The answer to both of your questions is yes! This can be seen through the construction of the top exterior bundle via transition functions.
The top exterior power of a vector bundle
$\Lambda^n E$ of a rank $n$ vector bundle $E$ has transition functions $\wedge^n g_{UV}:U\cap V\to\text{GL}(\wedge^n\mathbb{C}^n) = \mathbb{C}^*$ where $g_{UV}$ are the transition functions coming from $E$. This immediately implies what we are looking at is a line bundle and the expansion is shown cleanly as;
\begin{align*}
(\wedge^ng_{UV})(e_1\wedge\dots\wedge e_n)
&= \wedge_{i=1}^ng_{UV}(e_i) \\
&= \wedge_{i=1}^n\left(\sum_{j=1}^n g_{ji}e_j\right)\\
&= \left[\sum_{\sigma \in S_n}(-1)^{|\sigma|}\prod_{i=1}^n g_{i\sigma(i)}\right] \wedge_{i=1}^ne_i \\
&= \det(g_{UV})\cdot e_1\wedge\dots\wedge e_n.
\end{align*}
where the $e_i$'s denote the standard basis vectors and we have made use of the relations
\begin{align*}
\alpha\wedge\alpha &= 0\\
\alpha\wedge\beta &= -\beta\wedge\alpha
\end{align*} for any $\alpha,\beta\in \Omega^1(E)$.
This line bundle is, for now apparent reasons, known as the determinant bundle of $M$ and is also denoted $\det(E)$.
Finally, saying that $E$ having trivial determinant means that the determinant bundle of $E$ is a trivial bundle.
Note that the notion of top exterior power (for a vector space) is in fact the formal definition of determinant. That is the determinant is the unique multi-linear functional acting on $n$ vectors in an $n$-dimensional space which is alternating and whose evaluation on the standard basis is 1 (i.e. preserves the volume of the unit cube).