Bibcode
Henze, M.; Darnley, M. J.; Williams, S. C.; Kato, M.; Hachisu, I.; Anupama, G. C.; Arai, A.; Boyd, D.; Burke, D.; Ciardullo, R.; Chinetti, K.; Cook, L. M.; Cook, M. J.; Erdman, P.; Gao, X.; Harris, B.; Hartmann, D. H.; Hornoch, K.; Horst, J. Chuck; Hounsell, R.; Husar, D.; Itagaki, K.; Kabashima, F.; Kafka, S.; Kaur, A.; Kiyota, S.; Kojiguchi, N.; Kučáková, H.; Kuramoto, K.; Maehara, H.; Mantero, A.; Masci, F. J.; Matsumoto, K.; Naito, H.; Ness, J.-U.; Nishiyama, K.; Oksanen, A.; Osborne, J. P.; Page, K. L.; Paunzen, E.; Pavana, M.; Pickard, R.; Prieto-Arranz, J.; Rodríguez-Gil, P.; Sala, G.; Sano, Y.; Shafter, A. W.; Sugiura, Y.; Tan, H.; Tordai, T.; Vraštil, J.; Wagner, R. M.; Watanabe, F.; Williams, B. F.; Bode, M. F.; Bruno, A.; Buchheim, B.; Crawford, T.; Goff, B.; Hernanz, M.; Igarashi, A. S.; José, J.; Motta, M.; O’Brien, T. J.; Oswalt, T.; Poyner, G.; Ribeiro, V. A. R. M.; Sabo, R.; Shara, M. M.; Shears, J.; Starkey, D.; Starrfield, S.; Woodward, C. E.
Bibliographical reference
The Astrophysical Journal, Volume 857, Issue 1, article id. 68, 29 pp. (2018).
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2018
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Citations
46
Refereed citations
26
Description
Since its discovery in 2008, the Andromeda galaxy nova M31N 2008-12a has
been observed in eruption every single year. This unprecedented
frequency indicates an extreme object, with a massive white dwarf and a
high accretion rate, which is the most promising candidate for the
single-degenerate progenitor of a Type Ia supernova known to date. The
previous three eruptions of M31N 2008-12a have displayed remarkably
homogeneous multiwavelength properties: (i) from a faint peak, the
optical light curve declined rapidly by two magnitudes in less than two
days, (ii) early spectra showed initial high velocities that slowed down
significantly within days and displayed clear He/N lines throughout, and
(iii) the supersoft X-ray source (SSS) phase of the nova began extremely
early, six days after eruption, and only lasted for about two weeks. In
contrast, the peculiar 2016 eruption was clearly different. Here we
report (i) the considerable delay in the 2016 eruption date, (ii) the
significantly shorter SSS phase, and (iii) the brighter optical peak
magnitude (with a hitherto unobserved cusp shape). Early theoretical
models suggest that these three different effects can be consistently
understood as caused by a lower quiescence mass accretion rate. The
corresponding higher ignition mass caused a brighter peak in the
free–free emission model. The less massive accretion disk
experienced greater disruption, consequently delaying the
re-establishment of effective accretion. Without the early refueling,
the SSS phase was shortened. Observing the next few eruptions will
determine whether the properties of the 2016 outburst make it a genuine
outlier in the evolution of M31N 2008-12a.
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