2008
DOI: 10.1111/j.1365-2966.2008.13604.x
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Analytic relations for magnifications and time delays in gravitational lenses with fold and cusp configurations

Abstract: Gravitational lensing provides a unique and powerful probe of the mass distributions of distant galaxies. Four‐image lens systems with fold and cusp configurations have two or three bright images near a critical point. Within the framework of singularity theory, we derive analytic relations that are satisfied for a light source that lies a small but finite distance from the astroid caustic of a four‐image lens. Using a perturbative expansion of the image positions, we show that the time delay between the close… Show more

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Cited by 20 publications
(27 citation statements)
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“…More particularly, four-image lenses in cusp configurations (where the source is close to the cusp of the astroid caustic) and fold configurations (resulting from the source being close to the caustic fold) give clear theoretical expectations for image flux ratios which must be obeyed by any smooth model. In cusp lenses, there are three close images and the middle image is expected to have the brightness of the sum of the outer two (Schneider & Weiss 1992); in fold lenses, the two close images are expected to have the same flux (Keeton, Gaudi & Petters 2003;Congdon, Keeton & Nordgren 2008). Because of optical microlensing, radio lens systems have traditionally been used for this work (Mao & Schneider 1998, Fassnacht et al 1999, Metcalf & Zhao 2002, Metcalf 2005, Kratzer et al 2011.…”
Section: Introductionmentioning
confidence: 99%
“…More particularly, four-image lenses in cusp configurations (where the source is close to the cusp of the astroid caustic) and fold configurations (resulting from the source being close to the caustic fold) give clear theoretical expectations for image flux ratios which must be obeyed by any smooth model. In cusp lenses, there are three close images and the middle image is expected to have the brightness of the sum of the outer two (Schneider & Weiss 1992); in fold lenses, the two close images are expected to have the same flux (Keeton, Gaudi & Petters 2003;Congdon, Keeton & Nordgren 2008). Because of optical microlensing, radio lens systems have traditionally been used for this work (Mao & Schneider 1998, Fassnacht et al 1999, Metcalf & Zhao 2002, Metcalf 2005, Kratzer et al 2011.…”
Section: Introductionmentioning
confidence: 99%
“…Secondly, time‐variable sources allow us to measure time delays between multiple images; these time delays contain rich information on the lens potentials as well as cosmology (e.g. Witt, Mao & Keeton 2000; Kochanek 2002; Saha & Williams 2003; Schechter 2005; Oguri 2007a; Congdon, Keeton & Nordgren 2008; Keeton & Moustakas 2009; Congdon, Keeton & Nordgren 2010; Keeton 2010).…”
Section: Introductionmentioning
confidence: 99%
“…In this regard, gravitational lenses with two or three close images deserve special attention because, in these cases, the sources must be close to either a fold or a cusp of the caustic. It is well known for any smooth lensing potential that the close images follow asymptotic flux ratio relations: for a close pair, their flux ratio approaches unity when their separation goes to zero, while for a close triple, the ratio of the flux of the middle image to the sum of the fluxes of the two outer images asymptotically goes to unity (Mao 1992; Schneider & Weiss 1992; Keeton, Gaudi & Petters 2003; Congdon, Keeton & Nordgren 2008). However, the observed lensing systems often violate these asymptotic relations.…”
Section: Introductionmentioning
confidence: 99%