Skip to main content

The NASA/GSFC network is currently experiencing intermittent issues that affect our services. We are working on it and apologize for the inconvenience.
The offline tool hark (also on github) can be used to find and download data from the cloud.

Xspec Home Page


bkn2pow: broken power law, 2 break energies

A three-segment broken power law (i.e. with two break energies).

$\displaystyle A(E) = \left\{ \begin{array}{ll}
K E^{-\Gamma_1} & \mbox{if $E \...
.../1 keV)^{-\Gamma_3} &
\mbox{if $E_{break,2} \leq E$} \\
\end{array} \right.
$

where:

par1 = $\Gamma_1$ power law photon index for $E \leq E_{break,1}$
par2 = $E_{break,1}$ first break point for the energy in keV
par3 = $\Gamma_2$ power law photon index for $E_{break,1} \leq E \leq E_{break,2}$
par4 = $E_{break,2}$ second break point for the energy in keV
par5 = $\Gamma_3$ power law photon index for $E > E_{break,2}$
norm = K photons/keV/cm$^2$/s at 1 keV

If POW_EMIN and POW_EMAX have been defined by the xset command then the norm becomes the flux in units of $10^{-12}$ ergs/cm$^2$/s over the energy range (POW_EMIN, POW_EMAX) keV unless POW_EMIN = POW_EMAX in which case the norm becomes the flux density in micro-Jansky at POW_EMIN keV. In these cases it is important that POW_EMIN and POW_EMAX lie within the energy range on which the model is being evaluated.