Hermiticity of the Dirac Hamiltonian in Curved Spacetime

dc.creatorHuang, Xing
dc.creatorParker, Leonard
dc.date2008-11-14
dc.date.accessioned2026-07-07T13:07:38Z
dc.date.available2026-07-07T13:07:38Z
dc.descriptionIn previous work on the quantum mechanics of an atom freely falling in a general curved background spacetime, the metric was taken to be sufficiently slowly varying on time scales relevant to atomic transitions that time derivatives of the metric in the vicinity of the atom could be neglected. However, when the time-dependence of the metric cannot be neglected, it was shown that the Hamiltonian used there was not Hermitian with respect to the conserved scalar product. This Hamiltonian was obtained directly from the Dirac equation in curved spacetime. This raises the paradox of how it is possible for this Hamiltonian to be non-hermitian. Here, we show that this non-hermiticity results from a time dependence of the position eigenstates that enter into the Schrodinger wave function, and we write the expression for the Hamiltonian that is Hermitian for a general metric when the time-dependence of the metric is not neglected.
dc.description5 pages, no figure
dc.identifierhttps://arxiv.org/abs/0811.2296
dc.identifierhttp://arxiv.org/abs/0811.2296
dc.identifierPhys.Rev.D79:024020,2009
dc.identifierdoi:10.1103/PhysRevD.79.024020
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/228154
dc.subjectHigh Energy Physics - Theory
dc.titleHermiticity of the Dirac Hamiltonian in Curved Spacetime
dc.typetext

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