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Sunao Sakai

Publications and source records attributed to Sunao Sakai.

12 recordsLinked to original sources

Transport Coefficient of Gluon Plasma from Lattice QCD

In this report we present our calculation of the transport coefficient of gluon system on $24^3\times 8$ lattice in the quench approximation. Simulations are carried out in the range, $1.4 \le T/T_c \le 24$. In the temperature region slightly above the transition, where the perturbative calculation is not applicable, the shear viscosity($η$) is smaller than typical hadron masses. The bulk viscosity is consistent with zero within the range of error bars in $1.4 \le T/T_c \le 24$. We compare our results with the perturbative calculations in large $T/T_c$ region. It is found that the lattice and perturbative results are consistent with each other there. The ratio $η/s$ is around $0.1-0.4$ in $T/T_c < 3$ region and satisfies the KSS bound\cite{KSS}. In order to estimate the contribution from high frequency part of the spectral function, we study the effects of a term $ρ^{high}$ proposed by Aarts and Resco\cite{Aarts}. It is found that until the threshold mass becomes small, its effect is quite small, and that viscosity decreases as the threshold decreases. From these studies we think that although our result is obtained under an assumptions for the spectral function, it gives a reasonable estimation for $η$($=πdρ/dω$ at $ω=0$), and qualitative results will not be changed when the accurate spectral function is obtained.

hep-lat

Transport Coefficients of Gluon Plasma

Transport coefficients of gluon plasma are calculated for a SU(3) pure gauge model by lattice QCD simulations on $16^3 \times 8$ and $24^3 \times 8$ lattices. Simulations are carried out at a slightly above the deconfinement transition temperature $T_c$, where a new state of matter is currently being pursued in RHIC experiments. Our results show that the ratio of the shear viscosity to the entropy is less than one and the bulk viscosity is consistent with zero in the region, $1.4 \leq T/T_c \leq 1.8 $.

hep-lat

Improved gauge action on an anisotropic lattice II - Anisotropy parameter in the medium coupling region -

The quantum correction of the anisotropy parameter, $η$, is calculated for $ξ=2$ and 3 in the $β$ region where numerical simulations such as hadron spectroscopy are currently carried out, for the improved actions composed of plaquette and rectangular 6-link loops. The $β$ dependences of $η$ for the renormalization group improved actions are quite different from those of the standard and Symanzik actions. In Iwasaki and DBW2 actions, $η$ stays almost constant in a wide range of $β$, which also differs from the one-loop perturbative result, while in the case of Symanzik action, it increases as $β$ decreases, which is qualitatively similar to the perturbative result, but the slope is steeper. In the calculation of the $η$ parameter close to and in the confined phase, we have applied the link integration method to suppress the fluctuation of the gauge fields. Some technical details are summarized.

hep-lat

Quiescent String Dominance Parameter F and Classification of One-Dimensional Cellular Automata

The mechanism which discriminates the pattern classes at the same $λ$, is found. It is closely related to the structure of the rule table and expressed by the numbers of the rules which break the strings of the quiescent states. It is shown that for the N-neighbor and K-state cellular automata, the class I, class II, class III and class IV patterns coexist at least in the range, $\frac{1}{K} \le λ\le 1-\frac{1}{K} $. The mechanism is studied quantitatively by introducing a new parameter $F$, which we call quiescent string dominance parameter. It is taken to be orthogonal to $λ$. Using the parameter F and $λ$, the rule tables of one dimensional 5-neighbor and 4-state cellular automata are classified. The distribution of the four pattern classes in ($λ$,F) plane shows that the rule tables of class III pattern class are distributed in larger $F$ region, while those of class II and class I pattern classes are found in the smaller $F$ region and the class IV behaviors are observed in the overlap region between them. These distributions are almost independent of $λ$ at least in the range $0.25 \leq λ\leq 0.75$, namely the overlapping region in $F$, where the class III and class II patterns coexist, has quite gentle $λ$ dependence in this $λ$ region. Therefore the relation between the pattern classes and the $λ$ parameter is not observed. PACS: 89.75.-k Complex Systems

nlin.CG

A New Parameter $F$ to Classify Cellular Automata Rule Table Space and a Phase Diagram in $λ-F$ Plane

It is shown that for the N-neighbor and K-state cellular automata, the class II, class III and class IV patterns coexist at least in the range $\frac{1}{K} \le λ\le 1-\frac{1}{K} $. The mechanism which determines the difference between the pattern classes at a fixed $λ$ is found, and it is studied quantitatively by introducing a new parameter $F$. Using the parameter F and $λ$, the phase diagram of cellular automata is obtained for 5-neighbor and 4-state cellular automata. PACS: 89.75.-k Complex Systems

nlin.CG

Structure of Rule Table and Phase Diagram of One Dimensional Cellular Automata

In addition to the $λ$ parameter, we have found another parameter which characterize the class III, class II and class IV patterns more quantitatively. It explains why the different classes of patterns coexist at the same $λ$. With this parameter, the phase diagram for an one dimensional cellular automata is obtained. Our result explains why the edge of chaos(class IV) is scattered rather wide range in $λ$ around 0.5, and presents an effective way to control the pattern classes. \noindent PACS: 89.75.-k Complex Systems

nlin.CG

Anisotropic Lattice and Its Application to Quark Gluon Plasma

We have studied the link-integration method for the improved actions. With this method the $η$ parameter in the medium to strong coupling regions is obtained. Effects of the self-energy terms for the $η$ parameters are small in the regions of $β$ and $η$ studied. After these investigations, the anisotropic lattice is used for the calculation of transport coefficients of the quark gluon plasma.

hep-lat

Anisotropic Improved Actions

The studies of the quantum corrections for the anisotropy parameter,$η(=ξ_R/ξ_B)$, for the improved actions, $β(C_0 L({Plaq.}) + C_1 L({Rect.}))$, are proceeded in the medium to strong coupling region on anisotropic lattices. The global features for the $η$ parameters as a function of $β$ and the coefficient $C_{1}$ have been clarified. It has been found by the perturbative analysis that as $C_1$ decreases, the slope of the $η(β)$ becomes less steep and for the actions whose $C_{1}$ is less than -0.160, $η$ decreases as $β$ decreases, contrary to the case of the standard action. In the medium to strong coupling region, the $η$ parameter begins to increase as $β$ decreases for all $C_{1}$. This means that for the actions with $C_{1} < -0.160$, the one-loop perturbative results for $η$ break down qualitatively and the $η$ parameters have a dip. As a result of this dip structure the $η$ for Iwasaki's action remains close to unity in the wide range of $β$.

hep-lat

Anisotropic Improved Gauge Actions; --Perturbative and Numerical Studies --

The $Λ$ parameter on the anisotropic lattice, the spatial and temperature coupling constant $g_σ$, $g_τ$ and their derivative with respaect to the the anisotropy parameter $ξ$ are studied perturbatively for the class of improved actions, which cover tree level Symanzik's, Iwasaki's and QCDTARO's improved actions. The $η(=g_τ/g_σ)$ becomes less than 1 for Iwasaki's and QCDTARO's action, which is confirmed nonperturbatively by numerical simulations. Derivatives of the coupling constants with respect to the anisotropy parameter, $\partial g_τ/\partial ξ$ and $\partial g_σ/\partial ξ$, change sign for those improved actions.

hep-lat

Transport Coefficients of Quark Gluon Plasma From Lattice Gauge Theory

Numerical results for the transport coefficients of quark gluon plasma are obtained by lattice simulations on on $16^3 \times 8$ lattice with the quench approximation where we apply the gauge action proposed by Iwasaki. The bulk viscosity is consistent with zero, and the shear viscosity is slightly smaller than the typical hadron masses. They are not far from the simple extrapolation on the figure of perturbative calculation in high temperature limit down to $T \sim T_{c}$. The gluon propagator in the confined and deconfined phases are also discussed.

hep-lat

Transport Coefficients of Quark Gluon Plasma for Pure Gauge Models

The transport coefficients of quark gluon plasma are calculated on a lattice 16**3X8, with the pure gauge models. Matsubara Green's functions of energy momentum tensors have very large fluctuations and about a few million MC sweeps are needed to reduce the errors reasonably small in the case of the standard action. They are much suppressed if Iwasaki's improved action is employed. Preliminary results show that the transport coefficients roughly depend on the coupling constant as a**(-3)(g) in the case of SU(2).

hep-lat