Let $k$ be a finite field of sufficiently large characteristic, $F = k((t))$ and $\mathfrak{o} = k[[t]]$. Let $G$ be a reductive algebraic group defined over $\mathfrak{o}$. Roughly stated, for sake of brevity, the Lie algebra fundamental lemma of Ngô states there is an equality of the form $$ \mathcal{O}^\kappa_a = q^r\mathcal{SO}_{a_H} $$ where $\mathcal{O}^\kappa$ is a $\kappa$-orbital integral for $G$ and $\mathcal{SO}$ is a stable orbital integral for an endoscopic group $H$ associated to $\kappa$ (or more precisely and endoscopic datum). Here $\kappa$ is a character of a cohomology group associated to stable conjugacy class $a$ in $\mathrm{Lie}(G)(F)$, and $a_H$ is the corresponding conjugacy class in $\mathrm{Lie}(H)(F)$. A more detailed and precise formulation is in [1], but this should suffice for the question.
Consider transfer factor $q^r$ in front of the stable orbital integral: it is a simple power of $q$ and $r$ depends on $a$ and $a_H$ (the number $r$ is the difference in dimensions of the associated affine Springer fibers).
Is there a relatively simple, perhaps 'geometric' explanation or heuristic of why the transfer factor in the fundamental lemma is a simple power of $q$, as opposed to another polynomial in $q$ such as e.g. $q^{r_1} + 2q^{r_2}$ where $r_1$ and $r_2$ just depend on $a$ and $a_H$?
Hales' paper [2] is a good relatively nontechnical summary of the fundamental lemma that briefly discusses this transfer factor but doesn't quite answer this question.
[1] Ngô, Bao Châu. Le lemme fondamental pour les algèbres de Lie. Publ. Math. Inst. Hautes Études Sci. No. 111 (2010), 1-169
[2] Hales, Thomas C. The fundamental lemma and the Hitchin fibration [after Ngô Bao Châu]. Séminaire Bourbaki: Vol. 2010/2011. Exposés 1027–1042. Astérisque No. 348 (2012), Exp. No. 1035, ix, 233-263.