Expressing invertible maps $\bigwedge^{d-1} V \to \bigwedge^{d-1} V$ as $\bigwedge^{d-1}A$ for some $A$ Let $V$ be a real $d$-dimensional vector space, let $\bigwedge^{d-1} V$ be its exterior power. Consider the following claim:

Proposition: If $d$ is even, then every invertible linear map $\bigwedge^{d-1} V \to \bigwedge^{d-1} V$ equals $\bigwedge^{d-1}A$ for some $A \in \text{GL}(V)$. If $d$ is odd, then every orientation-preserving*  invertible map $\bigwedge^{d-1} V \to \bigwedge^{d-1} V$ equals $\bigwedge^kA$ for some $A \in \text{GL}(V)$. 

I found a proof for the above proposition, but it is based on endowing $V$ with an inner product, which I don't like very much.  Since there is no mention of products in the claim, it's natural to expect a metric-free proof.
Is there such a proof?
Edit:
Here is an argument for showing that when $d$ is odd, it is impossible to express orientation-reversing maps $\bigwedge^{d-1} V \to \bigwedge^{d-1} V$ as "$(d-1)$-wedge" of a map $V \to V$.
Let $A:V \to V$. Since $$\det (\bigwedge^k A)=(\det A)^{\binom{d-1}{k-1}},$$ we get for $k=d-1$ that
$$ \det (\bigwedge^{d-1} A)=(\det A)^{\binom{d-1}{d-2}}=(\det A)^{d-1},$$
so if $d$ is odd, we see that $\det (\bigwedge^{d-1} A)$ is always positive, whether or not $A$ was orientation-preserving to begin with.

*Note there is no need for a choice of orientation on $\bigwedge^{d-1} V$ to define which maps $\bigwedge^{d-1} V \to \bigwedge^{d-1} V$ are orientation preserving. (If you like you can put the same orientation on "both sides", it does not matter which).
 A: Consider the perfect pairing $\left< \cdot, \cdot \right> \colon V \times \bigwedge^{d-1}(V) \rightarrow \bigwedge^d(V)$ given by the wedge product $\left<v, \omega \right> = v \wedge \omega$. The adjugate of a linear map $T \colon V \rightarrow V$ is characterized by the property that it is the adjoint map to $\bigwedge^{d-1}(T)$ with respect to $\left< \cdot, \cdot \right>$. That is, we have
$$ \left< \operatorname{adj}(T)v, \omega \right> = \left<v, \bigwedge\nolimits^{d-1}(T)\omega \right> $$
for all $v \in V$ and $\omega \in \bigwedge^{d-1}(V)$. Using this definition, one can prove directly that 
$$\operatorname{adj}(T) \circ T = T \circ \operatorname{adj}(T) = \det(T) I$$
and
$$ \operatorname{adj}(\operatorname{adj}(T)) = \det(T)^{d-2} T. $$
I'll assume that $d$ is even and show that given any invertible map $S \colon \bigwedge^{d-1}(V) \rightarrow \bigwedge^{d-1}(V)$ we can find an invertible map $T \colon V \rightarrow V$ such that $\bigwedge^{d-1}(T) = S$. Since the pairing is perfect, there exists a (unique) map $R \colon V \rightarrow V$ which is adjoint to $S$ so that
$$ \left< Rv, \omega \right> = \left< v, S\omega \right> $$
for all $v \in V$ and $\omega \in \bigwedge^{d-1}(V)$. Note that $R$ must also be invertible. Define $T = \det(R)^{\frac{2-d}{d-1}}\operatorname{adj}(R)$. Then we have
$$ \operatorname{adj}(T) = \det(R)^{2 - d} \operatorname{adj}(\operatorname{adj}(R)) = \det(R)^{2-d} \det(R)^{d - 2} R = R $$
so
$$ \left< v, S\omega \right> = \left< Rv, \omega \right> = \left< \operatorname{adj}(T)v, \omega \right> = \left< v, \bigwedge\nolimits^{d-1}(T) \omega \right> $$
for all $v \in V$ and $\omega \in \bigwedge^{d-1}(V)$ which shows that $S = \bigwedge^{d-1}(T)$.
In general, one can show that $\det(R) = \det(S)$ (where $R,S$ are adjoint with respect to $\left< \cdot, \cdot \right>$, just like one has with an inner product). When $d$ is odd, $d - 1$ is even so the previous argument works only if $\det(R) > 0$ (because we need to take an even square root) which will happen if and only if $\det(S) > 0$. 
