TITLE: Prove known closed form for $\int_0^\infty e^{-x}I_0\left(\frac{x}{3}\right)^3\;dx$
QUESTION [12 upvotes]: I know that the following identity is correct, but I would love to see a derivation:
$$\int_0^\infty e^{-x}I_0\left(\frac{x}{3}\right)^3\;dx=\frac{\sqrt{6}}{32\pi^3}\Gamma\left(\frac{1}{24}\right)\Gamma\left(\frac{5}{24}\right)\Gamma\left(\frac{7}{24}\right)\Gamma\left(\frac{11}{24}\right)\tag{1}$$
where $I_0(x)$ is a modified Bessel function of the first kind. The form of the RHS makes me assume that the elliptic integral singular value $K(k_6)$ is somehow involved but I see no obvious way of transforming the LHS into an elliptic integral. My request is to see a way of evaluating this integral directly to show that it equals the RHS.

Background: This integral arises in the theory of the recurrence of random walks on a cubic lattice. Jonathan Novak elegantly shows here using generating functions that the recurrence probability of a random walk on $\mathbb{Z}^d$ is $p(d)=1-\frac{1}{u(d)}$ where:
$$u(d)=\int_0^\infty e^{-x}I_0\left(\frac{x}{d}\right)^d\;dx\tag{2}$$
The MathWorld page lists several ways of writing $u(3)$, including $(1)$, but in none of the references could I find a specific derivation of $(1)$. Most relevant discussions I found (e.g. here and here where elliptic integrals do appear) work from an alternative way of writing $u(3)$, namely:
$$u(3)=\frac{3}{2\pi^3}\int_{-\pi}^\pi\int_{-\pi}^\pi\int_{-\pi}^\pi\frac{dx\;dy\;dz}{3-\cos{x}-\cos{y}-\cos{z}}\tag{3}$$
rather than a representation like $(2)$. I believe $(3)$ comes from an alternative way of solving the random walk problem (e.g. see here) which I am not very familiar with. Accordingly, I am asking for a derivation of $(1)$ that works directly from the Bessel function integral, rather than considering other ways of calculating $u(3)$ (deriving the RHS of $(1)$ from $(3)$ would not answer my question). Although I appreciate that there may be simpler proofs of $(1)$ from the theory of random walks, I am wondering if there is a nice way of evaluating the integral in $(1)$ directly.

REPLY [2 votes]: I am having hesitations whether I should be writing this post because I will definitely not derive the closed form in question. Yet, after having glanced through all the material linked to this question I guess  I am able to contribute more than all what I have seen so far. We start from the formula (3) since the route from (1) to (3) is fairly simple and has been presented in the comments already.
\begin{eqnarray}
u(3) &=& \int\limits_{[0,\pi]^3} \frac{1}{3-\cos(t)-\cos(u)-\cos(v)} dt du dv\\
&=&-\pi \int\limits_{[0,\pi]^2} \frac{1}{\sqrt{-4+\cos(t)+\cos(u)}\sqrt{-2+\cos(t)+\cos(u)}} dt du\\
&\underbrace{=}_{v=\tan(u/2)}& 2\pi \int\limits_{[0,\pi] \times [0,\infty)} \frac{1}{\sqrt{(-3-5 v^2+(1+v^2) \cos(t))(-1-3 v^2 +(1+v^2) \cos(t))}}dt dv\\
&=& 2\pi \int\limits_{[0,\pi] \times [0,\infty)} \frac{1}{\sqrt{5-6 \cos(t)+\cos(t)^2}}\cdot \frac{1}{\sqrt{(1+v^2)(1+v^2 \frac{(\cos(t)-3)^2}{(\cos(t)-5)(\cos(t)-1)}}} dt dv\\
&=& 2\pi \int\limits_{[0,\pi]} \frac{K(-\frac{4}{5-6 \cos(t)+\cos(t)^2})}{\sqrt{5-6 \cos(t)+\cos(t)^2}} dt\\
&\underbrace{=}_{v=\tan(t/2)}& 2\pi \int_{[0,\infty)} \frac{K(-\frac{(1+v^2)^2}{v^2(2+3 v^2)})}{v\sqrt{2+3 v^2}} dv\\
&\underbrace{=}_{z=-\frac{(1+v^2)^2}{v^2(2+3 v^2)}}& \frac{\pi}{2} \int\limits_{(-\infty,-1/3)} \sqrt{\frac{-1+3 z-3\sqrt{z(-1+z)}}{(1+3z)(-1+z)z}} K(z) dz\\
&=& \frac{\pi}{2} \int\limits_{(-\infty,-1/3)} \sqrt{\frac{-1+3 z-3\sqrt{z(-1+z)}}{(1+3z)(-1+z)z}} \frac{1}{\sqrt{1-z}}K(\frac{z}{z-1}) dz\\
&\underbrace{=}_{y=z/(z-1)}&\frac{\imath \pi}{2} \int\limits_{(1/4,1)} \frac{K(y)}{\sqrt{y(1-3 \sqrt{y}+2 y)}}dy\\
&\underbrace{=}_{y\leftarrow \sqrt{y}}& \imath \pi \int\limits_{(1/2,1)} \frac{K(y^2)}{\sqrt{(1-y)(1-2 y)}} dy\\
&\underbrace{=}_{y\leftarrow 2y-1}& \frac{\pi}{\sqrt{2}} \int\limits_{(0,1)} \frac{K(\frac{(1+y)^2}{4})}{\sqrt{(1-y)y}} dy\\
&\underbrace{=}_{y\leftarrow \sqrt{y}}&\pi \sqrt{2} \int\limits_{(0,1)}\frac{K(\frac{(1+y^2)^2}{4})}{\sqrt{1-y^2}} dy\\
&\underbrace{=}_{y=\sin(\phi)}& \int\limits_{(0,\pi/2)} K\left( \frac{(1+\sin(\phi)^2)^2}{4}\right) d\phi\\
&\underbrace{=}_{\phi=\phi/2}& \frac{\pi \sqrt{2}}{4} \int\limits_{[-\pi,\pi]} K\left( \frac{19}{32} - \frac{3}{8} \cos(\phi)+\frac{1}{32} \cos(2 \phi)\right) d\phi\\
&\underbrace{=}_{z=\exp(\imath \phi)}& \frac{\pi \sqrt{2}}{4} \oint\limits_{|z|=1}K\left(\frac{19}{32} - \frac{3}{8}\frac{z+1/z}{2}+\frac{1}{32} \frac{z^2+1/z^2}{2} \right) \frac{dz}{\imath z}
\end{eqnarray}
I guess all the steps are pretty clear. The last expression lends itself for Cauchy-residue theorem computations. However, for the time being my knowledge of the singularities of the elliptic function is not sufficient to be able to complete this computation.