Mass Profiles
This section covers the lens mass profiles implemented in GLEE.
General Remarksβ
Below are important notes regarding the profiles used in GLEE.
The strength of the profiles (e.g., : the Einstein radius) corresponds to the true deflection angles (), not the scaled deflection angles ().
- In single-plane lensing, the D_ds / D_s factors will be multiplied by the true deflection angles to obtain the scaled deflection angle for ray tracing via the lens equation.
- In multi-plane lensing, the redshift/distance factors are incorporated into the recursive multi-plane lens equation for ray tracing.
- If D_ds / D_s = 1 for a specific source (
sources/esourcesin the config file), then the Einstein radius in the lens profiles corresponds directly to the observed lensed image separation for the specific lens and source redshifts. - If D_ds / D_s is set to its actual value (e.g., 0.48, based on spectroscopic z_d and z_s measurements), then the Einstein radius in the
lenses_varysection of the config file represents the Einstein radius for a source at redshift infinity, rather than the specific lens-source redshift pair. - If D_ds / D_s β 1.0, the
"scale:"parameter intheta_ewill correspond to the Einstein radius of a lens profile for a source at redshift infinity, since normalizations are defined before multiplying the D_ds / D_s factor. - To avoid numerical singularities, some profiles include a softening radius (
r_soft).- The default value is 1e-4.
- Users can override this value in the GLEE config file using:
Rsoft xyz
Profile Summaryβ
| Profile | Keyword | Description |
|---|---|---|
| Elliptical Power Law (EPL) | epl | Standard smooth power-law lens |
| External Shear | shear | Tidal shear from the lens environment |
| PIEMD | piemd | Pseudo-Isothermal Elliptical β cored isothermal |
| Mass-Follows-Light PIEMD (PIEMDMFL) | piemdmfl | PIEMD with mass-to-light ratio coupling |
| Dual Pseudo-Isothermal Elliptical (dPIE) | dpie | Truncated PIEMD for satellite galaxies |
| SPEMD | spemd | Softened Power-law Elliptical β generalized PIEMD |
| NFW | nfw | Navarro-Frenk-White dark matter halo |
| Elliptical NFW (eNFW) | enfw | NFW with ellipticity in surface density |
| Generalized NFW (GNFW) | gnfw | NFW with variable inner slope |
| Triaxial NFW (TNFW) | tnfw | Fully triaxial dark matter halo |
| Prolate NFW (PNFW) | pnfw | Axisymmetric cigar-shaped NFW |
| Point Mass | point | Point mass for compact objects |
| Convergence Gradient (kgrad) | kgrad | Constant external convergence gradient |
Below is a list of all detailed profile documentation:
Elliptical Power Law (EPL)
Power-law elliptical mass distribution β the standard model for galaxy-scale lenses.
External Shear
External shear component β models the tidal influence of the lens environment.
PIEMD (Mass)
Pseudo-Isothermal Elliptical Mass Distribution β a cored isothermal sphere with ellipticity.
Mass-Follows-Light PIEMD (PIEMDMFL)
PIEMD with mass-to-light ratio parameter β couples stellar light to mass distribution.
SPEMD (Mass)
Softened Power-law Elliptical Mass Distribution β a generalisation of PIEMD with a variable slope.
Dual Pseudo-Isothermal Elliptical (dPIE)
Truncated PIEMD profile with core and truncation radii β ideal for modeling satellite galaxies.
NFW (Navarro-Frenk-White)
NFW profile β the standard dark matter halo profile from N-body simulations.
eNFW (Elliptical NFW)
Elliptical NavarroβFrenkβWhite profile β NFW with applied ellipticity in the surface mass density.
Point Mass
Point mass lens model β useful for stellar or compact object microlensing perturbations.
Generalized NFW (GNFW)
NFW profile with variable inner slope β more flexible dark matter halo modeling.
Triaxial NFW (TNFW)
Fully triaxial dark matter halo profile β most realistic 3D halo shape.
Prolate NFW (PNFW)
Axisymmetric cigar-shaped NFW halo β simplified triaxial profile.
Convergence Gradient (kgrad)
Constant external convergence gradient β models large-scale structure effects.