1988
DOI: 10.1086/166226
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Degeneracies in parameter estimates for models of gravitational lens systems

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Cited by 185 publications
(170 citation statements)
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“…a given distribution of observed images can be reproduced by many different mass distributions. The most recognized degeneracy is mass sheet degeneracy, MSD (Gorenstein et al 1988;Saha 2000). It rescales the mass surface density by s: κ(θ) → sκ(θ), and adds a constant thickness mass sheet of surface mass density (1 − s), in units of critical density Table 2 shows the widths of these distributions (also displayed in each panel), quantified by the Normalized Median Absolute Deviation (see Section 3).…”
Section: Why Models' Magnifications Differ: Lensing Degeneraciesmentioning
confidence: 99%
“…a given distribution of observed images can be reproduced by many different mass distributions. The most recognized degeneracy is mass sheet degeneracy, MSD (Gorenstein et al 1988;Saha 2000). It rescales the mass surface density by s: κ(θ) → sκ(θ), and adds a constant thickness mass sheet of surface mass density (1 − s), in units of critical density Table 2 shows the widths of these distributions (also displayed in each panel), quantified by the Normalized Median Absolute Deviation (see Section 3).…”
Section: Why Models' Magnifications Differ: Lensing Degeneraciesmentioning
confidence: 99%
“…For example, mass sheet degeneracy, and some other degeneracies where different lenses reproduce exactly the same image observables have been well studied (Falco et al 1985;Gorenstein et al 1988;Saha 2000;Liesenborgs & De Rijcke 2012), especially in relation to mass modeling, where degeneracies affect E-mail:…”
Section: Introductionmentioning
confidence: 99%
“…For a general magnitude of flexion (Goldberg & Leonard 2007;Okura et al 2008), F ∼ 0.03 arcsec −1 , and for a typical scale of background source size ∼ 2 arcsec, the variation of magnification over the image can be significant, |∆µ/µ| ∼ 10%. In weak lensing, the shape of images is unchanged if the surface mass density κ is transformed as κ → κ ′ = λκ + (1 − λ), which is known as the mass-sheet degeneracy (Gorenstein et al 1988). The real observable quantity in weak lensing is the reduced shear g = γ/(1 − κ).…”
Section: Basic Formalismmentioning
confidence: 99%