Let $V,W$ be $d$-dimensional vector spaces, and let $A,B \in \text{Hom}(V,W)$.
Consider the induced maps on the exterior algebras: $\bigwedge^{d-1}A,\bigwedge^{d-1}B :\Lambda_{d-1}(V) \to \Lambda_{d-1}(W)$.
Suppose that $\bigwedge^{d-1}A=\bigwedge^{d-1}B$, and that $A,B$ are invertible.
I want to prove that $A=\pm B$. (Note that this implies $A=B$ in the case $d$ is even).
The assumption implies $$\bigwedge^{d-1}(AB^{-1})=\text{Id}_{\Lambda_{d-1}(V)}.$$
Hence, the problem reduces to showing that for $S \in \text{GL}(V)$ ,$$\bigwedge^{d-1}S=\text{Id}_{\Lambda_{d-1}(V)} \Rightarrow S=\pm \text{Id}_V.$$
I can show this by introducing an inner product and orientation on $V$, but this seems "unnatural" to me.
Is there a proof which avoids this?
Let us consider the reduced version. We have $S\in \text{GL}(V)$ such that $$\bigwedge^{d-1}S=\text{id}.$$ In particular, this means that every $d-1$-dimensional subspace is invariant under $S$. On the other hand, for any $v,w\in V$ such that $w\not\in\langle v\rangle$, there is a $d-1$-dimensional subspace containing $v$ but not $w$. It thus follows that every element of $V$ is an eigenvector of $S$, and so, $S$ is multiplication by a scalar $\alpha$. Finally, we must have $\alpha^{d-1}=1$.
As pointed out by Gunnar, this does not necessarily mean that $\alpha=\pm1$ if we allow fields with more roots of unity.