For everything to be well defined you need $L\lvert_{V_1}$ to be a map $V_1\to V_1$, otherwise the determinant does't exist. But with this there is no need to restrict to a subspace at all, if the statement holds for any map $L:\mathbb R^d\to\mathbb R^d$ then it also holds for the restriction to any subspace, as you will be in the same situation.
In finite dimensional spaces $\|L\|$ is the magnitude value of the largest (in absolute value) eigenvalue of $L$. The determinant is the product over all eigenvalues with multiplicity corresponding to the algebraic multiplicity of that eigenvalue. If $L$ is invertible then the eigenvalues of $L^{-1}$ are the inverses of the eigenvalues of $L$.
Put everything together:
$$\|L^{-1}\|^{-1}=(\sup_{\lambda \text{ EV of }L}|\lambda^{-1}|)^{-1}=\inf_{\lambda\text{ EV of }L}|\lambda|\\
\det(L)=\prod_{\lambda\text{ EV of }L}\lambda\implies |\det(L)|=\prod_{\lambda \text{ EV of }L}|\lambda|\\
\|L\|=\sup_{\lambda\text{ EV of }L}|\lambda|$$
One has for any eigenvalue $\lambda$ that $0≤\|L^{-1}\|^{-1}≤|\lambda|≤\|L\|$, taking the product over all eigenvalues gives then:
$$(\|L^{-1}\|^{-1})^d≤|\det(L)|≤\|L\|^d$$
In the case that $L\lvert_{V_1}$ is not a map $V_1\to V_1$ but a map $V_1\to V_2$ for some $V_2\subset V$ we do something similar. Since $L$ is invertible $V_1$, $V_2$ are isomorphic finite dimensional subspaces of $V=\mathbb R^n$. They inherit the inner product of $\mathbb R^n$ and are actually unitarily isomorphic as Hilbert spaces, so let $U: V_2\to V_1$ be such a unitary isomorphism. You have:
$$\|UL\lvert_{V_1}\|=\|L\lvert_{V_1}\|\qquad \|L\lvert_{V_1}^{-1}U^{-1}\|=\|L\lvert_{V_1}^{-1}\|\\
\mathrm{vol}(UL\lvert_{V_1}v_1,..,UL\lvert_{V_1}v_n)=\mathrm{vol}(L\lvert_{V_1}v_1,..,L\lvert_{V_1}v_n)\implies \det(UL\lvert_{V_1})=\det(L\lvert_{V_1})$$
all from the virtue of $U$ being unitary. This means we have reduced to the situation considered before, here $UL\lvert_{V_1}$ is our map $V_1\to V_1$ for which the inequality holds.