The 2001 Superoutburst of WZ Sagittae
Author(s) -
J. Patterson,
G. Masi,
M. Richmond,
Brian Martin,
E. C. Beshore,
David R. Skillman,
Jonathan Kemp,
Tonny Vanmunster,
Robert Rea,
William H. Allen,
Stacey M. Davis,
Tracy C. Davis,
A. A. Henden,
D. Starkey,
Jerry Foote,
A. Oksanen,
Lewis M. Cook,
Robert Fried,
D. Husar,
Р. Новак,
Tut Campbell,
J. W. Robertson,
Thomas Krajci,
Е. П. Павленко,
N. Mirabal,
P. G. Niarchos,
O. H. Brettman,
S. Walker
Publication year - 2002
Publication title -
publications of the astronomical society of the pacific
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.294
H-Index - 172
eISSN - 1538-3873
pISSN - 0004-6280
DOI - 10.1086/341696
Subject(s) - physics , astrophysics , dwarf nova , amplitude , brightness , astronomy , white dwarf , stars , optics
We report the results of a worldwide campaign to observe WZ Sagittae duringits 2001 superoutburst. After a 23-year slumber at V=15.5, the star rose within2 days to a peak brightness of 8.2, and showed a main eruption lasting 25 days.The return to quiescence was punctuated by 12 small eruptions, of ~1 magamplitude and 2 day recurrence time; these "echo outbursts" are of uncertainorigin, but somewhat resemble the normal outbursts of dwarf novae. After 52days, the star began a slow decline to quiescence. Periodic waves in the light curve closely followed the pattern seen in the1978 superoutburst: a strong orbital signal dominated the first 12 days,followed by a powerful /common superhump/ at 0.05721(5) d, 0.92(8)% longer thanP_orb. The latter endured for at least 90 days, although probably mutating intoa "late" superhump with a slightly longer mean period [0.05736(5) d]. Thesuperhump appeared to follow familiar rules for such phenomena in dwarf novae,with components given by linear combinations of two basic frequencies: theorbital frequency omega_o and an unseen low frequency Omega, believed torepresent the accretion disk's apsidal precession. Long time series reveal anintricate fine structure, with ~20 incommensurate frequencies. Essentially allcomponents occurred at a frequency n(omega_o)-m(Omega), with m=1, ..., n. Butduring its first week, the common superhump showed primary components at n(omega_o)-Omega, for n=1, 2, 3, 4, 5, 6, 7, 8, 9 (i.e., m=1 consistently); amonth later, the dominant power shifted to components with m=n-1. This mayarise from a shift in the disk's spiral-arm pattern, likely to be theunderlying cause of superhumps. The great majority of frequency components ... . (etc., abstract continues)
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