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Thermodynamics and heavy-quark free energy at finite temperature in full-QCD lattice simulations with Wilson quarks. Yu Maezawa (RIKEN) in collaboration with S. Aoki, K. Kanaya, H. Ohno, H. Saito (Univ. of Tsukuba) S. Ejiri (Niigata univ.) T. Hatsuda (Univ. of Tokyo) - PowerPoint PPT Presentation
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Thermodynamics and heavy-quark free energy
at finite temperature in full-QCD lattice simulations with Wilson quarks
Thermodynamics and heavy-quark free energy
at finite temperature in full-QCD lattice simulations with Wilson quarks
Yu Maezawa (RIKEN)
in collaboration with
S. Aoki, K. Kanaya, H. Ohno, H. Saito (Univ. of Tsukuba)
S. Ejiri (Niigata univ.)
T. Hatsuda (Univ. of Tokyo)
T. Umeda (Hiroshima univ.)
WHOT-QCD Collaboration
NFQCD @ YITP, Mar. 16, 2010
WHOT-QCD Coll. arXive:0907.4203WHOT-QCD Coll. PoS LAT2007 (2007) 207
WHOT-QCD Coll. Phys. Rev. D75 (2007) 074501
2
ContentsContents 1. Introduction
i. Heavy-quark free energy and potential on lattice
ii. Fixed scale approach
2. Results of lattice QCD simulations
i. Heavy-quark potential at T = 0 and T > 0
ii. Color-channel dependence and Debye screening effect in QGP
iii. Heavy-quark potential at finite density (q)
3. Summary
3
IntroductionStudy of Quark-Gluon Plasma (QGP)
• Early universe after Big Bang• Relativistic heavy-ion collision
Theoretical study based on first principle (QCD) Lattice QCD simulation at finite (T, q)
Bulk properties of QGP (p, , Tc,…) Internal properties of QGP
are well investigated. are still uncertain.
Big Bang
RHICT
q
QGP
nucleusCSC
s-QGP
Big Bang
RHICT
q
QGP
nucleusCSC
s-QGP
/T 4
T / Tpc
CP-PACS 2001 (Nf = 2, Tc ~ 170 MeV)
/T 4
T / Tpc
CP-PACS 2001 (Nf = 2, Tc ~ 170 MeV)
/T 4
T / Tpc
CP-PACS 2001 (Nf = 2, Tc ~ 170 MeV)
/T 4
T / Tpc
CP-PACS 2001 (Nf = 2, Tc ~ 170 MeV)
qq qqqq
Properties of quarks and gluons in QGP Heavy-quark potential: free energy btw. static charged quarks in QGP
1. Relation of inter-quark interaction between zero and finite T2. Temperature dependence of various color-channels3. Heavy-quark potential at finite density (q) in Taylor expansion method
r
44
Heavy-quark potential at finite THeavy-quark potential at finite THeavy-quark potential interaction btw. static quark (Q) and antiquark (Q) in QCD matter
T = 0,
T > 0, string tension () decreases,
string breaking at rc
At T > Tc, screening effect in QGP
rr
rV )(
rTmDer
TTrV )(eff )(
),(
Lattice QCD simulations
Properties of heavy-quark potential in quark-gluon plasma
• Heavy-quark bound state (J/, Υ) in QGP
• Screening effect in QGP
• Inter-quark interaction btw. QQ and QQ
T >Tc
T <Tc
55
)y()x(Trln),(1 †TTrF
Heavy-quark potential Brown and Weisberger (1979)
Wilson-loop operator
Heavy-quark free energyHeavy-quark free energy
r
r
WrV
);y,x(lnlim)( 1
Heavy-quark free energy Nadkarni (1986)x
r
);y,x( W
Correlation b/w Polyakov-lines projected to a color singlet channel in the Coulomb gauge
Heavy-quark free energy may behave in QGP as:
Polyakov-line : static quark at x
tN
U1
4 ),x()x(
T = 0
T > 0
To characterize an interaction b/w static quarks,
r0
)x(† )y(T/1
x
Operator similar to the Wilson-loop
at finite T
short r: F 1(r,T ) ~ V(r) (no effect from thermal medium)
mid r : screened by plasma long r : two single-quark free energies w/o interactions
CTT CTT
CTT CTT
6
Fixed Nt approach
Fixed scale approach WHOT-QCD, PRD 79 (2009) 051501.
Approaches of lattice simulations at finite TApproaches of lattice simulations at finite TTo vary temperature on the lattice,
• Changing a (controlled by the gauge coupling ( = 6/g2)), fixing Nt
• Changing Nt , fixing a
Advantages: T can be varied arbitrarily, because is an input parameter.
Advantages: investigation of T dependence w/o changing spatial volume possible.
renormalization factor dose not change when T changes.
tNaT 1 a: lattice spacing
Nt: lattice size in E-time direction
tN
ax
T/1
T
T/1
Tx
Kanaya san’s talk, yesterday
77
Results of lattice QCD simulations
1. Heavy-quark potential at T = 0 and T > 0
2. Color-channel dependence and Debye screening effect in QGP
3. Heavy-quark potential at finite density (q)
88
Simulation details
Nf = 2+1 full QCD simulations
Lattice size: Ns3 x Nt = 323 x 12, 10, 8, 6, 4
Temperature: T ~ 200-700 MeV (5 points)
Lattice spacing: a = 0.07 fm
Light quark mass*: m/m = 0.6337(38)
Strange quark mass*: m/m = 0.7377(28)
Scale setting: Sommer scale, r0 = 0.5 fm
*CP-PACS & JLQCD Coll., PRD78 (2008) 011502.
99
Heavy-quark potential at T = 0
00)( Vr
rrV
Data calculated by
CP-PACS & JLQCD Coll.on a 283 x 58 lattice
Phenomenological potential
)(rV
[fm] r
GeV .
GeV .
.
232
4340
4410
0
0
V
Our fit results
= Coulomb term at short r + Linear term at long r + const. term
10
),(1 TrF )(rV
[fm] r
Heavy-quark free energy at T > 0
At short distance
F 1(r,T ) at any T
converges to
V(r) = F 1(r,T=0 ).
Short distance physics is
insensitive to T.
Note:
In the fixed Nt approach, this property is used to adjust the constant term of F 1(r,T ).
In our fixed scale approach, because the renormalization is common to all T. no further adjustment of the constant term is necessary.
We can confirm the expected insensitivity!
11
),(1 TrF )(rV
[fm] r
Heavy-quark free energy at T > 0
At short distance
F 1(r,T ) at any T
converges to
V(r) = F 1(r,T=0 ).
Short distance physics is
insensitive to T.
T ~ 200 MeV: F 1 ~ V up to 0.3--0.4 fm
T ~ 700 MeV: F 1 = V even at 0.1 fm
Range of thermal effect is T-dependent
Debye screening effect
discussion, later
12
),(1 TrF )(rV
[fm] r
Heavy-quark free energy at T > 0
Long distanceF
1(r,T ) becomes flat and has no increase linealy.
Confinement is destroyed due to a thermal medium effect.
Qr FTTTrF 2Trln)y()x(Trln),(
21 †
At large r, correlation b/w Polyakov-lines will disappear,
F 1 converges to 2x(single-quark free energy) at long distance
2FQ calculated from
Polyakov-line operator
1313
Results of lattice QCD simulations
1. Heavy-quark potential at T = 0 and T > 0
2. Color-channel dependence and Debye screening effect in QGP
3. Heavy-quark potential at finite density (q)
Heavy-quark potential for various color-channels
qq qqqqDecomposition of color channel
Projection of Polyakov-line correlators Nadkarni (1986)
Normalized free energy (heavy-quark potential)
Nf = 2 lattice QCD simulations (fixed Nt approach)
Various color-channels of interaction are induced in QGP
CCC*C 8133
C*CCC 6333
• QQ correlator:
• QQ correlator:
0),(2),(),( r
MQ
MM TrVFTrFTrV 6 ,3 ,8 ,1 C*CCCM
MeV 186~,80.0,65.0/,416 pc33 TmmNN ts
Heavy-quark potential for various color-channels
C1
C8
*C3
C6
Temperature increases becomes weak
1c, 3*c: attractive force, 8c, 6c: repulsive force
Single gluon exchange ansatz
Consistent with Casimir scaling
extract eff(T) and mD(T) by fitting V(r,T)
),( TrV M
)x(† )y(
4A 4A
effg effg
at at
)()( yxtr †
mD
)x(† )y()x(† )y(
4A 4A
effg effg
at at
)()( yxtr †
mD
)x(† )y(
4A 4A
effg effg
at at
)()( yxtr †
mD
)x(† )y()x(† )y(
4A 4A
effg effg
at at
)()( yxtr †
mD
rTmM
Der
TCTrV )(eff )(
),(
3
1,
3
2,
6
1,
3
46*381 CCCC
M
a
a
aM ttC 2
8
1 1
Casimir factor
QQ potential QQ potential80.0/ mm
r [fm] r [fm]
disappears at T > 2Tpc
becomes large at T ~Tpc
~
Results of eff(T) and mD(T) for each color channel
Channel dependence of eff and mD
Universal descriptions byrTm
MDe
r
TCTrV )()(
),( eff
Single-gluon exchange ansatz dose not work well.
Debye screening effect in QGP65.0/ mm
Comparison with perturbative screening mass
Perturbative screening mass
)(ln)(),;(
)(SM2loop
2
6
6 2
12
1
1
2
311 go
m
mTgTg
T
Tm
mag
DN
NNLOD
f
f
LO NLO Rebhan, PRD 48 (1993) 48
Lattice screening mass is not reproduced by LO-type screening mass.
Contribution of NLO-type corrects the LO-type screening mass.
MeV 2613 fN
SMTT 3~
TTgmmag )(48.0~ 2
NLO
LO
pcTT
T
TmD )(
Results of mD(T) for color singlet channel
1818
Results of lattice QCD simulations
1. Heavy-quark potential at T = 0 and T > 0
2. Color-channel dependence and Debye screening effect in QGP
3. Heavy-quark potential at finite density (q)
19
Heavy-quark potential at finite qBig Bang
RHICT
q
QGP
nucleusCSC
s-QGP
Big Bang
RHICT
q
QGP
nucleusCSC
s-QGP
Motivation
Taylor expansion method in terms of q /T
Properties of QGP at 0 < q /T << 1
Expectation values at finite q
At q /T << 1, Taylor expansion of quark determinant detD(q)
where
• Early universe after Big Bang• Relativistic heavy-ion collisions
Low density
e.g. q /Tc ~ 0.1 at RHIC
c.f.) sign problem
detD becomes complex when q≠0
aq Re
20
Heavy-quark potential at finite q
Heavy-quark potential up to 2nd order
with expansion coefficients:
QQ potential (1c, 8c) QQ potential (3*c, 6c)
Odd term of QQ potential vanishes because of symmetry under q → -q
21
QQ potential80.0/ mm
1c channel: attractive force
8c channel: repulsive force
r [fm]
becomes weak
at 0 < q /T << 1
r [fm]
QQ potential
3*c channel: attractive force
6c channel: repulsive force
80.0/ mm
r [fm]
1
1
r [fm]
becomes strong
at 0 < q /T << 1
2
2
r [fm]
23
Heavy-quark potential at finite q
QQ potential (1c, 8c)
QQ potential (3*c, 6c)
Attractive channel in heavy-quark potential
Heavy-meson correlation (1c) weak
at 0 < q /T << 1
Diquark correlation (3*c) strong
• Channel dependence disappear
at T > 2Tpc
• mD is not reproduced by
LO thermal perturbation
24
Screened Coulomb form:
with the Debye mass,
rTmM
Der
TCTrV ),(),(
),,( qqeffq
)()()0,(),( 42
2 qqq
OTcTmTm TDD
650./ VPS mm
)(2 Tc Similar properties at q = 0
Debye screening mass at finite q
~
25
1. Heavy-quark potential at T = 0 and T > 0
2. Color channel dependence and Debye screening effect in QGP
3. Heavy-quark potential at finite density (q)
SummaryProperties of quark-gluon plasma
Heavy-quark potential (F 1(r,T )) defined
by free energy btw. static charged quarks
At short r : F 1 at any T converges to heavy-quark potential at T = 0
Short distance physics is insensitive to T.
At long r : F 1 becomes flat and has no linear behavior.
Correlation b/w Polyakov-lines disappears and F 1 converges to 2FQ
),(1 TrF )(rV
[fm] r
Taylor expansion in terms of q /T
Heavy-meson correlation (1c) weak Diquark correlation (3*c) strong
at 0 < q /T << 1
rTmM
Der
TCTrV )(eff )(
),(
single-gluon exchange ansatz works well at T > 2Tpc :
mD is not reproduced by LO thermal perturbation
mD has higher order or non-perturbative contribution.
~