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Strong gravitational lensing's 'external shear' is not shear

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arxiv 2301.05244 v3 pith:5SB2OGPH submitted 2023-01-12 astro-ph.CO astro-ph.GA

classification astro-ph.COastro-ph.GA
keywords shearexternallensingmassmodelstrongbest-fitgalaxies
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The distribution of mass in galaxy-scale strong gravitational lenses is often modelled as an elliptical power law plus 'external shear', which notionally accounts for neighbouring galaxies and cosmic shear. We show that it does not. Except in a handful of rare systems, the best-fit values of external shear do not correlate with independent measurements of shear: from weak lensing in 45 Hubble Space Telescope images, or in 50 mock images of lenses with complex distributions of mass. Instead, the best-fit shear is aligned with the major or minor axis of 88% of lens galaxies; and the amplitude of the external shear increases if that galaxy is disky. We conclude that 'external shear' attached to a power law model is not physically meaningful, but a fudge to compensate for lack of model complexity. Since it biases other model parameters that are interpreted as physically meaningful in several science analyses (e.g. measuring galaxy evolution, dark matter physics or cosmological parameters), we recommend that future studies of galaxy-scale strong lensing should employ more flexible mass models.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Line-of-sight shear in SLACS strong lenses II: validation tests with an extended sample

    astro-ph.CO 2025-12 conditional novelty 4.0 of 10

    Line-of-sight shear in 45 SLACS lenses is often larger than N-body expectations (mean |γ_LOS| ≈ 0.085–0.11), and adding mass octupoles or checking image properties does not remove the excess.

  2. Weak Gravitational Lensing: A Brief Overview

    gr-qc 2026-04 unverdicted novelty 2.0 of 10

    The paper reviews standard derivations of light deflection in curved spacetime and presents a unified geometric approach for static and rotating gravitational fields.

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