The 2:3:6 QPO structure in GRS 1915+105 and cubic subharmonics in the context of relativistic diskoseismology
Manuel Ortega-Rodr\'iguez, Hugo Sol\'is-S\'anchez, Vanessa, L\'opez-Barquero, Bryan Matamoros-Alvarado, Ariadna Venegas-Li

TL;DR
This paper introduces a simple model explaining the 2:3:6 QPO frequency structure in GRS 1915+105 and similar sources, based on diskoseismology and subharmonic resonances, predicting new observable QPOs.
Contribution
The paper presents a novel toy model linking QPO structures to resonances between g-modes and p-waves in accretion disks, advancing understanding of high-frequency QPOs.
Findings
Predicts a QPO at twice the higher twin frequency in twin peak sources.
Suggests the observed 2:3:6 structure results from diskoseismic resonances.
Indicates potential observation of a high-quality factor QPO in GRS 1915+105.
Abstract
We propose a simple toy model to explain the 2:3:6 QPO structure in GRS 1915+105 and, more generally, the 2:3 QPO structure in XTE J1550-564, GRO J1655-40, and H 1743-322. The model exploits the onset of subharmonics in the context of diskoseismology. We suggest that the observed frequencies may be the consequence of a resonance between a fundamental g-mode and an unobservable p-wave. The results include the prediction that, as better data become available, a QPO with a frequency of twice the higher twin frequency and a large quality factor will be observed in twin peak sources, as it might already have been observed in the especially active GRS 1915+105.
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