A Feynman integral in Lifshitz-point and Lorentz-violating theories in $R^D\oplus R^m$

We evaluate a one-loop, two-point, massless Feynman integral $I_{D,m}(p,q)$ relevant for perturbative field theoretic calculations in strongly anisotropic $d=D+m$ dimensional spaces given by the direct sum $\mathbb R^D\oplus\mathbb R^m$. Our results are valid in the whole convergence region of the integral for generic (non-integer) co-dimensions $D$ and $m$. We obtain series expansions of $I_{D,m}(p,q)$ in terms of powers of the variable $X:=4p^2\mathrm{/}{q}^4$, where $p=|\bm p|$,$q=|\bm q|$,$\bm p\in\mathbb R^D$,$\bm q\in\mathbb R^m$, and in terms of generalised hypergeometric functions ${}_3{F}_2(-X)$, when $X<1$. These are subsequently analytically continued to the complementary region $X\ge 1$. The asymptotic expansion in inverse powers of $X^{1\mathrm{/}2}$ is derived. The correctness of the results is supported by agreement with previously known special cases and extensive numerical calculations.