2007
DOI: 10.1016/j.physletb.2006.12.052
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Electromagnetic Casimir densities induced by a conducting cylindrical shell in the cosmic string spacetime

Abstract: We investigate the renormalized vacuum expectation values of the field square and the energy-momentum tensor for the electromagnetic field inside and outside of a conducting cylindrical shell in the cosmic string spacetime. By using the generalized Abel-Plana formula, the vacuum expectation values are presented in the form of the sum of boundary-free and boundary-induced parts. The asymptotic behavior of the vacuum expectation values of the field square, energy density and stresses are investigated in various … Show more

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Cited by 82 publications
(56 citation statements)
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“…This is the well-known Casimir effects. The analysis of Casimir effects in the idealized cosmic string space-time have been developed for a scalar [33], vector [34] and fermionic fields [35], obeying boundary conditions on the cylindrical surfaces. 2 Additionally to the contribution for the energy-momentum tensor associated with charged quantum fields, the presence of a magnetic flux along the cosmic string induces vacuum current densities, as well.…”
Section: Introductionmentioning
confidence: 99%
“…This is the well-known Casimir effects. The analysis of Casimir effects in the idealized cosmic string space-time have been developed for a scalar [33], vector [34] and fermionic fields [35], obeying boundary conditions on the cylindrical surfaces. 2 Additionally to the contribution for the energy-momentum tensor associated with charged quantum fields, the presence of a magnetic flux along the cosmic string induces vacuum current densities, as well.…”
Section: Introductionmentioning
confidence: 99%
“…The corresponding Casimir densities for the electromagnetic field with perfect conductor boundary conditions on bounding surfaces are considered in [30]. The closely related problem with a cylindrical shell in the geometry of a cosmic string is discussed in [31,32] for scalar and electromagnetic fields. In both scalar and electromagnetic cases the application of a variant of the generalized Abel-Plana formula [24] enables to extract from the vacuum expectation values the parts corresponding to the geometry of a wedge without the cylindrical shell and to present the shell induced parts in terms of rapidly converging integrals.…”
Section: Introductionmentioning
confidence: 99%
“…The case D = 3 has been considered previously in [40]. The electromagnetic field is conformally invariant in D = 3 and the modes (2.4) and (2.5) coincide with the Minkowskian modes having the time dependence e −iωη .…”
Section: Cylindrical Electromagnetic Modesmentioning
confidence: 95%