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arXiv math-ph/0503057math-phcond-mat.softhep-thmath.MP
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紧化$λϕ^4$理论的临界性态

Critical behaviour of the compactified $λϕ^4$ theory

L. M. Abreu, C. de Calan, A. P. C. Malbouisson, J. M. C. Malbouisson, A. E. Santana

摘要:

研究了$N$分量欧氏$λϕ^4$模型在首阶$\frac{1}{N}$展开式下的临界行为.我们认为它在三种情况下:限制在两个平行的平面之间的距离$L$彼此分开,限制在一个无限长的圆柱体具有正方形横截面面积$A$和体积$V$的立方体盒。以质量项的形式$m_{0}^2=α(T - T_{0})$,我们检索金斯堡-朗道模型,这是应该描述样品的材料经历相变,分别在一个薄膜,一个线和一个晶粒的形式,其体积转变温度($T_{0}$)是已知的。我们得到的方程的临界温度作为$L$(膜),$A$(线),$V$(粮食)和$T_{0}$的功能,并确定维持过渡的极限尺寸。

英文摘要:

We investigate the critical behaviour of the $N$-component Euclidean $λϕ^4$ model at leading order in $\frac{1}{N}$-expansion. We consider it in three situations: confined between two parallel planes a distance $L$ apart from one another, confined to an infinitely long cylinder having a square cross-section of area $A$ and to a cubic box of volume $V$. Taking the mass term in the form $m_{0}^2=α(T - T_{0})$, we retrieve Ginzburg-Landau models which are supposed to describe samples of a material undergoing a phase transition, respectively in the form of a film, a wire and of a grain, whose bulk transition temperature ($T_{0}$) is known. We obtain equations for the critical temperature as functions of $L$ (film), $A$ (wire), $V$ (grain) and of $T_{0}$, and determine the limiting sizes sustaining the transition.

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