1/3 factor in the CMB Sachs-Wolfe effect

dc.contributor.authorHwang, J.
dc.contributor.authorPadmanabhan, T.
dc.contributor.authorLahav, O.
dc.contributor.authorNoh, H.
dc.date.accessioned2012-02-29T10:27:27Z
dc.date.available2012-02-29T10:27:27Z
dc.date.issued1992-01-23
dc.description.abstractWe point out that a pseudo Newtonian interpretation of the 1/3 factor in the Sachs-Wolfe effect, which relates the fluctuations in temperature and potential, dT/T5(1/3)dF, is not supported by the general relativ-istic analysis. Dividing the full gravitational effect into separate parts depends on the choice of time slicing ~gauge! and there exist infinitely many different choices. More importantly, interpreting the parts as being due to the gravitational redshift and the time dilation is not justified in the rigorous relativistic perturbation theory. We suggest regarding the 1/3 factor as a general relativistic result that applies in a restricted situation of adiabatic perturbation in the K505L model with the last scattering occurring in the matter dominated era. For an isocurvature initial condition the corresponding result dT/T52dF has a different numerical coefficient.en_US
dc.identifier.urihttp://hdl.handle.net/11007/4
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.relation.ispartofseries;Physical Review D;65, 043005, 2002
dc.subjectCMBen_US
dc.subjectGeneral relativityen_US
dc.subjectSachs-Wolfe effecten_US
dc.title1/3 factor in the CMB Sachs-Wolfe effecten_US
dc.typeArticleen_US

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