Takashi Umeda This talk is based on the hep-lat/

Slides:



Advertisements
Similar presentations
Lattice study for penta-quark states
Advertisements

Heavy Quarkonia in a Hot Medium Cheuk-Yin Wong Oak Ridge National Laboratory & University of Tennessee Heavy Quark Workshop, BNL December 12-14, 2005 Introduction.
XQCD 2007T.Umeda (Tsukuba)1 Study of constant mode in charmonium correlators in hot QCD Takashi Umeda This talk is based on the Phys. Rev. D (2007)
Lattice 2007T.Umeda (Tsukuba)1 Study of constant mode in charmonium correlators at finite temperature Takashi Umeda Lattice 2007, Regensburg, Germany,
Thermal 2007T.Umeda (Tsukuba)1 Constant mode in charmonium correlation functions Takashi Umeda This is based on the Phys. Rev. D (2007) Thermal.
Η c and χ c at finite temperature from QCD Sum Rules C. A. Dominguez and Yingwen Zhang University of Cape Town, South Africa M. Loewe Pontificia Universidad.
Lattice QCD at finite temperature Péter Petreczky Physics Department and RIKEN-BNL Winter Workshop on Nuclear Dynamics, March 12-18, 2006 Bulk thermodynamics.
Quarkonia correlators and spectral functions Péter Petreczky Physics Department and RIKEN-BNL SQM 2006, March 26-31, 2006 Meson spectral functions and.
Stability of Quarkonia in a Hot Medium Cheuk-Yin Wong Oak Ridge National Laboratory & University of Tennessee SQM Workshop, UCLA, March 26-30, 2006 Introduction.
1 Thermodynamics of two-flavor lattice QCD with an improved Wilson quark action at non-zero temperature and density Yu Maezawa (Univ. of Tokyo) In collaboration.
ATHIC2008T.Umeda (Tsukuba)1 QCD Thermodynamics at fixed lattice scale Takashi Umeda (Univ. of Tsukuba) for WHOT-QCD Collaboration ATHIC2008, Univ. of Tsukuba,
Lecture 7-8: Correlation functions and spectral functions Relation of spectral function and Euclidean correlation functions Maximum Entropy Method Quarkonium.
ATHIC 2010T. Umeda (Hiroshima Univ.)1 Heavy Quarkonium in QGP on the Lattice Takashi Umeda 3rd Asian Triangle Heavy-Ion Conference CCNU, Wuhan, China,
TIFR Mumbai India Feb Ágnes Mócsy at RBRC 1 Quarkonium as Signal of Deconfinement Ágnes Mócsy Thanks to Sourendu, Saumen, Rajeev, Rajiv!
Heavy quarkonia in potential models and lattice QCD Péter Petreczky Heavy quark production in heavy ion collisions Purdue University, January 4-6, 2011.
Exploring Real-time Functions on the Lattice with Inverse Propagator and Self-Energy Masakiyo Kitazawa (Osaka U.) 22/Sep./2011 Lunch BNL.
5th Heavy Ion CafeT.Umeda (Tsukuba)1 Charmonium dissociation temperatures in lattice QCD Takashi Umeda This talk is based on the Phys. Rev. D
P. Gubler, K. Morita, and M. Oka, Phys. Rev. Lett. 107, (2011) K. Suzuki, P. Gubler, K. Morita, and M. Oka, arxiv: [hep-th]
Komaba seminarT.Umeda (Tsukuba)1 A study of charmonium dissociation temperatures using a finite volume technique in the lattice QCD T. Umeda and H. Ohno.
@ Brookhaven National Laboratory April 2008 Spectral Functions of One, Two, and Three Quark Operators in the Quark-Gluon Plasma Masayuki ASAKAWA Department.
Hot quarkonium spectral functions from QCD sum rules and MEM Heavy quarks and quarkonia in thermal ECT*, Villazzano, Italy Philipp Gubler.
Heavy quarks in finite temperature lattice QCD Péter Petreczky Physics Department and RIKEN-BNL Exploring QCD : Deconfinement etc, Newton Institute, Cambridge,
Heavy Flavor Productions & Hot/Dense Quark Matter 1 Lattice calculations on Heavy flavor ~ Open and Hidden charm states above Tc ~ Takashi Umeda (BNL)
Study of chemical potential effects on hadron mass by lattice QCD Pushkina Irina* Hadron Physics & Lattice QCD, Japan 2004 Three main points What do we.
RIKEN Lunch Seminar1 Study of Charmonia at finite temperature in quenched lattice QCD Takashi Umeda (BNL) RIKEN Lunch Seminar, Sept. 15th 2005.
JPS08autumnT.Umeda (Tsukuba)1 Thermodynamics at fixed lattice spacing Takashi Umeda (Univ. of Tsukuba) for WHOT-QCD Collaboration JPS meeting, Yamagata.
Ágnes Mócsy FIAS & ITP, Frankfurt Quarkonia Correlators above Deconfinement * Calculating correlators * Why interested in quarkonia correlators * Charm.
MEM Analysis of Glueball Correlators at T>0 speaker Noriyoshi ISHII (RIKEN, Japan) in collaboration with Hideo SUGANUMA (TITECH, Japan) START.
JPS07 AutumnTakashi Umeda (Tsukuba Univ.)1 Finite temperature lattice QCD with Nf=2+1 Wilson quark action WHOT-QCD Collaboration T.Umeda, S.Aoki, K.Kanaya.
Quarkonia in Quark-Gluon Plasma Cheuk-Yin Wong Oak Ridge National Laboratory Dubna July 14, 2008 Introduction Static properties of quarkonia in QGP Reactions.
CATHIE-INT 09T.Umeda (Hiroshima Univ.)1 Quarkonium correlators on the lattice T. Umeda (Hiroshima Univ.) H. Ohno, K. Kanaya (Univ. of Tsukuba) for WHOT-QCD.
Hard Probes Quarkonium states at finite temperature Takashi Umeda (BNL) Hard Probes 2006 June 9-16, 2006, Asilomar Conference Grounds Pacific Grove,
Charmonium prospects from anisotropic lattice study International workshop on “Heavy Quarkonium 2006” June 27-30, Brookhaven National Lab. Hideaki.
1 Meson mass in nuclear medium Su Houng Lee Thanks to: Hatsuda + former collaborators + and to Kenji Morita(GSI) and Taesoo Song(A&M) 1.Phase transition,
Riken Lunch SeminarT.Umeda (BNL)1 A constant contribution in meson correlators at finite temperature Takashi Umeda (BNL) Riken Lunch Seminar, BNL, Jan.
Quarks Quarks in the Quark-Gluon Plasma Masakiyo Kitazawa (Osaka Univ.) Tokyo Univ., Sep. 27, 2007 Lattice Study of F. Karsch and M.K., arXiv:
1 Properties of Quarkonia at T c Su Houng Lee In collaboration with Kenji Morita.
ATHIC 2008, Tsukuba Kenji Morita, Yonsei University Charmonium dissociation temperatures from QCD sum rules Kenji Morita Institute of Physics and Applied.
S. Aoki (Univ. of Tsukuba), T. Doi (Univ. of Tsukuba), T. Hatsuda (Univ. of Tokyo), T. Inoue (Univ. of Tsukuba), N. Ishii (Univ. of Tokyo), K. Murano (Univ.
QCD on Teraflops computerT.Umeda (BNL)1 QCD thermodynamics on QCDOC and APEnext supercomputers QCD thermodynamics on QCDOC and APEnext supercomputers Takashi.
Pentaquark in Anisotropic Lattice QCD --- A possibility of a new 5Q resonance around 2.1 GeV N. Ishii (TITECH, Japan) T. Doi (RIKEN BNL) H. Iida (TITECH,
Low energy scattering and charmonium radiative decay from lattice QCD
Recent developments in lattice QCD Péter Petreczky
Spatial charmonium correlators and spectral functions
Heavy quark potentials and spectral functions Péter Petreczky
Lattice QCD at finite temperature Péter Petreczky
Theory aspects of quarkonia production in heavy ion collisions
Thermodynamics of QCD in lattice simulation with improved Wilson quark action at finite temperature and density WHOT-QCD Collaboration Yu Maezawa (Univ.
WHOT-QCD Collaboration Yu Maezawa (RIKEN) in collaboration with
QCD Thermodynamics at fixed lattice scale
Quarkonia at finite temperature: lattice results Peter Petreczky
Can Quarkonia Survive Deconfinement?
Charmonium production in hot and dense matter Péter Petreczky
Constant mode in meson correlators at finite temperature
Thermodynamics of SU(3) gauge theory at fixed lattice spacing
Quarkonium correlators at finite temperature
QCD thermodynamics on QCDOC Machine
A Bayesian Approach to QCD Sum Rules
Takashi Umeda (Hiroshima Univ.) for WHOT-QCD Collaboration
Overview of Potential models at finite temperature Péter Petreczky
for the WHOT-QCD Collaboration
Lattice QCD study of charmonium dissociation temperatures
Takashi Umeda This talk is based on the Phys. Rev. D (2007)
Quarkonium states at finite temperature
Hot wave function from lattice QCD
Quarkonium Correlators
T. Umeda, H. Ohno (Univ. of Tsukuba) for the WHOT-QCD Collaboration
EoS in 2+1 flavor QCD with improved Wilson fermion
P. Gubler and M. Oka, Prog. Theor. Phys. 124, 995 (2010).
Lattice study of charmonia in Hot QCD
Presentation transcript:

A constant mode in charmonium correlators in finite temperature lattice QCD Takashi Umeda This talk is based on the hep-lat/0701005. Tokyo Metropolitan University, Tokyo, JPS meeting, Mar. 28, 2007 JPS meeting 07 Spring T.Umeda (Tsukuba)

Introduction J/ψ suppression is one of the most promising probe to find the QGP formation in HIC experiment. Lattice QCD studies of charmonium spectral function suggest the survival of J/ψ state above Tc (1.5Tc?) Indirect (sequential) J/ψ suppression total yield of J/ψ = direct production of J/ψ ( 60% ) + decay from higher states, ψ’ & χc ( 40% ) L. Antoniazzi et al. (E705 Collab.), PRL70, 383, (1993).  A part of the J/ψ suppression may be observed at Tdis.(ψ’orχc) when Tdis.(ψ’orχc) < Tdis.(J/ψ) Most of this talk is not so recent studies JPS meeting 07 Spring T.Umeda (Tsukuba)

χc states on the lattice S. Datta et al., PRD69, 094507 (2004). A.Jakovac et al., PRD75, 014506 (2007). Most of this talk is not so recent studies JPS meeting 07 Spring T.Umeda (Tsukuba)

Quenched QCD at T>0 Lattice setup anisotropic lattices : 203 x Nt 1/as = 2.03(1) GeV, as/at = 4 Clover quark action with tadpole imp. on anisotropic lattice H. Matsufuru et al., PRD64, 114503 (2001). rs=1 to reduce cutoff effects in higher energy states F. Karsch et al., PRD68, 014504 (2003). quark mass is tuned with MJ/ψ(= 3097MeV) Most of this talk is not so recent studies equilib. is 20K sweeps each config. is separated by 500 sweeps JPS meeting 07 Spring T.Umeda (Tsukuba)

Quenched QCD at T>0 small change in S-wave states 0.1at=800MeV small change in S-wave states  survival of J/ψ & ηc at T>Tc drastic change in P-wave states  dissociation of χc just above Tc (?) Most of this talk is not so recent studies S. Datta et al., PRD69, 094507 (2004). etc... JPS meeting 07 Spring T.Umeda (Tsukuba)

A constant mode Now we consider the meson correlator with p=0 & mq1=mq2 exp(-mqt) x exp(-mqt) = exp(-2mqt) mq is quark mass or single quark energy exp(-mqt) x exp(-mq(Lt-t)) = exp(-mqLt) Lt = temporal extent in imaginary time formalism Lt = 1/Temp. gauge field : periodic b.c. quark field : anti-periodic b.c. in confined phase: mq is infinite  the effect appears only in deconfined phase Most of this talk is not so recent studies Pentaquark (KN state): two pion state:  Dirichlet b.c. c.f. T.T.Takahashi et al., PRD71, 114509 (2005). JPS meeting 07 Spring T.Umeda (Tsukuba)

Physical interpretation Spectral function at high temp. limit F. Karsch et al., PRD68, 014504 (2003). G. Aarts et al., NPB726, 93 (2005). constant mode remains in the continuum & infinite volume Most of this talk is not so recent studies The constant term is related to some transport coefficients. From Kubo-formula, for example, a derivative of the SPF in the V channel is related to the electrical conductivity σ. JPS meeting 07 Spring T.Umeda (Tsukuba)

Removing the constant mode An analysis to avoid the constant mode Midpoint subtracted correlator Free quarks Free quarks Most of this talk is not so recent studies JPS meeting 07 Spring T.Umeda (Tsukuba)

Midpoint subtraction analysis usual effective masses at T>0 subtracted effective mass Most of this talk is not so recent studies 0.1at=800MeV the drastic change in P-wave states disappears in meffsub(t)  the change is due to the constant mode JPS meeting 07 Spring T.Umeda (Tsukuba)

Results with extended op. usual effective mass subtracted effective mass 0.1at=800MeV Most of this talk is not so recent studies extended op. enhances overlap with const. mode small constant effect is visible in V channel no large change above Tc in meffsub(t) JPS meeting 07 Spring T.Umeda (Tsukuba)

MEM analysis fails ? MEM test using T=0 data for T/Tc=1.2 for T/Tc=0.6 Most of this talk is not so recent studies A.Jakovac et al., PRD75, 014506 (2007). (also S. Datta et al., PRD69, 094507 (2004).) MEM sometimes fails when (# or quality) of data point is not sufficient. JPS meeting 07 Spring T.Umeda (Tsukuba)

Conclusion There is the constant mode in charmonium correlators above Tc The drastic change in χc states is due to the constant mode  the survival of χc states above Tc, at least T=1.4Tc. The result may affect the scenario of J/ψ suppression. In the MEM analysis, one has to check consistency of the results using, e.g., midpoint subtracted correlators. Most of this talk is not so recent studies JPS meeting 07 Spring T.Umeda (Tsukuba)