Consider the determinant of the euclidean form of the Dirac operator:
$$\text{det}(iD), \quad iD = i\gamma_{\mu}(\partial_{\mu}+A_{\mu})$$
It is an elliptic operator, so has a discrete spectrum on compact manifolds. The euclidean manifold $R^{4}$ is not a compact manifold. However, people typically writes
$$
\text{det}(iD) = \prod_{i = 1}^{\infty}\lambda_{i},
$$
where $\lambda_{i}$ defines the $i$th eigenvalue:
$$
iD\psi_{i} = \lambda_{i}\psi_{i}
$$
Why can they do this?