2008
DOI: 10.1051/0004-6361:200810155
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Modeling of non-stationary accretion disks in X-ray novae A 0620–00 and GRS 1124–68 during outburst

Abstract: Aims. We address the task of modeling soft X-ray and optical light curves of X-ray novae in the high/soft state. Methods. The analytic model of viscous evolution of an externally truncated accretion α-disk is used. Relativistic effects near a Kerr black hole and self-irradiation of an accretion disk are taken into account. Results. The model is applied to the outbursts of X-ray nova Monocerotis 1975 (A 0620−00) and X-ray nova Muscae 1991 (GRS 1124−68). Comparison of observational data with the model yields con… Show more

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Cited by 36 publications
(38 citation statements)
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References 74 publications
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“…Another possibility is to make use of a combination of optical and Xray light-curves of these systems. Here, constraints on C irr can be derived by computing the fraction of X-ray emission needed to be reprocessed to explain the observed optical luminosity (e.g., see Suleimanov et al 2008;Lipunova & Malanchev 2017). A third possibility involves using the correlation between X-ray and optical variability often observed in LMXBs to understand physical properties of the different components (i.e.…”
Section: Discussionmentioning
confidence: 99%
“…Another possibility is to make use of a combination of optical and Xray light-curves of these systems. Here, constraints on C irr can be derived by computing the fraction of X-ray emission needed to be reprocessed to explain the observed optical luminosity (e.g., see Suleimanov et al 2008;Lipunova & Malanchev 2017). A third possibility involves using the correlation between X-ray and optical variability often observed in LMXBs to understand physical properties of the different components (i.e.…”
Section: Discussionmentioning
confidence: 99%
“…However, semi-analytical and numerical simulations (see, for example, Masada & Sano 2008;Stone 2011;Hawley et al 2013;Suzuki & Inutsuka 2014;Nauman & Blackman 2015) suggest that the total (Reynolds + Maxwell) stresses due to MRI are insufficient to cause the effective angular momentum transfer in accretion discs in terms of the phenomenological alpha-parameter α S S (Shakura & Sunyaev 1973), giving rather low values α S S ∼ 0.01 − 0.03. Note that from the observational point of view, the alpha-parameter can be reliably evaluated, e.g., from the analysis of non-stationary accretion discs in X-ray novae (Suleimanov, Lipunova & Shakura 2008), dwarf-nova and AM CVn stars (Kotko & Lasota 2012), and turns out to be an order of magnitude higher than typically found in the numerical MRI simulations.…”
Section: Introductionmentioning
confidence: 97%
“…The size of the hot part of the disk depends on the radial temperature distribution, meanwhile the disk temperature depends on the viscous heating rate and the incident flux of central X-rays. Previously, Suleimanov et al (2008) have analysed X-ray and optical lightcurves of A 0620-00 (1975) and GS 1124GS -68 (1991, which have The left panels show the disk-to-total-flux ratio in 0.5 − 50 keV and reduced χ 2 . Empty circles denote the spectral fits made with the fixed distance ≈ 8.62 kpc, which has been found as the average for the observations at moments when the distance is least variable (before MJD 52456).…”
Section: Introductionmentioning
confidence: 99%