Cyclotron line formation in the radiative shock of an accreting magnetized neutron star

• Published in: arXiv.org
• Main Authors: Loudas, Nick, Kylafis, Nikolaos D, Trümper, Joachim E
• Format: Paper Journal Article
• Language: English
• Published: Ithaca Cornell University Library, arXiv.org 12.02.2024
• Subjects: Centroids; Deposition; Doppler effect; Elastic scattering; Field strength; Luminosity; Mathematical analysis; Neutron stars; Neutrons; Optical thickness; Photons; Physics - High Energy Astrophysical Phenomena; Radiation; X ray spectra
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.2402.07983

Magnetic neutron stars (NSs) often exhibit a cyclotron resonant scattering feature (CRSF) in their X-ray spectra, but the site of the CRSF formation is still an open puzzle. A promising candidate for high-luminosity sources has always been the radiative shock (RS) in the accretion column. Yet, no quantitative calculations of spectral formation at the RS have been performed so far. Here we explore the scenario where the shock is the site of the CRSF formation. We study spectral formation at the RS and the emergent spectral shape across a wide range of the parameter space. We developed a Monte Carlo code to conduct radiation transfer simulations at the RS, adopting a fully relativistic scheme for the interaction between radiation and electrons. We properly treated bulk-motion Comptonization in the pre-shock region, thermal Comptonization in the post-shock region, and resonant Compton scattering in both regions. We calculated the angle- and energy-dependent emergent X-ray spectrum from the RS, focusing on both the CRSF and the X-ray continuum, under diverse conditions. We find that a power law, hard X-ray continuum and a CRSF are naturally produced by the first-order Fermi energization as the photons criss-cross the shock. The CRSF shape depends mainly on the transverse optical depth and the post-shock temperature. We show that the CRSF energy centroid is shifted by ~(20-30)% to lower energies compared to the classical cyclotron energy, due to the Doppler boosting between the shock frame and the bulk-motion frame. We demonstrate that a "bump" feature arises in the right wing of the CRSF due to upscattering of photons by the accreting plasma and extends to higher energies for larger optical depths and post-shock temperatures. The implications of the Doppler effect on the centroid of the emergent CRSF must be considered if an accurate determination of the magnetic field strength is desired.