Download - Kei Suzuki ( Tokyo Institute of Technology ) Philipp Gubler ( RIKEN ) Kenji Morita ( YITP )
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Thermal modification of bottomonium spectral functions from QCD sum rules with the maximum entropy method
Kei Suzuki (Tokyo Institute of Technology)
Philipp Gubler (RIKEN)Kenji Morita (YITP)
Makoto Oka (TITech, KEK)
P. Gubler, K. Morita, and M. Oka, Phys. Rev. Lett. 107, 092003 (2011)K. Suzuki, P. Gubler, K. Morita, and M. Oka, arxiv:1204.1173 [hep-th]
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Heavy Quark Hadrons at J-PARC 2012 2
Outline of Our Work
・ Background Quarkonium melts in quark gluon plasma (QGP)
2012/6/22
ccー
・ Purpose To investigate melting temperature
・ Method QCD sum rules with MEM
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Heavy Quark Hadrons at J-PARC 2012 3
Outline of Today’s Talk
1. Introduction 1-1. Quarkonium suppression 1-2. Previous work2. Methods3. Results 3-1. Charmonium 3-2. Bottomonium 3-3. Bottomonium excited states4. Summary
2012/6/22
GeV46.9:(1S)
GeV02.10:(2S)
GeV36.10:(3S)
bbー
c
cーT=?
T=?
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Heavy Quark Hadrons at J-PARC 2012 42012/6/22
1. Introduction
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Heavy Quark Hadrons at J-PARC 2012 5
Quarkonium suppression
• Quarkonium suppression Quarkonium (J/Ψ,Υ etc.) dissociates at finite temperature ⇒Characteristic phenomenon in QGP
2012/6/22
T. Matsui and H. Satz, Phys. Lett. B178, 416 (1986), T. Hashimoto et al. , Phys. Rev. Lett. 57, 2123 (1986)
• Mechanism―Color Debye scereening• In experiment―This phenomenon is observed as suppression of quarkonium production
c
cー
Taken from K. Fukushima and T. Hatsuda, Rept. Prog. Phys. 74, 014001 (2011)
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Heavy Quark Hadrons at J-PARC 2012 6
Previous work (Theory)
J/Ψ
2012/6/22
ηc
M. Asakawa and T. Hatsuda, Phys. Rev. Lett. 92, 012001 (2004)
⇒J/Ψ and ηc melt at 1.6Tc
J/Ψ
• Lattice QCD with MEM
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Heavy Quark Hadrons at J-PARC 2012 7
Previous work (Theory)
2012/6/22
G. Aarts et al., JHEP 1111 (2011) 103• Lattice QCD + NRQCD with MEM
⇒Excited state Υ(2S) melts at lower temperature than ground state Υ(1S)
Υ
GeV46.9:(1S)
GeV02.10:(2S)
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Heavy Quark Hadrons at J-PARC 2012 8
Previous work (Experiment)
⇒Excited states Υ(2S), Υ(3S) melt at lower temperature than ground state Υ(1S)
2012/6/22
S. Chatrchyan et al. [CMS Collaboration], Phys. Rev. Lett.107, 052302 (2011)
• Heavy ion collision at the LHC (CERN)
78.0)1(/)32( SSS 24.0)1(/)32( SSS
Υ(1S)
Υ(2S,3S)
GeV46.9:(1S)
GeV02.10:(2S)
GeV36.10:(3S)
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Heavy Quark Hadrons at J-PARC 2012 92012/6/22
2. Methods
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Heavy Quark Hadrons at J-PARC 2012 10
Theoretical approach for quarkonium suppression
2012/6/22
How can we describe quarkonium suppression from QCD?⇒We study temperature dependence of spectral function
Non-perturbative QCD approach
Quarkonium correlation function
Spectral function of hadron state
T-dependence input T-dependence outputlatticeQCD, QCD sum rule etc.
m t
ρ(t) ρ(t)
t
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Heavy Quark Hadrons at J-PARC 2012 11
dtteM
M Mt
0
/2
2OPE )(1)(
2
QCD sum rule
• QCD sum rule―treats non-perturbative information of QCD―relates correlation function given from operator product expansion (OPE) to spectral function of hadron
2012/6/22
dtqttq
0 22
OPE)()(
M.A. Shifman, A.I. Vainshtein, and V.I. Zakharov, Nucl. Phys. B147, 385 (1979); B147, 448 (1979)
Output spectral function with MEM
Input OPE One hadron state
m t
ρ(t)
Borel transformation
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Heavy Quark Hadrons at J-PARC 2012 12
OPE
)]()()()(
)()(1)[( 22
TcTb
aMAe)(MM
cJ
bJ
Js
JJ
2012/6/22
A. Bertlmann, Nucl. Phys. B204, 387 (1982 )
・ 1st term → Free massive correlator ・ 2nd term → αs correction ・ 3rd term → Scalar gluon condensate ・ 4th term → Twist-2 gluon condensate
)mass Borel :M( /4 where, 22 Mmh
temperature dependence
perturbative
non-perturbative
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Heavy Quark Hadrons at J-PARC 2012 13
OPE
2012/6/22
+
+
)]()()()(
)()(1)[( 22
TcTb
aMAe)(MM
cJ
bJ
Js
JJ
+
+
+
+
・ 3rd-term + 4th-term (Gluon condensates))()()()( TcTb c
Jb
J
)()4(9
4022
2
TGmh
b )(
)4(34
222
2
TGmh
c
⇒coefficients of gluon condensates are inversely proportional to m4
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Heavy Quark Hadrons at J-PARC 2012 14
Temperature dependence of gluon condensates
Gluon condensates at finitetemperature are expressed asenergy density ε and pressure p
2012/6/22
We Input ε and p from quenched lattice QCD
K. Morita and S.H. Lee, Phys. Rev. Lett. 100, 022301 (2008); Phys. Rev. C 77, 064904 (2008)
)3(118)( 00 pGTG vac
)()()(2 pTTG S
⇒Gluon condensates decrease with increasing temperature
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Heavy Quark Hadrons at J-PARC 2012 152012/6/22
3. Results
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Heavy Quark Hadrons at J-PARC 2012 16
Charmonium at zero temperature
2012/6/22
Mass=3.06GeV exp.)3.10GeV Mass=3.02GeV exp.)2.98GeV
Mass=3.36GeV exp.)3.42GeV Mass=3.50GeV exp.)3.51GeV
Υ ηb
χc0 χc1
J/Ψ ηc
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Heavy Quark Hadrons at J-PARC 2012 17
Charmonium at finite temperature
2012/6/22
disappear at T=1.2Tc disappear at T=1.1-1.2Tc
disappear at T=1.0-1.1Tc disappear at T=1.0-1.1Tc
ηcJ/Ψ
χc1χc0
c
cー
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Heavy Quark Hadrons at J-PARC 2012 18
Bottomonium at zero temperature
2012/6/22
Υ ηb
χb1χb0
Mass=9.63GeV exp.)9.46GeV Mass=9.55GeV exp.)9.39GeV
Mass=10.18GeV exp.)9.86GeV Mass=10.44GeV exp.)9.89GeV
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Heavy Quark Hadrons at J-PARC 2012 19
Bottomonium at finite temperature
2012/6/22
χb1
ηbΥ
χb0
disappear at T>2.5Tc disappear at T>2.5Tc
disappear at T=2.0-2.5Tc disappear at T=2.0-2.5Tc
bbー
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Heavy Quark Hadrons at J-PARC 2012 20
Bottomonium excited states • The obtained bottomonium spectral functions
contain contributions of excited states
• To investigate behavior of the excited states, we analyzed “residue’’ of peak (integral value of peak)
• We used least squares fitting to exclude contributions of continuum (one peak + continuum as Breit-Wigner + step-like function)
2012/6/22
Υ
Υ(1S), Υ(2S) and Υ(3S)
GeV46.9:(1S)
GeV02.10:(2S)
GeV36.10:(3S)
・ Our method cannot separate these states
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Heavy Quark Hadrons at J-PARC 2012 21
Temperature dependence of residue
2012/6/22
Obtained residue of Υ peak decreases with increasing temperature⇒Excited states(2S, 3S) melt at 1.5-2.0Tc and ground state(1S) survives?
Υ(1S+2S+3S)
Υ(1S) only?
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Heavy Quark Hadrons at J-PARC 2012 22
Summary
• We extracted melting temperature of quarkonia from QCD sum rules with MEM
• Melting temperatures of quarkonia
• We suggested that bottomonium excited states Υ(2S,3S) melt at lower temperature than ground state Υ(1S)
2012/6/22
J/Ψ ηc χc0 χc1
1.2Tc 1.1-1.2Tc 1.0-1.1Tc 1.0-1.1Tc
Υ ηb χb0 χb1
>2.5Tc >2.5Tc 2.0-2.5Tc 2.0-2.5Tc