2014
DOI: 10.1093/mnras/stu488
|View full text |Cite
|
Sign up to set email alerts
|

The 2:3:6 quasi-periodic oscillation structure in GRS 1915+105 and cubic subharmonics in the context of relativistic discoseismology

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 freque… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2

Citation Types

1
3
0

Year Published

2015
2015
2020
2020

Publication Types

Select...
5
1

Relationship

0
6

Authors

Journals

citations
Cited by 7 publications
(4 citation statements)
references
References 34 publications
1
3
0
Order By: Relevance
“…The simulations described in Paper I demonstrate that in a hydrodynamic approximation, the saturation of r-mode growth can lead to the excitation of higher-frequency, vertically unstructured inertial-acoustic waves (sometimes called p-modes, but here referred to as f-modes to differentiate them from purely acoustic oscillations). The presence of such a secondary coupling supports the idea that the non-linear interaction of multiple discoseismic oscillations might be responsible for the appearance of multiple HFQPOs in some sources (e.g., Ortega-Rodríguez et al 2014). The simulations in Paper I additionally suggest that r-modes can redistribute angular momentum locally, reshaping their own trapping regions and blurring their own frequencies over time.…”
Section: Introductionsupporting
confidence: 64%
“…The simulations described in Paper I demonstrate that in a hydrodynamic approximation, the saturation of r-mode growth can lead to the excitation of higher-frequency, vertically unstructured inertial-acoustic waves (sometimes called p-modes, but here referred to as f-modes to differentiate them from purely acoustic oscillations). The presence of such a secondary coupling supports the idea that the non-linear interaction of multiple discoseismic oscillations might be responsible for the appearance of multiple HFQPOs in some sources (e.g., Ortega-Rodríguez et al 2014). The simulations in Paper I additionally suggest that r-modes can redistribute angular momentum locally, reshaping their own trapping regions and blurring their own frequencies over time.…”
Section: Introductionsupporting
confidence: 64%
“…As suggested by Ferreira (2010), this might indicate that separate but correlated mechanisms, one of which could be r-mode excitation, are responsible for each oscillation. Alternatively, simulations or a dynamical systems approach might reveal a non-linear interaction between differ-ent diskoseismic modes that could give rise to oscillations with frequencies in near-integer ratios, as was preliminarily investigated with a toy model by Ortega-Rodríguez et al (2014).…”
Section: Discussionmentioning
confidence: 99%
“…The MHR equations thus introduce correlations in the output over time scales longer than the one of fluctuations and originate a red noise PDS. The idea of considering a non-linear ODE for describing some properties of accretion disc oscillations was already adopted by other authors: for instance, Ortega-Rodríguez et al (2014) considered the harmonic oscillator equation including quadratic and cubic terms and a sinusoidal forcing for describing the spectral structure of the normal mode oscillations in a thin accretion discs.…”
Section: Summary and Discussionmentioning
confidence: 99%