BK Lyncis: the oldest old nova?... and a Bellwether for cataclysmic variable evolution
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Author
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Publication Date
2013 -
Publisher
Oxford University Press -
Citation
Patterson, J., Uthas, H., Kemp, J., Miguel Agustino, E., Krajci, T., Foote, J., Hambsch, F.J., Campbell, T., Roberts, G., Cejudo, D., Dvorak, S., Vanmunster, T., Koff, R., Skillman, D., Harvey, D., Martin, B., Rock, J., Boyd, D., Oksanen, A., Morelle, E., Ulowetz, J., Kroes, A., Sabo, R., Jensen, L.: "BK Lyncis: the oldest old nova?... and a Bellwether for cataclysmic variable evolution". Monthly Notices of the Royal Astronomical Society. Vol. 43, n. 3, págs. 1902-1919, (2013). ISSN 0035-8711 -
Abstract
We summarize the results of a 20-year campaign to study the light curves of BK Lyncis, a nova-like star strangely located below the 2-3 hour orbital period gap in the family of cataclysmic variables. Two apparent “superhumps” dominate the nightly light curves – with periods 4.6% longer, and 3.0% shorter, than Porb. The first appears to be associated with the star's brighter states (V~14), while the second appears to be present throughout and becomes very dominant in the low state (V~15.7). It's plausible that these arise, respectively, from a prograde apsidal precession and a retrograde nodal precession of the star's accretion disk. Starting in the year 2005, the star's light curve became indistinguishable from that of a dwarf nova – in particular, that of the ER UMa subclass. No such clear transition has ever been observed in a cataclysmic variable. Reviewing all the star's oddities, we speculate: (a) BK Lyn is the remnant of the probable nova on 30 December 101, and (b) it has been fading ever since, but has taken ~2000 years for the accretion rate to drop sufficiently to permit dwarf-nova eruptions. If such behavior is common, it can explain other puzzles of CV evolution. One: why the ER UMa class even exists (because all members can be remnants of recent novae). Two: why ER UMa stars and short-period novalikes are rare (because their lifetimes, which are essentially cooling times, are short). Three: why short-period novae all decline to luminosity states far above their true quiescence (because they're just getting started in their postnova cooling). Four: why the orbital periods, accretion rates, and whitedwarf temperatures of short-period CVs are somewhat too large to arise purely from the effects of gravitational radiation (because the unexpectedly long interval of enhanced postnova brightness boosts the mean mass-transfer rate). And maybe even five: why very old, post-period-bounce CVs are hard to find (because the higher mass-loss rates have “burned them out”). These are substantial rewards in return for one investment of hypothesis: that the second parameter in CV evolution, besides Porb, is time since the last classical-nova eruption.
Fichero | Tamaño | Formato |
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Bk Lyncis.pdf | 753.5Kb | View/ | versión pre-print |
Fichero | Tamaño | Formato |
| Description |
---|---|---|---|---|
Bk Lyncis.pdf | 753.5Kb | View/ | versión pre-print |