  For Toeplitz operators $T_f^{(t)}$ acting on the weighted Fock space $H_t^2$,
we consider the semi-commutator $T_f^{(t)}T_g^{(t)}-T_{fg}^{(t)}$, where $t>0$
is a certain weight parameter that may be interpreted as Planck's constant
$\hbar$ in Rieffel's deformation quantization. In particular, we are interested
in the semi-classical limit \tag{$*$}\lim\limits_{t\to
0}\|T_f^{(t)}T_g^{(t)}-T_{fg}^{(t)}\|_t. It is well-known that
$\|T_f^{(t)}T_g^{(t)}-T_{fg}^{(t)}\|_t$ tends to $0$ under certain smoothness
assumptions imposed on $f$ and $g$. This result was extended to $f,g \in
\mathrm{BUC}(\mathbb{C}^n)$ in a recent paper by Bauer and Coburn. We now
further generalize this result to (not necessarily bounded) uniformly
continuous functions and symbols in the algebra $\mathrm{VMO} \cap L^{\infty}$
of bounded functions having vanishing mean oscillation on $\mathbb{C}^n$. Our
approach is based on the algebraic identity
$T_f^{(t)}T_g^{(t)}-T_{fg}^{(t)}=-(H_{\bar{f}}^{(t)})^*H_g^{(t)}$, where
$H_g^{(t)}$ denotes the Hankel operator corresponding to the symbol $g$, and
norm estimates in terms of the (weighted) heat transform. As a consequence,
only $f$ (or likewise only $g$) has to be contained in one of the above classes
for $(*)$ to vanish. For $g$ we only have to impose $\limsup_{t \to
0}\|H_g^{(t)}\|_t<\infty$, e.g. $g \in L^{\infty}(\mathbb{C}^n)$. We prove that
the set of all symbols $f\in L^{\infty}(\mathbb{C}^n)$ with the property that
$\lim_{t \rightarrow 0}\|T^{(t)}_fT^{(t)}_g-T^{(t)}_{fg}\|_t=\lim_{t\to
0}\|T_g^{(t)}T_f^{(t)}-T_{gf}^{(t)}\|_t=0$ for all $g\in
L^{\infty}(\mathbb{C}^n)$ coincides with $\mathrm{VMO}\cap L^{\infty}$.
Additionally, we show that $\lim_{t\to 0}\|T_f^{(t)}\|_t=\|f\|_{\infty}$ holds
for all $f\in L^{\infty}(\mathbb{C}^n)$. Finally, we present new examples,
including bounded smooth functions, where $(*)$ does not vanish.
