Technology of Cheesemaking 2010
DOI: 10.1002/9781444323740.ch12
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Cited by 22 publications
(23 citation statements)
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“…The action of a gravitational lens on the plane of polarization of electromagnetic radiation from a distant source has been found to be negligible to first order, according to the result by DS. We describe the gravitational lens with a Newtonian potential, as customary in the conventional gravitational lens theory (Bourassa et al 1973;Bourassa & Kantowski 1975;Schneider 1985;Blandford & Narayan 1986;Blandford & Kochanek 1988). This approach is alternative to that of DS, but it is obviously limited to situations in which the assumptions needed to apply the standard scalar or vector formalism (based on the use of a post-Newtonian metric) hold.…”
Section: Discussionmentioning
confidence: 99%
“…The action of a gravitational lens on the plane of polarization of electromagnetic radiation from a distant source has been found to be negligible to first order, according to the result by DS. We describe the gravitational lens with a Newtonian potential, as customary in the conventional gravitational lens theory (Bourassa et al 1973;Bourassa & Kantowski 1975;Schneider 1985;Blandford & Narayan 1986;Blandford & Kochanek 1988). This approach is alternative to that of DS, but it is obviously limited to situations in which the assumptions needed to apply the standard scalar or vector formalism (based on the use of a post-Newtonian metric) hold.…”
Section: Discussionmentioning
confidence: 99%
“…For brevity, we refer the reader to Suyu et al (2006Suyu et al ( , 2013 and Cappellari (2008), which cover in detail the theory and application of each to real observational data. Here, we confine ourselves to a description of the main formalisms, following the strong lensing and stellar dynamical framework developed and formulated in Schneider (1985); Schneider et al (1992); Blandford & Narayan (1986) and Binney & Tremaine (1987).…”
Section: Historical Contextmentioning
confidence: 99%
“…If the source itself is variable, these variations will appear at different times in different images. The time delay between image points θi and θj of the same source point β, is then given by ∆tij ≡ t(θi, β) − t(θj, β) where (Schneider 1985;Schneider et al 1992). Here, the pre-factor also includes the redshift z d of the gravitational lens.…”
Section: Gravitational Lensing Formalismmentioning
confidence: 99%