fluctuations and qcd phase structure
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Fluctuations and QCD Phase Structure. Masakiyo Kitazawa (Osaka U.). My Messages. Fluctuations are inval uable observables in HIC But, we must understand them in more detail It’s possible , interesting, and important. Why Fluctuations?. Brownian Motion. A. Einstein 1905. - PowerPoint PPT PresentationTRANSCRIPT
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Fluctuations and QCD Phase StructureMasakiyo Kitazawa
(Osaka U.)
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My Messages
Fluctuations are invaluable observables in HIC
But, we must understand them in more detail
It’s possible, interesting, and important
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Why Fluctuations?
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Brownian Motion
from Wikipedia
A. Einstein1905
Fluctuations opened atomic physics
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Shot NoiseX. Jehl+, Nature405,50 (2000)
at Normal-Superconductor Junction
super
normal
cu
rren
t
Similar experiments for fractional QHE ex. Saminadayar+, PRL79,2526(1997)
Normal
Normal
Super
Normal
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Conserved-Charge Fluctuations
Fluctuations of CC : rigorously defined in a theory
Fluctuations of CC
LAT-HIC crossover
=
They are lattice observables
• operators as the Noether current• as derivatives of the partition function
QCD phase diagram 3, Wed. 11:00-13:30
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Electric Charge FluctuationAsakawa,Heinz,Muller; Jeon,Koch,2000
D-measure• D ~ 3-4 Hadronic• D ~ 1-1.5 QGP
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Electric Charge FluctuationPHENIX (2002); STAR (2003)ALICE, PRL 110, 152301 (2013)
D measure
• D ~ 3-4 Hadronic• D ~ 1-1.5 QGP
• No suppression at RHIC energy• Fluctuations @ LHC cannot be described by hadronic d.o.f.
Suppression@ LHC energy
hadronic
STAR
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Rapidity Window Dependence
• Smaller Dhmore hadronic
• Larger Dhmore QGP like
Same information in
balance function
to be studied by fluctuating hydro.
• •
Stochastic Diffusion eq.Shuryak,Stephanov,2001
ALICE, PRL 110, 152301 (2013)
hadronic
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Various Contributions
Initial fluctuations Effect of jets Negative binomial (?) Final state rescattering Coordinate vs pseudo rapidities Particle missID Efficiency correction Global charge conservation
Enhance
Enhance
Enhance
Enhance to Poisson
Enhance to Poisson
Enhance to Poisson
Enhance to Poisson
Suppress
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Global Charge Conservation
For equilibrated mediumJeon,Koch,2000
Bleicher,Jeon,Koch,2001
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Global Charge Conservation
GCC effect on the hadronic diffusion is negligible in the ALICE result!
Sakaida, Poster I-35
For equilibrated medium
Solving the time evolution…
Jeon,Koch,2000Bleicher,Jeon,Koch,2001
GCC effectdetectorcoverage
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Electric-Charge Fluctuations Electric charge fluctuations is
suppressed at LHC!
The suppression is most probably attributed to primordial physics
Qualitative difference b/w RHIC and LHC
… but why?
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Non Gaussianity
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Non-GaussianityCMB
Cosmic Microwave BackgroundMesoscopic Systems
• No statistically-significant signals • Full counting statistics• Cumulants up to 5th orderPlanck, 2013
Gustavsson+, Surf.Sci.Rep.64,191(2009)
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Non-Gaussianity in HIC
Ratio of conserved charges
Critical enhancement
Sign change
Strange confinement
Distribution funcs themselvesMorita+(2013); Nakamura (Wed.)
Asakawa,Ejiri,MK (2009); Friman+(2011); Stephanov(2011)
Stephanov(2009)
Ejiri,Karsch,Redlich(2005)
BNL-Bielefeld(2013)
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Ratio of CumulantsEjiri, Karsch, Redlich, 2005
hadronic
quark-gluon
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Strange ConfinementBaryonic
Strangeness
baryons confined
something else
strangeness confined
something else
BNL-Bielefeld,PRL(2013)H.T. Ding, This Morning
Many lattice studies (LAT-HIC crossover):Budapest-Wuppertal, 2013; BW,1403.4578; BNL-Bi.,1404.4043; Gupta+,1405.2206; Ratti, Wed.; Schmidt, Wed.; Nakamura, Wed.; Sharma, J-13
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Proton Number Cumulants at RHIC-BES
STAR 2012STAR, PRL112,032302(2014)
Exp. results are close to and less than Poissonian values. Something interesting around
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Effects of Various Contributions
Initial fluctuations Effect of jets Negative binomial (?) Final state rescattering Coordinate vs pseudo rapidities Particle missID Efficiency correction Global charge conservation
Enhance
Enhance
Enhance
Enhance to Poisson
Enhance to Poisson
Enhance to Poisson
Enhance to Poisson
Suppress
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Caution!!
proton number
cumulants
baryon number
cumulants
Let’s clarify their relation!
MK, Asakawa (2012;2012)
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Nucleon isospin and a coin
N
p n
MK, Asakawa,2012
Nucleon hastwo isospin states.
A coin has two sides.
a coin
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Slot Machine Analogy = +
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Reconstructing Total Coin Number
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Charge Exchange Reaction
mean reaction time < 5fm/c
3
1
2
2:1
1:2
cross sections of p
decay rates of D
Isospin of N is not frozen at chemical freezeout!
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Nucleons in Hadronic Medium
time
had
ron
ize
mesonsbaryons
• so many pions• rare NN collisions• no quantum corr.
chem
. f.o.
kin
eti
c f.o.
NOTE:
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Difference b/w NB and Np
genuine info. noise
net-cumulants deviate from thermal valueBut, are Poissoian
Assumptions:
Proton number cumulants are dominated by Poissonian noise
cf.) Nahrgang+, arXiv:1402.1238
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Efficiency Correction
for Particle missID: Ono,Asakawa,MK, PRC,2013
MK, Asakawa, 2012Bdzak, Koch, 2012
STAR, 2013
If efficiency for each particle is uncorrelated
binomial correction todistribution function
STAR, arXiv:1402.1558
Electric charge
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More Information on/from Fluctuations
Dh dependence
MK, Asakawa, Ono,PLB728, 386 (2014)
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Dh Dep. of Non-Gaussianity
How does the 4-th order cumulant behave as a function of Dh?
enhance?
suppress?
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Fluctuating Hydrodynamics?
Distributions in experiments are close to Poissonian Cumulants are expected to increase in the hadronic medium
These behaviors cannot be described bythe theory of hydrodynamic fluctuations
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Nucleons in Hadronic Medium
time
had
ron
ize
mesonsbaryons
chem
. f.o.
kin
eti
c f.o.
Baryons in hadronic mediumbehave like Browinian pollen
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Diffusion Master Equation
Divide spatial coordinate into discrete cells
Master Equation
probability
Solve the DME exactly, and take a0 limit
MK,Asakawa,Ono,PLB728,386(2014)
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hadronizationchemical freezeout
kinetic freezeout
Browniandiffusion
Initial condition• boost invariance• locality of fluctuations• small cumulants
Comments:• agreement with stochastic diffusion eq. up to Gaussian fluctuaion• Poisson (Skellam) distribution in equilibrium: consistent with HRG
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4th order Cumulant at ALICE MK, Asakawa,Ono (2014)
Sakaida+, poster I-35
rapidity coverage at ALICE
4th order cumulant is sensitive to initial fluctuation / transport property / confinement
It can be non-monotonic and negative!
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Dh Dep. of Non-Gaussianity
How does the 4-th order cumulant behave as a function of Dh?
enhance?
suppress?
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Suggestions to Experimentalists
many conserved charges
Dh window dependencesprimordial thermodynamics, transport property, confinementno normalization
various cumulants
electric charge, baryon number, (and strangeness?)with different diffusion constans
second, third, fourth, mixed, (and much higher?)
Beam Energy ScanLHC, RHIC-BES, FAIR, NICA, J-PARC, …
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My Messages
Fluctuations are invaluable observables in HIC
But, we must understand them in more detail
It’s possible, interesting, and important
primordial thermodynamics, confinement nature, transport property, LAT-HIC crossover, etc.
qualitative difference between RHIC and LHCreal baryon number fluc. / various corrections / thermal or non-thermal
We are just arriving at the starting point to explore QCD phase structure
with fluctuations!
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backup
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Dh Dependence at STAR Dh Dependence at STAR STAR, QM2012
decreases as Dh becomes larger at RHIC energy.
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3rd & 4th Order Fluctuations 3rd & 4th Order Fluctuations
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Strange Baryons Strange Baryons
Decay modes:Decay Rates:
Regarding these ratios even, protons from these decaysis incorporated into the binomial distribution. Then, NNNB
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Dh Dependence at Freezeout Dh Dependence at Freezeout
Initial fluctuations:
2nd
4th
parameter sensitive to
hadronization
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Total Charge Number Total Charge Number
In recombination model,
6 quarks6 antiquarks
can fluctuate, while does not.