Spin Wandering of an Accreting Neutron Star near Torque Balance: Implications for Gravitational-wave Searches

Abstract Torque balance between gravitational radiation reaction and magnetocentrifugal accretion is one reason why accreting neutron stars rotate slower than centrifugal breakup. Random processes in the accretion disk, such as Rayleigh–Taylor instabilities and flicker noise, drive the spin frequency f * and gravitational wave frequency f gw ∝ f * to wander stochastically around their torque balance values. Here it is shown theoretically, in terms of an idealized Ornstein–Uhlenbeck model, that the standard deviation of f gw is given by σ f gw ( h 0 ) ∝ f gw h 0 D β T 1 / 2 , or equivalently σ f gw ( F X ) ∝ f gw 1 / 2 F X 1 / 2 D β T 1 / 2 , where h 0 is the characteristic wave strain, F X is the X-ray flux, D is the source distance, and β and T are the fractional amplitude and autocorrelation timescale of the stochastic torque. One can use σ f gw ( h 0 ) and σ f gw ( F X

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Publication Details

Journal
The Astrophysical Journal
Published
2026-11-11
DOI
https://doi.org/10.3847/1538-4357/aeacd6
Primary Topic
Pulsars and Gravitational Waves Research
Type
article
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article

Spin Wandering of an Accreting Neutron Star near Torque Balance: Implications for Gravitational-wave Searches

Andrew Melatos
1 links
The Astrophysical Journal
Pulsars and Gravitational Waves Research
article

Spin Wandering of an Accreting Neutron Star near Torque Balance: Implications for Gravitational-wave Searches

Andrew Melatos
article en

Abstract

Abstract Torque balance between gravitational radiation reaction and magnetocentrifugal accretion is one reason why accreting neutron stars rotate slower than centrifugal breakup. Random processes in the accretion disk, such as Rayleigh–Taylor instabilities and flicker noise, drive the spin frequency f * and gravitational wave frequency f gw ∝ f * to wander stochastically around their torque balance values. Here it is shown theoretically, in terms of an idealized Ornstein–Uhlenbeck model, that the standard deviation of f gw is given by σ f gw ( h 0 ) ∝ f gw h 0 D β T 1 / 2 , or equivalently σ f gw ( F X ) ∝ f gw 1 / 2 F X 1 / 2 D β T 1 / 2 , where h 0 is the characteristic wave strain, F X is the X-ray flux, D is the source distance, and β and T are the fractional amplitude and autocorrelation timescale of the stochastic torque. One can use σ f gw ( h 0 ) and σ f gw ( F X

The Astrophysical JournalVol. 1012(1)
Australian Research Council (AU), ARC Centre of Excellence for Gravitational Wave Discovery (AU)
Pulsars and Gravitational Waves Research
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