The Dirichlet Casimir Problem

dc.creatorGraham, N.
dc.creatorJaffe, R. L.
dc.creatorKhemani, V.
dc.creatorQuandt, M.
dc.creatorSchroeder, O.
dc.creatorWeigel, H.
dc.date2003-09-12
dc.date.accessioned2026-07-07T11:10:13Z
dc.date.available2026-07-07T11:10:13Z
dc.descriptionCasimir forces are conventionally computed by analyzing the effects of boundary conditions on a fluctuating quantum field. Although this analysis provides a clean and calculationally tractable idealization, it does not always accurately capture the characteristics of real materials, which cannot constrain the modes of the fluctuating field at all energies. We study the vacuum polarization energy of renormalizable, continuum quantum field theory in the presence of a background field, designed to impose a Dirichlet boundary condition in a particular limit. We show that in two and three space dimensions, as a background field becomes concentrated on the surface on which the Dirichlet boundary condition would eventually hold, the Casimir energy diverges. This result implies that the energy depends in detail on the properties of the material, which are not captured by the idealized boundary conditions. This divergence does not affect the force between rigid bodies, but it does invalidate calculations of Casimir stresses based on idealized boundary conditions.
dc.description29 pages, 4 figures
dc.identifierhttps://arxiv.org/abs/hep-th/0309130
dc.identifierhttp://arxiv.org/abs/hep-th/0309130
dc.identifierNucl.Phys.B677:379-404,2004
dc.identifierdoi:10.1016/j.nuclphysb.2003.11.001
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/190720
dc.subjectHigh Energy Physics - Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectQuantum Physics
dc.titleThe Dirichlet Casimir Problem
dc.typetext

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