The three types of high-mass X-ray pulsator

High mass X-ray pulsators are shown to be divisible into three distinct groups on the basis of their observational properties: 1) the Be star systems, 2) non-Be star systems with long pulse periods, (~102 — 103 s), and 3) non-Be star systems with short pulse periods (~100 — 101 s). Differences in mass transfer processes between the groups are invoked to account for the different properties. The separation of high mass pulsators into three clearly defined groups enables some of the properties of a pulsator to be predicted if only a few of its parameters are known. Because of this the optical counterparts of the X-ray sources H0850-42, OAO1653-40 and 1E1048.1-5937 are predicted to be either Be stars or, much less likely, low mass binaries. The orbital (Po) and spin (Ps) periods of the short period systems may be anti-correlated, a phenomenon which is also exhibited by the intermediate polar white dwarf binaries. For the long period systems there is no strong relationship between Po and Ps as there is for the Be star systems. It is shown that for the Be star systems this relationship cannot be accounted for by accretion from a stellar wind if there is equality between the Alfven and corotation radii of the neutron stars in these systems. However, accretion from a non-expanding atmosphere is not excluded. The lack of any correlation between Ps and Po for the supergiant systems is attributed to the low angular momentum of accreted matter. The Be star systems, however, probably accrete significant angular momentum which can result in an accretion disk.

[1]  John I. Castor,et al.  Radiation-driven winds in Of stars. , 1975 .

[2]  A. Treves,et al.  B-emission stars and X-ray sources , 1976, Nature.

[3]  S. Pravdo,et al.  The discovery of 38.22 second X-ray pulsations from the vicinity of OAO 1653-40 , 1979 .

[4]  G. Clark,et al.  A0535+26: Refined position measurement and new pulse period data , 1979 .

[5]  C. Page,et al.  Observation of an outburst from the X-ray pulsator 0115+63 , 1981 .

[6]  A. Parmar,et al.  A comparison of the X-ray properties of X Per and gamma Cas , 1982 .

[7]  G. Skinner,et al.  Discovery of 69 ms periodic X-ray pulsations in A0538 — 66 , 1982, Nature.

[8]  R. Poeckert Model Atmospheres of Be Stars , 1982 .

[9]  J. Thorstensen,et al.  Extreme variability in the Be-type, periodic recurrent X-ray transient A0538 – 66: a highly eccentric interacting binary , 1983 .

[10]  Walter H. G. Lewin,et al.  Accretion-driven stellar X-ray sources , 1983 .

[11]  N. White,et al.  The 41.5 day binary X-ray pulsar 4U 1223-62 (GX 301-2). , 1984 .

[12]  S. Ilovaisky Massive X-Ray Binary Systems: An Overview , 1984 .

[13]  A. King,et al.  Secular evolution of magnetic cataclysmic variables. , 1985 .

[14]  M. Coe,et al.  The first uv studies of the optical candidate for the X-ray source 1118-61 , 1985 .

[15]  L. Stella,et al.  The discovery of 4.4 second X-ray pulsations from the rapidly variable X-ray transient V0332 + 53 , 1985 .

[16]  B. Ramsey,et al.  On fast X-ray rotators with long-term periodicities , 1985 .

[17]  P. Charles,et al.  A 6 second periodic X-ray source in Carina , 1986 .