
Derivative along T direction

simple T-derivative:

E : total energy in a subvolume

measurable experimentally

mixed 3rd moments:

Problem: T and m can not be determined experimentally.

elliptic flow 1

z

x

Elliptic Flow 1

Elliptic flow v2

beam axis

reaction

plane

v2<0

v2>0

reaction

plane

quark scaling of v 2
Quark # Scaling of v2
  • Divide by quark number.
  • Clear quark number scaling!

How to interpret?

Nonaka, et al., ’03

elliptic flow @ alice
Elliptic Flow @ ALICE

ALICE, 1011.3914

Heavy ion collisions have been performed at LHC!

new data

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