outline 1.critical short-time dynamics ― hot start & cold start ― 2. application to lattice...
TRANSCRIPT
Outline
1. Critical short-time dynamics
― hot start & cold start ―
2. Application to lattice gauge theory
― extract critical exponents ―
3. Summary
Short-Time Scaling in SU(2) Lattice Gauge Theory
at Finite Temperature
OTOBE, Tsuyoshi (Waseda Univ.)
OKANO, Keisuke (Tokuyama Univ.)
Motivation
Certain initial State Relaxation in Tc
non-equilibrium
critical slowing down
Initial StateRelaxation in Tc
long-time
Usual method
thermalequilibrium
Ising model etc. (statistical system), lattice gauge theory
New method ?
Ex. : calculating the critical exponents
t
M(t)
t
zt t_mic : O(101 ~ 2)
t_max : depending on N_space
tte
Critical short-time dynamics (Hot start & Cold start)
x0 : anomalous dimension of m0
Janssen et. al. Z. Phys. B73(1989)539.
),,,(,,, 011
00 mbLbbtbMbmLtM xzkkk
Generalized scaling law
New universal stage !
tmic ttmax
HOT
COLD
zd
z
z
d
ttM
ttM
ttA
ttM
)2()2(
1
0
~ )(
~),(ln
~ )(
~ )(
HOT start
z
x 0
Initial state
new dynamic exponent
z : dynamic exponent
ν, β : static exponent
Second moment M(2)
(t)
Autocorrelation A(t)
M(0) = 0 : high temperature
Magnetization M(t)
M(0) = m0 : small but non-ze
ro
(θ, z, ν, β)
z
z
z
d
ttM
ttM
ttU
1
0
~ )(
~ ),(ln
~ )(
1))(()()( 2)2( tMtMtU
LbbtbMbLtM zkkk 11 ,,,,
generalized scaling law
Finite size dynamic scaling law in short-time
m0=1
z : dynamic exponent
ν, β : static exponent
Binder cumulant :
COLD start
Initial state For U(t), M(t) M(0) = 1 : completely ordered
(z, ν, β)
d : spatial dim. of the system
・・・
Practical simulation t0 O(102 ~ 3)
…
tM tM
t t
samples
Initial states with the condition
z
~)(
ttM
・・・
・・・
sample averaging
(2+1)-dim. SU(2) lattice gauge theory
at finite temperature
1 , 1
s
t
tt N
N
NaNT
~
Wilson action p
pUUS
0
),( 00x
ii xxUTrW : Polyakov line
i
iWN
M2
1
asymptotic scaling
―Analysis of deconfinement phase transition ―
Heat Bath algorithm
Order parameter
Physical temperatureof the system
Relaxation dynamics
Universality
In relaxation process
2-dim.Ising model2-dim.Ising model (2+1)-dim. (2+1)-dim. SU(2) LGTSU(2) LGT
same universalitysame universality classclass
Same values for ( ν , β )
In equilibrium
Same values for ( θ, z ) ?
(1) Christensen & Damgaard ( NP B348 (1991) 226 )
N=64, N0 =2 : 4/gc2 = 3.39, β= 0.120 (8)
(2) Teper ( PL B313 (1993) 417 )
N=64, N0 =2 : 4/gc2 = 3.47, ν= 0.98 (4)
β= 0.125(exact)
ν= 1(exact)
HOT start ・ includes a new phenomena related to θ ( the anomalous dimension of m0 )
・ difficult to prepare the clean Initial state ( with m0≠0 )
Finally one has to extrapolate the result to m0 → 0
⇒ technical difficulty and complexity
・ less convergent compared to the COLD start
COLD start ・ very simple to prepare initial state
・ good convergence compared to the HOT start
・ needs a relatively bigger lattice
zz
zz
tatb
tFttM
1
1
1
),(
~
~at τ= 0 → pure power law
for τ≠0 → some modification
Determination of βc from the short-time scaling law (COLD Start)
β = βc
β > βc
β < βc
β
Inclination parameter
①②③
①②③
①②③
①②
③
t
M(t)
τ : reduced temperature
βc = 3.4505
Fit-range dependence of Inclination parameter
[200,800]
[250,800]
[300,800]
[350,800]
[400,800]
Magnetization (COLD start)
M(t)
zttM
~ )(
t
βc = 3.4505
Lattice size : 1282×2
Sample : 20000
tmic
Cumulant (COLD start)
zttU2
~
βc = 3.4505
Lattice size : 1282×2
Sample : 20000
t
U(t)
tmic
Summary of Results (COLD start)
①① ②② ③③
2/z2/z 1/νz1/νz β/νzβ/νz
SU(2)SU(2) 0.917(4)0.917(4) 0.496(17)0.496(17) 0.0633(2)0.0633(2)
IsingIsing 0.9280.928 0.4640.464 0.05800.0580
zz νν ββ
SU(2)SU(2) 2.182(10)2.182(10) 0.925(40)0.925(40) 0.128(5)0.128(5)
IsingIsing 2.16(2)2.16(2)** 1.01.0**** 0.1250.125****
① cumulant tau-difference of magnetization magnetization ② ③
From K. Okano, L. Schulke and B. Zheng, Nucl. Phys. B485 (1997) 727
** exact** 2.155(03)2.155(03)
* From several literature
Magnetization (HOT start)
tM )( ttM ~
Linear increase of the magnetization
M(t)
t
βc = 3.4505
Lattice size : 1282×2
Sample : 20000 tmic
)()2( tM
tA
Auto-correlation & second moment of magnetization
(HOT start)
t
βc = 3.4505
Lattice size : 1282×2
Sample : 30000
tmic
z
d
ttA
~ )(
zdttM
)2()2( ~ )(
θθ zz νν ββ
hothot 0.1943(4)0.1943(4) 2.108(35)2.108(35) 1.08(9)1.08(9) 0.117(27)0.117(27)
coldcold 2.182(10)2.182(10) 0.925(40)0.925(40) 0.128(5)0.128(5)
IsingIsing
(hot)(hot)0.191(1)0.191(1) 2.16(2)2.16(2) 11 1/81/8
Summary for HOT and COLD simulation
(includes preliminary result)
The 2+1 dim. SU(2) Lattice gauge theory 2-dim. Ising model
Universal (including dynamics)
Summary(1) Short time scaling behavior is observed near the critical point.
(2) It is possible to determine the Critical point βc.
(3) Static critical exponents (ν , β) (SU(2) LGT) ⇔ (Ising Model) consistent
⇒⇒ Validity of short-time critical dynamics
(4) Dynamic critical exponents (z , θ) are also obtained. (Also consistent)
(5) 2+1 dim. SU(2) Lattice gauge theory ⇔ 2-dim. Ising model universal ( including the relaxation
dynamics )
We can obtain Much information from non-equilibrium(short-time).