By hypothesis, the \(F\)-vector space
\begin{equation*}
W_F = \Hom_{F}(V_1 \otimes_{E} F, V_2 \otimes_{E} F),
\end{equation*}
on which \(G\) acts by the formula \(T^g(x) = T(x^{g^{-1}})^g\text{,}\) contains an invariant vector which, as a linear transformation, is invertible. Now \(W_F\) can also be written as
\begin{equation*}
W \otimes_E F, \qquad W = \Hom_{E}(V_1, V_2).
\end{equation*}
The fact that \(W_F\) has an invariant vector says that a certain set of linear equations has a nonzero solution over \(F\text{,}\) namely the equations that express the fact that the action of \(G\) leaves the vector invariant. But those equations have coefficients in \(E\text{,}\) so
\begin{equation*}
W^G \otimes_E F = W_F^G;
\end{equation*}
in particular, the space of invariant vectors in \(W\) is also nonzero.
It remains to check that some element of
\(W^G\) corresponds to a map
\(V_1 \to V_2\) which is actually an isomorphism; for this, we argue as in
Exercise 3. Fix an isomorphism of vector spaces between
\(V_2 \otimes_{E} F\) and
\(V_1 \otimes_{E} F\) (which need not respect the
\(G\)-action). By composing each element of
\(W\) with this isomorphism and taking the determinant, we get a well-defined polynomial function on
\(W\text{,}\) which we can restrict to
\(W^G\text{.}\) By hypothesis, this function is not identically zero on
\(W_F^G\text{,}\) so (because
\(E\) is infinite) it cannot be identically zero on
\(W^G\) either.