The analytical properties of the lattice Green function for the fully anisotropic honeycomb lattice are studied, where (α 1, α 2, α 3) are anisotropy parameters with {α j ∈ (0, ∞): j = 1, 2, 3}, and w = u + iv is a complex variable in a (u, v) plane. This integral defines a single-valued analytic function G H(α 1, α 2, α 3; w) provided that a cut is made along the real axis from u = −(α 1 + α 2 + α 3) to u = (α 1 + α 2 + α 3). We show that G H(α 1, α 2, α 3; w) is a solution of a second-order linear differential equation with ten ordinary regular singular points and four apparent singular points. The apparent singularities are removed by constructing a particular differential equation of fourth order. Next, the series solution where |w| > (α 1 + α 2 + α 3), and is introduced. It is proved that, in general, satisfies a five-term linear recurrence relation. The asymptotic behaviour of as n → ∞ is also established. In order to determine the behaviour of G H(α 1, α 2, α 3; w) along the edges of the cut we define the limit function where u ∈ [−(α 1 + α 2 + α 3), (α 1 + α 2 + α 3)]. Integral representations are established for and . In particular, it is found that where J 0(z) and Y 0(z) denote Bessel functions of the first and second kind, respectively, and u ∈ (0, α 1 + α 2 + α 3). It is also demonstrated that the piecewise functions and can be sectionally evaluated exactly for all u ∈ (0, α 1 + α 2 + α 3), in terms of complete elliptic integrals of the first kind K(k), where k 2 ≡ k 2(α 1, α 2, α 3, u) is a rational function of (α 1, α 2, α 3) and u. Finally, applications of the results are made to the lattice Green function for the fully anisotropic simple cubic lattice, and to the theory of Pearson random walks in a plane. In particular, various Bessel function integrals are evaluated in order to derive a new exact formula for the mean end-to-end distance of a general three-step random walk.
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