2020ApJ...892...38W


Query : 2020ApJ...892...38W

2020ApJ...892...38W - Astrophys. J., 892, 38-38 (2020/March-3)

Spot model for identifications of periods in asynchronous polars.

WANG Q., QIAN S., HAN Z., FANG X., ZANG L. and LIU W.

Abstract (from CDS):

We improved the discless accretion models in Wynn & King considering the effects of the changing aspect due to the white dwarf (WD) spin and the variable feeding intensity caused by the asynchronism, and set up a more general spot model that is not sensitive to the different forms of these effects and can be applied for the period analysis of the optical and X-ray light curve. The spot model can produce the power spectra compatible with the observations, and its simulations limit the ratio Pspin/Porb < 2 between the powers at the WD spin and the binary orbital frequencies, which is a strong criterion for identification of periods. Then we recognize the periods for CD Ind, BY Cam, and 1RXS J083842.1-282723. The spot model reveals a complex accretion geometry in the asynchronous polars (APs), which may indicate that the complex magnetic field causes their asynchronism. We think 1RXS J083842.1-282723 is a prepolar because of its highest asynchronism and stable light curve. Giving the unstable accretion process in APs, the period analysis of the long-term light curve will make the orbital signal prominent.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): AM Herculis stars - X-ray binary stars - X-ray photometry - CCD photometry

Simbad objects: 5

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Number of rows : 5
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* BY Cam CV* 05 42 48.8013535344 +60 51 31.376128608   16.60       ~ 270 0
2 RX J0838.7-2827 CV* 08 38 43.3520551272 -28 27 01.143230076           ~ 23 0
3 V* V1432 Aql CV* 19 40 11.4199326288 -10 25 25.771706256     14.40 15.437   ~ 181 0
4 V* V1500 Cyg No* 21 11 36.5809818696 +48 09 01.952490204           ~ 820 0
5 V* CD Ind CV* 21 15 41.0450813472 -58 40 54.058462428           ~ 108 0

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