For any $q\in \Imm$ we can associate a varifold $\mu_q\in\mathcal{M}(\mathbb R^3\times S^{2})$ as the push forward measure $\mu_q:= (q,n_q)_*\operatorname{vol}_q$ where $n_q$ is the Gauss of $q$.
Thus, for a test function $\omega\in C_1(\R^3\times S^2, \R)$,
$$\mu_q(\omega) = \int_M \omega(q,n_q) \operatorname{d} \operatorname{vol}_q .$$
By a change of variables, for any $\gamma\in\Diff$, $\mu_{q\circ\gamma} = \mu_q$.
To represent a varifold with a fixed finite dimension requires solving a quantization problem. Thus, we cannot directly use the varifold representations.
We may equip $\mathcal{M}(\mathbb R^3\times S^{2})$ with an RKHS norm $\|\cdot\|_V$.