We obtain the same sheaf of differential forms on ${X^{\rm an}}$ as in [CD12], §3. In the latter reference, all analytic moment maps were used to define differential forms on ${X^{\rm an}}$ and so it is clear that our differential forms here are also differential forms in the sense of [CD12]. To see the converse, we argue as follows: By Proposition 4.16, tropical charts $(V,\varphi_{U})$ form a basis in ${X^{\rm an}}$. It follows from Proposition 7.2 that an analytic moment map $\varphi:V\rightarrow({\mathbb{G}}_{m}^{r})^{\rm an}$ may be locally in $x\in V$ approximated by an algebraic moment map $\varphi^{\prime}:U^{\prime}\rightarrow{\mathbb{G}}_{m}^{r}$ such that $(\varphi^{\prime})_{\rm trop}={\rm trop}\circ\varphi$ in an open neighbourhood of $x$ in $V$. Here, $U^{\prime}$ is a suitable very affine open subset of $U$ with $x\in(U^{\prime})^{\rm an}$. It follows from [CD12], Lemma 3.1.10, that we may use algebraic moment maps to define differential forms in the sense of [CD12]. Using that $\varphi_{U^{\prime}}$ factorizes through $\varphi^{\prime}$ (see 4.12), we get the claim.