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Elliptical Power Law (EPL)

Usage

    epl
4.006098 #x-coord noprior: step:0.001
4.006098 #y-coord noprior: step:0.001
0.800000 #b/a flat:0.3,1 step:0.01
3.141590 #theta noprior: step:0.05
1.500000 #theta_e flat:0.75,2.5 step:0.01
2.400000 #gam exact: step:0.01

Surface Mass Density

The surface mass density κ(r)\kappa(r) is given by:

κ(r)=3γ2(bqR2+rsoft2)γ1\kappa(r) = \frac{3 - \gamma}{2} \left( \frac{b}{q \sqrt{R^2 + r_{\text{soft}}^2}} \right)^{\gamma - 1}

where:

  • R2=x2+y2q2R^2 = x^2 + \frac{y^2}{q^2}
  • rsoft=105r_{\text{soft}} = 10^{-5} (must set Rsoft 1e-5 in config)
  • γ=γ12\gamma = \frac{\gamma^\prime - 1}{2}
  • b=(21+q)1γ1qθEb = \left( \frac{2}{1 + q} \right)^{\frac{1}{\gamma - 1}} \cdot q \cdot \theta_E

Important Notes

  • This profile assumes a very small softening core (via rsoft=105r_{\text{soft}} = 10^{-5}), suitable for lensing-only analysis.
    It diverges at the centre, so not ideal for dynamical modelling.
  • For extended core usage (e.g. in dark matter halos for group/cluster lenses), use the SPEMD profile instead.
  • θE\theta_E should represent the observed ring radius from imaging — not a free scaling factor.

Slope Conversion

To convert between EPL and SPEMD slope conventions: γEPL=2γSPEMD+1\gamma^\prime_{\text{EPL}} = 2 \cdot \gamma_{\text{SPEMD}} + 1


Citation

@ARTICLE{2015A&A...580A..79T,
author = {{Tessore}, Nicolas and {Metcalf}, R. Benton},
title = "{The elliptical power law profile lens}",
journal = {\aap},
keywords = {gravitational lensing: strong, methods: analytical, Astrophysics - Cosmology and Nongalactic Astrophysics},
year = 2015,
month = aug,
volume = {580},
eid = {A79},
pages = {A79},
doi = {10.1051/0004-6361/201526773},
archivePrefix = {arXiv},
eprint = {1507.01819},
primaryClass = {astro-ph.CO},
adsurl = {https://ui.adsabs.harvard.edu/abs/2015A&A...580A..79T},
adsnote = {Provided by the SAO/NASA Astrophysics Data System}
}