On the dependence of the X-ray continuum variations with luminosity in accreting X-ray pulsars

TL;DR

This study examines how the spectral hardness ratio in transient X-ray pulsars varies with X-ray luminosity, revealing a saturation or decrease at high luminosities and modeling the accretion column structure to explain these observations.

Contribution

It introduces a detailed model of accretion columns in X-ray pulsars to explain the observed dependence of spectral hardness on luminosity, including the effects of reflected emission.

Findings

Spectral hardness increases with luminosity at low levels.

Hardness saturates or decreases above a critical luminosity.

Reflected emission from the neutron star atmosphere influences spectral hardness.

Abstract

Using RXTE/ASM archival data, we investigate the behaviour of the spectral hardness ratio as a function of X-ray luminosity in a sample of six transient X-ray pulsars (EXO 2030+375, GX 304-1, 4U 0115+63, V 0332+63, A 0535+26 and MXB 0656-072). In all sources we find that the spectral hardness ratio defined as $F_{5-12\mathrm{keV}}/ F_{1.33-3\mathrm{keV}}$ increases with the ASM flux (1.33--12 keV) at low luminosities and then saturates or even slightly decreases above some critical X-ray luminosity falling into the range $\sim(3-7)\times10^{37}$~erg~s$^{-1}$. Two-dimensional structure of accretion columns in the radiation-diffusion limit is calculated for two possible geometries (filled and hollow cylinder) for mass accretion rates $\dot M$ ranging from $10^{17}$ to 1.2$\times 10^{18}$~g s$^{-1}$. The observed spectral behaviour in the transient X-ray pulsars with increasing $\dot M$ can be reproduced by a Compton saturated sidewall emission from optically thick magnetized accretion columns with taking into account the emission reflected from the neutron star atmosphere. At $\dot M$ above some critical value $\dot M_{cr}\sim (6-8)\times 10^{17}$~g~s$^{-1}$, the hight of the column becomes such that the contribution of the reflected component to the total emission starts decreasing, which leads to the saturation and even slight decrease of the spectral hardness. Hollow-cylinder columns have a smaller height than the filled-cylinder ones, and the contribution of the reflected component in the total emission does not virtually change with $\dot M$ (and hence the hardness of the continuum monotonically increases) up to higher mass accretion rates than $\dot M_{cr}$ for the filled columns.