SU(2)格点规范理论一种新作用量的弦张力的Monte Carlo计算

在10⁴格点上我们对作用量为S_p=sin1-sin(1/2)TrU_p的SU(2)格点规范系统进行了Monte Carlo模拟,计算了弦张力σ和标度常数Δ₀²之比。计算还表明,元格的平均内能和比热峰对于格点体积的变化来说是稳定的。 关键词：     

SU(2)格点规范理论几种不同形式的作用量的Monte Carlo研究

对SU(2)格点规范理论用三种不同于常用形式的作用量进行了Monte Carlo模拟,计算了平均内能和比热。内能曲线都趋向共同的弱耦合极限,都有比热峰标志着临界点。观察到仅由于格点间隔α的高次幂项不同而引起临界点明显漂移的现象。 关键词：     

三维X-Y模型的滞后标度和动态相变行为

采用Monte Carlo方法对3DX-Y模型进行数值模拟计算，研究了在非线性外场驱动下3DX-Y模 型的滞后标度和动态相变.得出了滞后标度关系为Area～h^α₀ωβ(1-T/T_c)^γ， 其中α=0.57，β=0.34，γ=0.90.发现其动态相变行为在一定的临界参数条件下，初始短周 期(周期数PN≤10)内的结果具有与Ising模型类似的对称性破缺；但在长周期内(PN≥200)的 结果则明显区别于Ising模型而与Heisenberg模型相近，也即无稳定动态有序铁磁相的存在. 关键词： X-Y模型 滞后标度 动态相变 Monte Carlo方法     

用SU(2)的分立子群对SU(2)格点规范新作用量的Monte Carlo 模拟

我们用SU(2)的正二十面体分立子群对SU(2)格点规范理论的正弦作用量与指数作用量进行了Monte Carlo模拟。发现由分立子群本身产生的一阶相变点分别在β_c′≈9.2±0.2和β_c′=6.8±0.2。对方格能量和比热所得的结果与用SU(2)群所得的结果一致。从而证实了对以上两种作用量,用分立子群代替连续群的适用性,为以后进行计算时利用分立子群提供了依据。 关键词：     

SU(3)格点规范理论两种新作用量的Monte Carlo研究

我们对SU(3)格点规范理论的两种新作用量进行了Monte Carlo模拟, 计算了元格平均内能和比热. 内能曲线都趋向共同的弱耦合极限, 比热都有峰. 我们观察到了由于格点间隔α的高次幂项不同引起的比热峰明显漂移的现象.     

变分累积展开方法中确定相变点的新方法

在计算有限温度SU(2)格点规范模型Polyakov线的过程中,考虑到变分累积展开法中有限距离相互作用效应与Monte Carlo中的有限体积效应的相似性,采用了新的方法来确定相变点.与已有的方法以及Monte Carlo模拟给出的结果比较,新方法给出的结果更接近Monte Carlo结果.     

格点定模SU(2)-Higgs模型的解析计算

对格点上基础表示的定模Higgs场与SU(2)规范场耦合系统的相图进行解析计算至累积展开的第四级,用扫瞄确定变分参数的方法,得到与Monte Carlo模拟很好符合的相图.计算了N_τ=1的有限温度情形下SU(2)-Higgs系统和纯SU(2)模型的Polyakov线,对后者得到迄今最佳的近似解析结果β_c.     

格点规范理论的平均场研究与普适性讨论

我们利用朴素的平均场近似方法与Shahbazyan提出的方法研究了格点规范理论的Manton作用量和其他几种作用量. 用平均场方法计算了几种SU(2)格点规范作用量的过渡点的β值, 用Shahbazyan提出的方法, 假设普适性存在, 直接由SU(2) Wilson作用量的Monte确良Carlo结果和几种作用量与Wilson作用量的关系, 得到这几种作用量过渡点的β值. 最后, 我们对用两种方法计算得到β_c值进行了比较, 作为对普适性假设的一个检验.     

SU(2)格点规范理论SIN作用量在有限温度下的解除禁闭的相变

我们对SU(2)群格点规范理论的Sinl-Sin((1/2)T_rU_p)作用量做了有限温度下的Monte Carlo计算,观察到一个高温下解除禁闭的相变。临界点是Tc≈334±40Mev,这与使用Wilson作用量及其它类型作用量所得结果可以相容。     

格点规范场论Monte Carlo模拟中一种节省时间的取样方法

我们在格点规范场理论的Monte Carlo模拟中引入了一种节省时间的取样方法,研究了该方法在Z₂规范群和SU(3)规范群临界点附近的行为,发现在越过一阶相变点时该方法将失效。按一定的程序,此特点可用来寻找一阶相变点。     

Influence of frustrations on the thermodynamic properties of the low-dimensional Potts model studied by computer simulation

Influence of disorder in the form of frustration on the thermodynamic behavior of a two-dimensional three-vertex Potts model has been studied by the Monte Carlo method, taking into account the nearest and next-nearest neighbors. Systems with linear sizes of L × L = N (L = 9–48) on a triangular lattice have been considered. It has been shown that in the case of J₁ > 0 and J₂ < 0 frustrations appear in the spin system within the interval of 0.5 ≤ |r| ≤ 1.0. The model undergoes a phase transition outside this region.     

Topology and universality in the lattice CP2 model

The topological susceptibility χ_t and the correlation length ξ in the CP² model on a two-dimensional triangular lattice are calculated by the Monte Carlo simulation method. Using variant lattice actions, we verify the universality of the dimensionless quantity χ_tξ² ～- 0.09 in the scaling region, thus indicating the presence of physical topological effects in the scaling limit. As a by-product, we obtain a combinatorial formula for the topological charge.     

CPN−1 coupled to gauge fields: Mean field theory and monte carlo results

We define a two parameter lattice field theory which interpolates between the O (2N) Heisenberg model, pure U(1) gauge theory, and a lattice version of the CP^N?1 model. The phase diagram in space-time dimension d=4 is obtained by Monte Carlo simulation on a 4⁴ lattice, and the nature of the phases is discussed in mean field approximation.     

The string tension of compact U(1) four-dimensional lattice gauge theory

Monte Carlo simulations of the string tension are calculated for four-dimensional U(1) gauge theory on a 6⁴ lattice. The string tension follows the result -1n(β/2) in the high temperature region and is zero for β > β_c, where β_c is the critical inverse temperature.     

The percolation mechanism for fragmentation of nuclei using Monte Carlo technique

A statistical bond-percolation model for the fragmentation has been applied to the proton-induced reactions assuming a lattice structure to the prefragment nucleus and using the Monte Carlo technique to determine the bond to be broken. The model succeeded to reproduce the essential features of the mass yield curves for the p-Cu reaction at 3.9 GeV and to describe qualitatively the charge and the multiplicity distributions of the projectile fragments for the ²⁸Si interactions with the quasi-free emulsion nucleon at 3.7 AGeV.     

Modified action glueballs

The mass of the 0⁺ glueball in 4-dimensional lattice gauge theory with a mixed SU(2)-SO(3) action is obtained via Monte Carlo. We work in a region far from the critical end point in the phase diagram, with an action partly motivated by renormalization group flows in the Migdal-Kadanoff approximation. A large-N resummation of perturbation theory is used to show that the mass gap scales as predicted by the perturbative renormalization group. Independent of this, our results show that the ratio of the glueball mass to the square root of the string tension, obtained from a previous Monte Carlo, is a renormalization group invariant.     

Quantum corrections for lattice gases

Classical lattice gases consisting of structureless particles (with spin) have been quantized by introducing a kinetic energy operator that produces nearest-neighbor hops. Systematic quantum corrections for the partition function and the particle distribution functions appear naturally as power series inX = ²/2ml ² ( ^–1 =k _B T,m is the mass,l is a distance related to lattice spacing). These corrections require knowledge of certain particle displacement probabilities in the corresponding classical lattice gases. Leading-order corrections have been derived in forms that should facilitate their use in computer simulation studies of lattice gases by the standard Monte Carlo method.     

AnSU(2)l ⊗SU(2)r symmetric Yukawa model in the symmetric phase

The lattice regularizedSU(2)l ?SU(2)r symmetric scalar fermion model with explicit mirror fermions is investigated in the phase with unbroken symmetry. In the present work numerical Monte Carlo calculations with dynamical fermions are performed on 4³·8 and 4³·16 lattices near the expected perturbative Gaussian fixed point. The bare Yukawa coupling of the mirror fermion is fixed at zero. Global symmetries of the model are discussed, and the numerical results are supported by lattice perturbation theory.     

Vortex free energy and string tension at strong and intermediate coupling

We present results of high temperature expansions up to order g^?24 for the vortex free energy respectively string tension in pure lattice gauge theories with gauge groups SU(2) and Z₂ in 3 and 4 dimensions. For SU(2) in 4 dimensions the result is compared with Monte Carlo calculations of Creutz and is in good agreement. An intermediate coupling region is seen, where the string tension smoothly interpolates between strong coupling and weak coupling behaviour.     

Application of the multicanonical multigrid Monte Carlo method to the two-dimensional φ4: Autocorrelations and interface tension: Autocorrelations and interface tension

We discuss the recently proposed multicanonical multigrid Monte Carlo method and apply it to the scalar ⁴ on a square lattice. To investigate the peformance of the new algorithm at the field-driven first-order phase transitions between the two ordered phases we carefully analyze the autocorrelations of the Monte Carlo process. Compared with standard mlticanonical simulations a real-time improvement of about one order of magnitude is established. The interface tension between the two ordered phases is extracted from highstatistics histograms of the magnetization applying histogram reweighting techniques.