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PNFW (Prolate NFW)

:::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 PNFW (Prolate Navarro-Frenk-White) profile is a special case of the TNFW (Triaxial NFW) profile, specifically for prolate (cigar-shaped) halos where a=b≤ca = b \leq c.

Due to the axial symmetry of prolate halos, the viewing angle Ļ•\phi (which matters for fully triaxial halos) becomes irrelevant. All projected prolate halos have PA = 90° when measured from the observer's x-axis. Instead of Ļ•\phi, PNFW directly specifies the observed position angle PA.

Mathematical Definition​

See TNFW for full mathematical details. The key difference:

Triaxial case (TNFW): a≤b≤ca \leq b \leq c (three independent axes)
Prolate case (PNFW): a=b≤ca = b \leq c (axisymmetric around long axis)

Simplifications for Prolate Halos​

  1. Axial symmetry: Rotation about the long axis (c-axis) doesn't change the halo
  2. Viewing angle Ļ•\phi → PA: Since Ļ•\phi is degenerate, replace it with the directly observable position angle
  3. Fixed PA behavior: All projections have PA = 90° in the natural frame

Projected Convergence​

The convergence formula is identical to TNFW, but with simplified geometry due to a=ba = b:

Īŗ(x′,y′)=bPNFW2ā‹…fGNFW(ζ)\kappa(x', y') = \frac{b_{\text{PNFW}}}{2} \cdot f_{\text{GNFW}}(\zeta)

where ζ\zeta depends on (a/c,Īø,PA)(a/c, \theta, \text{PA}) instead of the full set (a/c,b/c,Īø,Ļ•)(a/c, b/c, \theta, \phi).

Softening Radius​

Like TNFW, a softening radius avoids singularities:

R2→R2+rsoft2R^2 \rightarrow R^2 + r_{\text{soft}}^2

Default: rsoft=10āˆ’4r_{\text{soft}} = 10^{-4} (adjustable via Rsoft keyword).

GLEE Configuration​

Basic Usage​

pnfw
4.000000 #x-coord exact:
4.000000 #y-coord exact:
0.600000 #a/c exact:
0.750000 #theta exact:
1.570796 #PA exact:
10.000000 #theta_e exact:
25.000000 #r_scale exact:
0.740028 #q exact:

Parameter Summary​

#ParameterDescriptionInput/OutputNotes
1xx-coordinate of centroid (arcsec)Input
2yy-coordinate of centroid (arcsec)Input
3a/cShort-to-long axis ratio (= b/c for prolate)Input0<a/c≤10 < a/c \leq 1
4thetaViewing angle (radians)InputAngle from line-of-sight
5PAPosition angle (radians, CCW from +x axis)InputReplaces Ļ•\phi from TNFW
6theta_eEinstein radius rEr_E (arcsec)InputFor equivalent sphere
7r_scaleScale radius R0R_0 (arcsec)Input
8qOutput axis ratio of projected ĪŗOutputCan impose prior

:::tip Output Parameter Parameter 8 (qq) is an output computed from the 3D→2D projection. It is included in the parameter list to allow imposing priors based on observed 2D light distributions (e.g., from photometry). :::

Key Differences from TNFW​

FeatureTNFWPNFW
ShapeTriaxial (a≤b≤ca \leq b \leq c)Prolate (a=b≤ca = b \leq c)
Axis ratios2 independent (a/c, b/c)1 independent (a/c)
Viewing angles2 angles (Īø,Ļ•\theta, \phi)1 angle (Īø\theta) + PA
Position angleComputed outputDirect input parameter
Parameters10 total8 total (simpler)

Use Cases​

Observationally Motivated Models:

  • Prolate halos are common in simulations for isolated elliptical galaxies
  • Measure PA directly from 2D imaging (e.g., HST)
  • Impose prior on output qq based on observed light axis ratio

Simplified Modeling:

  • When full triaxiality is not required (e.g., visual inspection suggests prolate geometry)
  • Reduces parameter space by 2 compared to TNFW
  • Faster MCMC convergence due to fewer parameters

Physical Interpretation​

Input Parameters (3D Halo)​

  • a/c: How "cigar-like" the halo is (smaller = more elongated)
  • theta: Inclination angle (0 = edge-on, 90° = face-on)
  • PA: Orientation of long axis on the sky

Output Parameter (2D Projection)​

  • q: Observed axis ratio depends on both a/c and theta
    • Face-on (Īøā‰ˆ90°\theta \approx 90°): qā‰ˆ1q \approx 1 (circular)
    • Edge-on (Īøā‰ˆ0°\theta \approx 0°): qā‰ˆa/cq \approx a/c (most elongated)
  • TNFW - General triaxial NFW (includes PNFW as special case)
  • NFW - Standard spherical NFW
  • GNFW - Generalized NFW with variable inner slope
  • eNFW - Elliptical NFW with ellipticity in Īŗ

References​

  • Oguri, M., Lee, J., & Suto, Y. (2003). Detailed Cluster Lensing Profiles at Large Radii and the Impact on Cluster Weak Lensing Studies. ApJ, 599, 7. ADS Link