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PIEMDMFL (Mass-Follows-Light PIEMD)

:::info Migrated from Old Wiki This content was migrated from the old wiki using GitHub Copilot and should be double-checked for accuracy. :::

Overview​

The PIEMDMFL (Pseudo-Isothermal Elliptical Mass Distribution - Mass Follows Light) profile is almost identical to PIEMD, but specifically designed as a mass-follows-light (MFL) model for baryonic components.

PIEMDMFL has one additional parameter multfac to multiply the theta_e parameter. This is particularly useful when:

  • A PIEMD profile models the lens light (e.g., as part of a chameleon profile)
  • The chameleon profile (difference of 2 PIEMDs mimicking a SΓ©rsic profile) is used as the baryonic ΞΊ profile
  • The first six parameters of PIEMDMFL are identical to the PIEMD light profile
  • The 7th parameter multfac converts the light amplitude (theta_e) to ΞΊ amplitude

Mathematical Definition​

The convergence is given by:

ΞΊ(x,y)=E02w2+rem2\kappa(x,y) = \frac{E_0}{2\sqrt{w^2 + r_{\text{em}}^2}}

where:

rem2=x2(1+e)2+y2(1βˆ’e)2r_{\text{em}}^2 = \frac{x^2}{(1+e)^2} + \frac{y^2}{(1-e)^2}
  • E0E_0 = lens strength
  • ww = core radius
  • ee = ellipticity, e=1βˆ’q1+qe = \frac{1-q}{1+q} (inverting: q=1βˆ’e1+eq = \frac{1-e}{1+e})
  • qq = axis ratio (minor/major)

In the limiting case where w=e=0w = e = 0, E0E_0 is the Einstein radius of the SIS.

Parameter Calculation​

Without scale:​

E0=ΞΈEΓ—mfE_0 = \theta_E \times m_f

where ΞΈE\theta_E is the 5th parameter and mfm_f is the 7th parameter (multfac).

With scale:​

E0=ΞΈEΓ—mfE_0 = \theta_E \times m_f E0=E02E02+w2βˆ’wE_0 = \frac{E_0^2}{\sqrt{E_0^2 + w^2} - w}

:::warning Softening Radius If w<rsoftw < r_{\text{soft}}, then ww will be set to rsoftr_{\text{soft}} (default: rsoft=10βˆ’4r_{\text{soft}} = 10^{-4}) :::

Logarithmic Parameters​

The parameters E0E_0 and ww (5th and 6th parameters) support the log: option:

  • E0E_0 is computed first as E0=ΞΈEΓ—mfE_0 = \theta_E \times m_f
  • Then treated as a logarithmic value (base 10)

Combined log: and scale:​

When both options are used:

  1. First: E0=ΞΈEΓ—mfE_0 = \theta_E \times m_f is exponentiated (10E010^{E_0}) to account for log:
  2. Then: The scaling E0=E02E02+w2βˆ’wE_0 = \frac{E_0^2}{\sqrt{E_0^2 + w^2} - w} is applied for scale:

GLEE Configuration​

Basic Usage​

piemdmfl
0.000 #x-coord (x centroid)
0.000 #y-coord (y centroid)
0.800 #b/a (q, axis ratio related to e in kappa definition)
0.500 #theta (position angle, ccw from +x in radians; 0 = elongated along x)
2.600 #theta_e (Einstein radius or amplitude)
0.200 #r_core (w, core radius)
1.500 #multfac (mf, multiplication factor for theta_e)

Parameter Summary​

#ParameterDescriptionOptions
1xx-coordinate of centroid (arcsec)
2yy-coordinate of centroid (arcsec)
3qAxis ratio (b/a, minor/major)0<q≀10 < q \leq 1
4thetaPosition angle (radians, CCW from +x axis)
5theta_eEinstein radius / strengthlog:, scale:
6r_coreCore radius wwlog:
7multfacMultiplication factor for theta_e

Alternative Formulation​

To express the PIEMD ΞΊ distribution in terms of (x2+y2/q2)(x^2 + y^2/q^2) instead of remr_{\text{em}}, see the PIEMD profile description.

Use Cases​

Chameleon Profile Example:

  1. Model lens light with 2 PIEMD profiles (difference mimics SΓ©rsic)
  2. Use PIEMDMFL for baryonic mass:
    • Copy parameters 1–6 from the PIEMD light profile
    • Set multfac (parameter 7) as the mass-to-light ratio
    • This enforces mass-follows-light with a constant M/L ratio
  • PIEMD - Standard pseudo-isothermal elliptical mass distribution
  • SPEMD - Softened power-law elliptical mass distribution
  • dPIE - Dual pseudo-isothermal elliptical (truncated version)