1997
DOI: 10.1086/304150
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The Nature of the Fluctuations Preceding the Giant Bursts in the Bursting Pulsar GRO J1744−28

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Cited by 12 publications
(11 citation statements)
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“…In this case, the radiation pressure is comparable to the gas pressure around the inner disk radius (i.e., the magnetospheric radius), resulting in a viscous instability with slightly increased mass accretion (e.g., Cannizzo 1996Cannizzo , 1997. Because the instability develops near the inner edge of the accretion disk, it has an advantage in explaining bursts/flares with a short recurrence time.…”
Section: Discussionmentioning
confidence: 99%
“…In this case, the radiation pressure is comparable to the gas pressure around the inner disk radius (i.e., the magnetospheric radius), resulting in a viscous instability with slightly increased mass accretion (e.g., Cannizzo 1996Cannizzo , 1997. Because the instability develops near the inner edge of the accretion disk, it has an advantage in explaining bursts/flares with a short recurrence time.…”
Section: Discussionmentioning
confidence: 99%
“…Interestingly, the variability at low Fourier frequencies (below ∼ 10 Hz) in GRO J1744−28 is suppressed at high mass accretion rates and the suppression starts as soon as type-II bursts start to appear in the light curve of the source. Note that numerical simulations of accretion instability of RPD part of a disk (Cannizzo 1997) show an appearance of QPOs, which finally end up in a type-II burst. Typical time scale of the oscillations is t osc ∼ 10 − 20 s. We suggest that these oscillations suppress the fluctuations of the mass accretion rate at frequencies below 1/t osc originating from the outer parts of the accretion disk.…”
Section: Transfer Functionmentioning
confidence: 96%
“…At the same time, it has been shown that the aperiodic variability by itself can principally stabilize RPD accretion flow(Suková & Janiuk 2016). See alsoCannizzo (1996Cannizzo ( , 1997 discussing the bursts of GRO J1744−28.…”
mentioning
confidence: 98%
“…Cannizzo (1996) showed that these oscillations eventually lead to a Lightman-Eardley instability (Lightman, Eardley, 1974), which Cannizzo (1996) considered to be the cause of Type II bursts. Cannizzo (1997) further showed that the characteristic QPO frequency can be reproduced by a selection of parameters. Abramowicz et al (1995) suggested that low-frequency QPOs in some XBs (including those of the Rapid Burster) and black-hole candidates can be produced via dissipation of energy in the coronal region above the accretion disk.…”
Section: Comparison With Qpos In Xbsmentioning
confidence: 94%