dc.contributor.author |
Isogai K. |
|
dc.contributor.author |
Kato T. |
|
dc.contributor.author |
Ohshima T. |
|
dc.contributor.author |
Kasai K. |
|
dc.contributor.author |
Oksanen A. |
|
dc.contributor.author |
Masumoto K. |
|
dc.contributor.author |
Fukushima D. |
|
dc.contributor.author |
Maeda K. |
|
dc.contributor.author |
Kawabata M. |
|
dc.contributor.author |
Matsuda R. |
|
dc.contributor.author |
Kojiguchi N. |
|
dc.contributor.author |
Sugiura Y. |
|
dc.contributor.author |
Takeda N. |
|
dc.contributor.author |
Matsumoto K. |
|
dc.contributor.author |
Itoh H. |
|
dc.contributor.author |
Pavlenko E. |
|
dc.contributor.author |
Antonyuk K. |
|
dc.contributor.author |
Antonyuk O. |
|
dc.contributor.author |
Pit N. |
|
dc.contributor.author |
Sosnovskij A. |
|
dc.contributor.author |
Baklanov A. |
|
dc.contributor.author |
Babina J. |
|
dc.contributor.author |
Sklyanov A. |
|
dc.contributor.author |
Kiyota S. |
|
dc.contributor.author |
Hambsch F. |
|
dc.contributor.author |
Littlefield C. |
|
dc.contributor.author |
Maeda Y. |
|
dc.contributor.author |
Cook L. |
|
dc.contributor.author |
Masi G. |
|
dc.contributor.author |
Dubovsky P. |
|
dc.contributor.author |
Novák R. |
|
dc.contributor.author |
Dvorak S. |
|
dc.contributor.author |
Imada A. |
|
dc.contributor.author |
Nogami D. |
|
dc.date.accessioned |
2018-09-19T20:04:29Z |
|
dc.date.available |
2018-09-19T20:04:29Z |
|
dc.date.issued |
2016 |
|
dc.identifier.issn |
0004-6264 |
|
dc.identifier.uri |
https://dspace.kpfu.ru/xmlui/handle/net/142517 |
|
dc.description.abstract |
© The Author 2016.We report on two superoutbursts of the AMCVn-type object CR Boo in 2014 April-March and 2015 May-June. A precursor outburst accompanied both of these superoutbursts. During the rising branch of the main superoutburst in 2014, we detected growing superhumps (stage A superhumps) whose period was 0.017669(24) d. Assuming that this period reflects the dynamical precession rate at the radius of the 3:1 resonance, we could estimate the mass ratio (q = M2/M1) of 0.101(4) by using the stage A superhump period and the orbital period of 0.0170290(6) d. This mass ratio is consistent with that expected from the theoretical evolutionary model of AMCVn-type objects. The detection of precursor outbursts and stage A superhumps is the second case in AMCVn-type objects. There are two interpretations of the outbursts of AMCVn-type objects. One is a dwarf nova (DN) outbursts analogy, which suggets that the outbursts are caused by thermal and tidal instabilities. Another is the VY Scl-type variation, which suggests that the outbursts are caused by the variation of the mass-transfer rate of the secondary. This detection of the superhump variations strongly supports the former interpretation. |
|
dc.relation.ispartofseries |
Publications of the Astronomical Society of Japan |
|
dc.subject |
Accretion |
|
dc.subject |
Accretion disks-novae |
|
dc.subject |
Cataclysmic variables-stars |
|
dc.subject |
Dwarf novae-stars |
|
dc.subject |
Individual (CR Bootis) |
|
dc.title |
Superoutburst of CR Bootis: Estimation of mass ratio of a typical AMCVn star by stage A superhumps |
|
dc.type |
Article |
|
dc.relation.ispartofseries-issue |
4 |
|
dc.relation.ispartofseries-volume |
68 |
|
dc.collection |
Публикации сотрудников КФУ |
|
dc.source.id |
SCOPUS00046264-2016-68-4-SID84988981226 |
|