We suggest that high-mass black holes; i.e., black holes of several solar masses, can be formed in binaries with low-mass main-sequence companions, provided that the hydrogen envelope of the massive star is removed in common envelope evolution which begins only after the massive star has finished He
Lense-thirring precession and QPOs in low mass x-ray binaries
β Scribed by Luigi Stella; Mario Vietri
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 475 KB
- Volume
- 69
- Category
- Article
- ISSN
- 0920-5632
No coin nor oath required. For personal study only.
β¦ Synopsis
The relativistic dragging of inertial frames around fast rotating collapsed stars is substantial and can give rise to observable effects. We apply this to the kHz quasi periodic oscillations (QPOs) sources, low mass X-ray binaries (LMXRBs) containing an accreting neutron star. Within the beat frequency model, both the Keplerian frequency of the innermost region of the accretion disk (,-~ 0.3 -1.2 kHz) and the neutron star spin frequency (~ 0.3 -0.4 kHz) arc directly observed. From these the Lense-Thirring precession frequency (tens of Hz) of the same material in the innermost disk regions which gives rise to the kIIz QPOs is determined within a factor of 4, depending on the neutron star equation of state. The classical contribution from neutron star oblateness decreases the precession frequency slightly. The broad peaks at frequencies ~, 20 -40 Hz in the power spectra of the "Atoll'-sources 4U 1728-34, 4U 0614+091 and KS 1731-260 and their variations with the higher kHz QPO frequency are well matched by Lense-Thirring precession of material in the innermost disk region. We also suggest that the ~ 15 -60 Hz horizontal branch QPOs of GX 5-1 and GX 17+2 (and likewise other "Z"-type low mass X-ray binaries) arise from the same mechanism.
π SIMILAR VOLUMES
## Abstract Our aim is to investigate tidal interaction in HighβMass Xβray Binary stars in order to determine in which objects the rotation of the mass donors is synchronized or pseudosynchronized with the orbital motion of the compact companion. We calculate the pseudosynchronization period (__P__