There are several (in the end equivalent) methods for obtaining the vacuum energy density corresponding to the Casimir effect. Here, a detailed, pedagogical account is provided of the most elegant of them, namely the zeta-function regularization procedure. It is shown how it yields (in many instances)exact results, without ever having to resort to the usual issue of infinity cancellations. This extremely simple way of dealing—by analytic continuation—with the series of eigenmodes, can be made into a closed procedure owing to a recent theorem, which extends a previous result of Weldon on the commutation of the order of the summations of infinite series. The cases of a scalar field with Dirichlet, Neumann and periodic boundary conditions, and of an electromagnetic field between perfectly conducting plates—intimately related from a mathematical point of view—are investigated.
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