VACUUM ENERGY IN THE PRESENCE OF DIELECTRIC AND CONDUCTING SURFACES

The polarization of the electromagnetic vacuum is examined in the neighborhood of dielectric and conducting surfaces and the energy associated with this polarization is shown to depend on a cutoff related to the microstructure of the boundary. The appearance of the cutoff permits the vacuum energy t...

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Main Author: Candelas, P
Format: Journal article
Language:English
Published: 1982
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author Candelas, P
author_facet Candelas, P
author_sort Candelas, P
collection OXFORD
description The polarization of the electromagnetic vacuum is examined in the neighborhood of dielectric and conducting surfaces and the energy associated with this polarization is shown to depend on a cutoff related to the microstructure of the boundary. The appearance of the cutoff permits the vacuum energy to be expressed in terms of a surface tension and certain higher shape tensions. For the case of a dielectric boundary the surface tension reproduces the Schmitt-Lucas formula which accounts reasonably for the observed surface tensions of many materials. The curvature tension is also calculated and it seems the effect of this energy may well be accessible to experimental verification. For the case of perfectly conducting surfaces the first four shape tensions are calculated. It is shown that previous calculations of the vacuum energy due to perfectly conducting surfaces are in error and these errors are corrected. © 1982.
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spelling oxford-uuid:e1bd825a-5c8b-4ab9-ac64-6faf01b067f72022-03-27T09:56:25ZVACUUM ENERGY IN THE PRESENCE OF DIELECTRIC AND CONDUCTING SURFACESJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:e1bd825a-5c8b-4ab9-ac64-6faf01b067f7EnglishSymplectic Elements at Oxford1982Candelas, PThe polarization of the electromagnetic vacuum is examined in the neighborhood of dielectric and conducting surfaces and the energy associated with this polarization is shown to depend on a cutoff related to the microstructure of the boundary. The appearance of the cutoff permits the vacuum energy to be expressed in terms of a surface tension and certain higher shape tensions. For the case of a dielectric boundary the surface tension reproduces the Schmitt-Lucas formula which accounts reasonably for the observed surface tensions of many materials. The curvature tension is also calculated and it seems the effect of this energy may well be accessible to experimental verification. For the case of perfectly conducting surfaces the first four shape tensions are calculated. It is shown that previous calculations of the vacuum energy due to perfectly conducting surfaces are in error and these errors are corrected. © 1982.
spellingShingle Candelas, P
VACUUM ENERGY IN THE PRESENCE OF DIELECTRIC AND CONDUCTING SURFACES
title VACUUM ENERGY IN THE PRESENCE OF DIELECTRIC AND CONDUCTING SURFACES
title_full VACUUM ENERGY IN THE PRESENCE OF DIELECTRIC AND CONDUCTING SURFACES
title_fullStr VACUUM ENERGY IN THE PRESENCE OF DIELECTRIC AND CONDUCTING SURFACES
title_full_unstemmed VACUUM ENERGY IN THE PRESENCE OF DIELECTRIC AND CONDUCTING SURFACES
title_short VACUUM ENERGY IN THE PRESENCE OF DIELECTRIC AND CONDUCTING SURFACES
title_sort vacuum energy in the presence of dielectric and conducting surfaces
work_keys_str_mv AT candelasp vacuumenergyinthepresenceofdielectricandconductingsurfaces