Spivak phrases it well (theorem 4.6, page 82):
If \(V\) has dimension \(n\), it follows that
^n(V). has dimension 1. Thus all alternating
\(n\)-tensors on \(V\) are multiples of any non-zero one. Since the
determinant is an example of such a member of ^n(V). it
is not surprising to find it in the following theorem:
Let v_1,…,v_nv_1,...,v_n be a basis for \(V\) and let
^n(V).. If w_i=_j=1^n
a_ijv_j. then
(w_1,…,w_n)=(a_ij)(v_1,…
v_n)omitted; see PDF
(see the examples for numerical verification of this).
Neither the zero \(k\)-form, nor scalars, are considered to be a
volume element.