{ "id": "2004.13435", "version": "v1", "published": "2020-04-28T11:35:19.000Z", "updated": "2020-04-28T11:35:19.000Z", "title": "Galaxy mass profiles from strong lensing II: The elliptical power-law model", "authors": [ "Conor M. O'Riordan", "Stephen J. Warren", "Daniel J. Mortlock" ], "comment": "11 pages, 8 figures. To be submitted to MNRAS", "categories": [ "astro-ph.GA" ], "abstract": "We present a systematic analysis of the constraints $\\sigma_\\gamma$ on the mass profile slope $\\gamma$ obtainable when fitting a singular power-law ellipsoid model to a typical strong lensing observation of an extended source. These results extend our previous analysis of circular systems, Paper I. We draw our results from 676 mock observations covering a range of image configurations, each created with a fixed signal to noise ratio $S=100$ in the images. We analyse the results using a combination of theory and a simplified modelling technique which identifies the contribution to the constraints of the individual fluxes and positions in each of the two or four images. The main results are: 1. Regardless of the lens ellipticity, the constraints $\\sigma_\\gamma$ for two image systems are well described by the results of Paper I, transformed to elliptical coordinates; 2. We derive an analytical expression for $\\sigma_\\gamma$ for systems with the source aligned with the axis of the lens; 3. For both two-image systems and aligned systems the slope uncertainties $\\sigma_\\gamma$ are limited by the flux uncertainties; 4. The constraints for off-axis four-image systems are a factor of two to eight better, depending on source size, than for two-image systems, and improve with increasing lens ellipticity. We show that the constraints on $\\gamma$ in these systems derive from the complementary positional information of the images and the flux measurements do not contribute to $\\sigma_\\gamma$. The complementarity improves as the offset of the source from the axis increases, such that the best constraints $\\sigma_\\gamma<0.01$, for $S=100$, occur when the source approaches the caustic.", "revisions": [ { "version": "v1", "updated": "2020-04-28T11:35:19.000Z" } ], "analyses": { "keywords": [ "galaxy mass profiles", "elliptical power-law model", "strong lensing", "constraints", "lens ellipticity" ], "note": { "typesetting": "TeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable" } } }