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Sample Datasets

Hezaveh uses 192×192192\times192 image size with a pixel size of 0.04" (seconds of arc). This seems to be a reasonable choice to follow.

Proposed Selection Algorithm

This is based on a sketch by Ben David March 2026.

  1. Choose the Einstein radius uniformly at random, so that 0.1"θE3.0"0.1"\le\theta_E\le3.0".

    • where θE=RE/χ\theta_E=R_E/\chi, i.e. RER_E converted to angular units.

  2. Choose the source position inside or around the critical curve, For example, choose the polar coordinates (R,ϕ)(R,\phi)

    • so that RcθER\le c\theta_E for some constant CC, e.g. c=1.2c=1.2.

    • ϕ\phi chosen uniformly at random

  3. Choose the orientation of the elliptical lens uniformly at random from a half-circle.

  4. Choose the orientation of the elliptical source uniformly at random from a half-circle.

  5. CHoose the ellipticity ff of the lens uniformly at random, so that 0.1f0.90.1\le f\le 0.9.

  6. Source parameters - sersic profile

    • size: 0.04"σ0.2"0.04"\le\sigma\le0.2"

    • sersic index 1ns51\le n_s\le 5

    • luminosity 10l2010\le l\le 20, exponentially distributed with λ=2.0\lambda=2.0 (see below)

Cluster lenses

  1. For cluster lenses, each constituent lens is placed in the same way as the source, relative to the origin, in polar co-ordinates (RL,ϕL)(R_L,\phi_L).

    • select random distance RL2θER_L\le2\theta_E, where θE\theta_E is the Einstein radius of the constituent lens

    • select random angle ϕL\phi_L

Proposal from Oda

ParameterHezaveh (arcsec)CosmoSim (512x512)
RER_E0.1"3.0"0.1"\ldots3.0"1391\ldots 39 (resiprocal)
Lens Ellipticity00.90\ldots0.91.00.11.0\ldots 0.1 (resiprocal)
Source Size0.05"0.8"0.05"\ldots0.8"1101\ldots10
Source Position (RR)not specified1101\ldots10
χ\chinot specified50
Lens rotation (θ\theta)not specified0°179°0°\ldots 179°
Source rotation (ϕ\phi)not specified0°359°0°\ldots 359°
Sersisk indeks (n_sersic)N/A151\ldots5
LuminosityN/A102010\ldots20[1]

The exponential distribution used for luminsoty returns u=1expλxu = 1 - \exp{-\lambda\cdot x} where xx is exponentially distributed, that is with a probability density function f(x;λ)=λexpλxf(x;\lambda) = \lambda\exp{-\lambda x} for positive xx.
This uu is scaled to within the given range.

Footnotes
  1. Luminosity is exponentially distributed with λ=2.0\lambda=2.0.