Reconsidering the quantization of electrodynamics with boundary conditions and some measurable consequences

dc.creatorBordag, M.
dc.date2004-03-22
dc.date2004-05-28
dc.date.accessioned2026-07-07T11:10:15Z
dc.date.available2026-07-07T11:10:15Z
dc.descriptionWe show that the commonly known conductor boundary conditions $E_{||}=B_\perp=0$ can be realized in two ways which we call 'thick' and 'thin' conductor. The 'thick' conductor is the commonly known approach and includes a Neumann condition on the normal component $E_\perp$ of the electric field whereas for a 'thin' conductor $E_\perp$ remains without boundary condition. Both types describe different physics already on the classical level where a 'thin' conductor allows for an interaction between the normal components of currents on both sides. On quantum level different forces between a conductor and a single electron or a neutral atom result. For instance, the Casimir-Polder force for a 'thin' conductor is by about 13% smaller than for a 'thick' one.
dc.description22 pages, basic statement weakened, conclusions changed, misprints corrected
dc.identifierhttps://arxiv.org/abs/hep-th/0403222
dc.identifierhttp://arxiv.org/abs/hep-th/0403222
dc.identifierPhys.Rev.D70:085010,2004
dc.identifierdoi:10.1103/PhysRevD.70.085010
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/190730
dc.subjectHigh Energy Physics - Theory
dc.subjectQuantum Physics
dc.titleReconsidering the quantization of electrodynamics with boundary conditions and some measurable consequences
dc.typetext

Files

Collections