Thermodynamics of (2+1)-flavor QCD from the lattice

Transcription

1 INT Seattle, December 7, 2006 Thermodynamics of (2+1)-flavor QCD from the lattice Christian Schmidt for the RBC-Bielefeld Collaboration --- results from QCDOC --RIKEN BNL Saumen Datta Frithjof Karsch Chulwoo Jung Peter Petreczky Wolfgang Söldner Takashi Umeda Columbia Michael Cheng Norman Christ Robert Mawhinney NBI Kostya Petrov Bielefeld Olaf Kaczmarek Edwin Laermann Chuan Miao Jan van der Heide BU Michael Clark 1

2 The Machines 2

3 Outline Motivation The Lattice Setup The p4-action The critical temperature of QCD The flavor dependence The Equation of State (preliminary results) Lattice QCD at non-zero density (the Taylor expansion method) The The The The EoS non-zero chemical potential isentropic EoS speed of sound critical point? Summary 3

4 Improving the accuracy on Tc (as a function of quark mass and chemical potential) is mandatory to make contact to HIC phenomenology LA TT ICE QCD phase diagram calculations from first principals are important for Heavy Ion Phenomenology (and Cosmology and Astrophysics) QC D The Motivation critical region str ha ong dr ly on int ga era s cti ng Do we have a window of a strongly interacting hadron gas in the phase diagram? How large is the size of the critical region? 4

5 The Lattice Setup Analyzing hot and dens matter on the lattice: grid points, 10 d.o.f., 3 N N integrate eq. of motion 5

6 The Lattice Setup The p4-action (fermionic part): an improved staggered fermion action Remove cutoff-effects and improve rotation symmetry by adding irrelevant operators Improve flavor symmetry by smearing the one link term [ 1 3 S F N, N = n n n, n 1 [ 48 ] ] n ' mq n n n [Karsch, Heller, Sturm (1999)] 6

7 The Lattice Setup The p4-action (gluonic part): Symanzik improvement scheme 2 Remove cut-off effects of order O a 0 (tree-level improvement O g ) SG N, N = n, [ 1 6 [ ℜTr [ 1 3 ℜTr ] ] ] [Weisz, Wohlert (1984)] 7

8 The Lattice Setup Properties of the p4-action: the rotational symmetry 4 The free quark propagator is rotational invariant up to order O p Rotational symmetry of the heavy quark potential improved Dispersions relation: [Karsch, Heller, Sturm (1999)] 8

9 The Lattice Setup Properties of the p4-action: the rotational symmetry 4 The free quark propagator is rotational invariant up to order O p Rotational symmetry of the heavy quark potential improved Dispersions relation: RBC-Bielefeld MILC Wuppertal [Karsch, Heller, Sturm (1999)] 8

10 The Lattice Setup Properties of the p4-action: the cut-off effects Bulk thermodynamic quantities (pressure, energy density,...) show drastically reduced cut-off effects Continuum limit of the pressure for the free lattice gas: 9

11 The Lattice Setup The final goal: Almost realistic quark mass spectrum (2+1 flavor, Pion mass ~ 200 MeV, Kaon mass ~500 MeV) Exploring the continuum limit (a ~ 0.1 fm 0.2 fm N = 4, 6, 8 ) Analyzing the thermodynamic limit (V ~ 500 fm³, N = 8, 16, 32 ) The current status: 3-flavor QCD (masses: m /m 0.2 ) (lattices: N = 8, 16, 32 ; N = 4, 6 ) (2+1)-flavor QCD (masses: am q 0.05 am s ) (lattices: N = 8, 16 ; N = 4, 6 ) 10

12 The nature of the QCD transition ( =0 ) Mass range of the RBC-Bielefeld Collaboration for (2+1)-flavor Mass range of the RBC-Bielefeld Collaboration for 3-flavor Aoki et al., Nature 443 (2006) 675. Std. staggered + stout smearing crossover! 11

13 The critical temperature of QCD --order Parameters and susceptibilities (2+1)-flavor, 8³x4 and 16³x4 lattices Strange- and light-quark Strange- and light-quark chiral condensate: chiral susceptibility: q q /T² s s / T 3 q q /T 3 s s / T² Transition becomes stronger for smaller light quark masses. Critical couplings are determined by peak positions of the susceptibilities. All susceptibilities peak at the same critical coupling. We see no significant volume dependence crossover We use a multi-histogram analysis method (Ferrenberg-Swendson) 12

14 The critical temperature of QCD --order Parameters and susceptibilities (2+1)-flavor 8³x4 and 16³x4 q q /T² 16³x6 and 32³x6 q q /T² Transition becomes stronger for smaller light quark masses. Critical couplings are determined by peak positions of the susceptibilities. All susceptibilities peak at the same coupling. We see no significant volume dependence crossover We use a multi-histogram analysis method (Ferrenberg-Swendson) 13

15 The critical temperature of QCD --order Parameters and susceptibilities (2+1)-flavor, 8³x4 and 16³x4 lattices Polyakov Loop: L /T³ Polyakov Loop Susceptibility: L /T² Transition becomes stronger for larger light quark masses. Critical couplings are determined by peak positions of the susceptibilities. Critical couplings from chiral and Polyakov Loop susceptibilities coincide. We use a multi-histogram analysis method (Ferrenberg-Swendson) 14

16 The critical temperature of QCD --determination of the crossover point First Step: Determination of the critical couplings from peak positions of the chiral susceptibilities 3-favor and (2+1)-flavor results N = 4 ; N = 6 Critical couplings: Fits have been performed with power laws We find mass a moderate mass dependence of the beta-separation:

17 The critical temperature of QCD --the static quark potential Static Quark Potential: (2+1)-flavor results Second Step: V r / r 0 r 0 Scale determination at each critical coupling We use the Sommer scale: r 0 and the string tension: r² V r r =r 0 T=0: 16³x32 lattices =1.65 r fm 425 MeV r /r 0 Almost no mass or cut-off dependence in the scaled static quark potential 16

18 The critical temperature of QCD --combined chiral and continuum extrapolation The critical Temperature: (2+1)-flavor versus 3-flavor results T C r 0 chiral = T C r 0 phys. = extrapolation Ansatz: T C r 0= r 0 T C m e cont a r 0 m 2 r 0 me 2 d c/ N 2 3-flavor: (2+1)-flavor: e e m =0.00, d =0.64 Z 2 m =0.16, d =0.54 O 4 T C r 0 r 0 m e = Similar cut-off effects for (2+1)-flavor and 3-flavor Flavor dependence is about 5% or less. 17

19 The equation of state for (2+1)-flavor QCD the line of constant physics Goal: calculate the pressure and interaction measure on a line of constant physics (LCP) LCP determined by: m / m K =const. r 0 m =const. In good approximation we find: m / m K =const. m l / m s=const. m l Remains to be determined: m l =d 0 4 / 9 6b 0 m l / m s= R 1 d 2 a d 4 a (RG inspired Ansatz) 18

20 The equation of state for (2+1)-flavor QCD the integral method Integrate the derivative ln Z over along the line of physics to get the pressure The -function is required to calculate the interaction measure 19

21 The equation of state for (2+1)-flavor QCD the -function The non-perturbative -function: 20

22 The equation of state for (2+1)-flavor QCD the interaction measure 21

23 The equation of state for (2+1)-flavor QCD the interaction measure 22

24 Taylor coefficients with respect to the chemical potential Why Taylor coefficients? LA TT IC E QC D QCD partition function on the lattice: Z N t, N s,,am q, a = DU det [U ] am q, a exp { S G [U ]} critical region str ha ong dr ly on int ga era s cti ng complex for 0 Sign Problem! known tricks: re-weighting the =0 ensemble Fodor, Katz (2002) Taylor expansion around =0 Bielefeld-Swansea (2002) imaginary chemical potential + analytic continuation de Forcrand, Philipsen (2002) D'Elia, Lombardo (2002) canonical approach Non-zero chemical potential de Forcrand, Kratochvila (2003) Alexandru et al. (2005) 23

25 Taylor coefficients with respect to the chemical potential - expanding the pressure Allton et al. PRD 71, (2005) down quark chemical potential up quark chemical potential N f =2 m/t =0.4 N t= 4 Non-zero chemical potential 24

26 Taylor coefficients with respect to the chemical potential - bulk thermodynamics at small Pressure, Quark number density, Quark number susceptibility,... q /T Allton et al. PRD 71, (2005) N f =2 m/t =0.4 N t= 4 Non-zero chemical potential 25

27 Taylor coefficients with respect to the chemical potential - the mass dependence c2 Fluctuations increase over the resonance gas level for smaller quark masses RBC-Bielefeld preliminary c4 Non-zero chemical potential c6 26

28 Taylor coefficients with respect to the chemical potential - the radius of convergence The radius of convergence can be estimated by ratios of expansion coefficients 2 c 6 / c4 =1 / 4 n= cn c n 2 The radius of convergence gives the Distance to the closest singularity in the complex chemical potential plane resonance gas T /T c RBC-Bielefeld preliminary If all coefficients are positive the singularity lies on the real axis The critical point will show up as dip in (as peak in 1/ ) c 6 /c4 3 corresponds to crit 330 MeV B Non-zero chemical potential 27

29 Taylor coefficients with respect to the chemical potential - the radius of convergence Allton et al. PRD 71 (2005) Non-zero chemical potential 28

30 Taylor coefficients with respect to the chemical potential - the radius of convergence Fodor, Katz, JHEP 0404 (2004) 050. (re-weighting) Gavai, Gupta, PRD 71 (2005) (Taylor-expansion) Allton et al. PRD 71 (2005) Non-zero chemical potential 29

31 Taylor coefficients with respect to the chemical potential - bulk thermodynamics at small q /T Pressure Energy and Entropy density Non-zero chemical potential 30

32 Taylor coefficients with respect to the chemical potential - bulk thermodynamics at small q /T N f =2 m/t =0.4 N t= 4 S. Ejiri, F. Karsch, E. Laermann, CS, PRD 73 (2006) Non-zero chemical potential 31

33 Taylor coefficients with respect to the chemical potential - lines of constant S/ N B N f =2 m/t =0.4 N t= 4 S. Ejiri, F. Karsch, E. Laermann, CS, PRD 73 (2006) Non-zero chemical potential 32

34 Taylor coefficients with respect to the chemical potential - the isentropic equation of state N f =2 m/t =0.4 N t= 4 S. Ejiri, F. Karsch, E. Laermann, CS, PRD 73 (2006) Non-zero chemical potential 33

35 Taylor coefficients with respect to the chemical potential - the isentropic equation of state N f =2 m/t =0.4 N t= 4 S. Ejiri, F. Karsch, E. Laermann, CS, PRD 73 (2006) Non-zero chemical potential 34

36 Taylor coefficients with respect to the chemical potential - the velocity of sound F. Karsch, hep-lat/ (PANIC 05) Non-zero chemical potential 35

37 Taylor coefficients with respect to the chemical potential - the lattice EoS and hydro-expansion F. Karsch, hep-lat/ (PANIC 05) Non-zero chemical potential 36

38 Summary A large scale calculation of the critical temperature and EoS is on-going (RBC-Bielefeld on QCDOC+APEnext ): -- we find the critical temperature of QCD, continuum extrapolated from Nt=4 and Nt=6 lattices to be T c MeV -- the critical energy density shows a rapid crossover at this temperature -- the Nt=6 Eos is work in progress -- the calculation of Taylor coefficients to the 8th order has been started The transition is most likely crossover Taylor coefficients are a powerful tool to analyze bulk thermodynamic quantities at non-zero density: -- pressure, quark number density, quark number susceptibility energy and entropy density can be studied at non-zero chemical potential -- we find increasing hadronic fluctuations with decreasing quark mass -- the isentropic EoS, speed of sound has been calculated -- the critical point? -- d.o.f. in the QGP can be analyzed 37