Abstract

The Casimir-Lifshitz force ${F}_{(C\ensuremath{-}L)}$ between planar objects when one of them is stratified at the nanoscale is herein investigated. Layering results in optical interference effects that give rise to a modification of the optical losses, which, as stated by the fluctuation-dissipation theorem, should affect the Casimir-Lifshitz interaction. On these grounds, we demonstrate that, by nanostructuring the same volume of dielectric materials in diverse multilayer configurations, it is possible to access ${F}_{(C\ensuremath{-}L)}$ of attractive or repulsive nature, even getting canceled, at specific separation distances.

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