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首页> 外文期刊>Journal of physics, A. Mathematical and theoretical >Application of Mahler measure theory to the face-centred cubic lattice Green function at the origin and its associated logarithmic integral
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Application of Mahler measure theory to the face-centred cubic lattice Green function at the origin and its associated logarithmic integral

机译:马勒测度理论在面心立方晶格格林函数的原点及其对数积分中的应用

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The mathematical properties of the face-centred cubic lattice Green function G(w) ≡ 1/π ~3 ∫ ~π _0 ∫ π _0 ∫ π _0 dθ _1 dθ _2 dθ _3/w - c(θ1) c(θ _2) - c(θ _2) c(θ _3) - c(θ _3) c(θ _1) and the associated logarithmic integral S(w) ≡ 1/π ~3 ∫ ~π _0 ∫ π _0 ∫ π _0 ln[w - c(θ _1) c(θ _2) - c(θ _2) c(θ _3) -c(θ _3) c(θ _1)] dθ _1 dθ _2 dθ _3 are investigated, where c(θ) ≡ cos(θ) and w = w 1+iw 2 is a complex variable in the w plane. In particular, the theory of Mahler measures is used to obtain a closed-form expression for S(w) in terms of 5F_4 generalized hypergeometric functions. The method of analytic continuation is then applied to this result in order to prove that S(3) = -14/15 ln 2 + 8/5 ln 3 8/135 5F 4 [4/3, 3/2, 5/3, 1, 1; 1 2, 2, 2, 2]. Next the relation dS/dw = G(w), where w = (3,+∞), is used to derive the simple formula G(w) = 1/w { _2F ~1 1/6, 1/3; 1; 27(w + 1)/4w ~3}2, where w lies in a restricted region R1 of the cut w plane. The limit function G- (w1) ≡ lim ε → 0+ G(w1 iε) = GR(w1) + iGI(w1) is also evaluated in the intervals w1 ε (-1, 0] and w1 ε (0, 3]. It is shown that GR(w1) and GI(w1) can be expressed in terms of 2F1[z(w1)] hypergeometric functions, where the independent variable z(w1) is a real-valued rational function of w 1. Finally, new formulae are derived for the number of random walks r _n on the face-centred cubic lattice which return to their starting point (not necessarily for the first time) after n nearest-neighbour steps.
机译:面心立方晶格Green函数G(w)≡1 /π〜3∫〜π_0∫π_0∫π_0dθ_1dθ_2dθ_3 / w-c(θ1)c(θ_2) -c(θ_2)c(θ_3)-c(θ_3)c(θ_1)和相关对数积分S(w)≡1 /π〜3∫〜π_0∫π_0∫π_0 ln [w -c(θ_1)c(θ_2)-c(θ_2)c(θ_3)-c(θ_3)c(θ_1)]dθ_1dθ_2dθ_3,其中c(θ)≡cos (θ)和w = w 1 + iw 2是w平面上的复变量。特别地,根据5F_4广义超几何函数,使用了Mahler测度的理论来获得S(w)的闭式表达式。为了证明S(3)= -14/15 ln 2 + 8/5 ln 3 8/135 5F 4 [4/3,3/2,5/3 ,1,1; 1 2、2、2、2]。接下来,关系式dS / dw = G(w),其中w =(3,+∞),用于得出简单公式G(w)= 1 / w {_2F〜1 1/6,1/3; 1; 27(w +1)/ 4w〜3} 2,其中w位于切割的w平面的限制区域R1中。极限函数G-(w1)≡limε→0+ G(w1iε)= GR(w1)+ iGI(w1)也在区间w1ε(-1,0]和w1ε(0,3结果表明,GR(w1)和GI(w1)可以用2F1 [z(w1)]超几何函数表示,其中自变量z(w1)是w 1的实值有理函数。最后,针对以面为中心的立方晶格上的随机游动数r _n推导新公式,这些随机游程r _n在n个最近邻居步长之后返回其起点(不一定是第一次)。

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