Does the accreting millisecond pulsar XTE J1814-338 precess?

被引:7
作者
Chung, C. T. Y. [1 ]
Galloway, D. K. [1 ,2 ]
Melatos, A. [1 ]
机构
[1] Univ Melbourne, Sch Phys, Parkville, Vic 3010, Australia
[2] Monash Univ, Sch Phys, Clayton, Vic 3800, Australia
关键词
gravitational waves; stars: neutron; pulsars: general; pulsars: individual: XTE J1814-338; stars: rotation; X-ray: binaries;
D O I
10.1111/j.1365-2966.2008.13882.x
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Precession in an accretion-powered pulsar is expected to produce characteristic variations in the pulse properties. Assuming surface intensity maps with one and two hotspots, we compute theoretically the periodic modulation of the mean flux, pulse-phase residuals and fractional amplitudes of the first and second harmonic of the pulse profiles. These quantities are characterized in terms of their relative precession phase offsets. We then search for these signatures in 37 d of X-ray timing data from the accreting millisecond pulsar XTE J1814-338. We analyse a 12.2-dmodulation observed previously and show that it is consistent with a freely precessing neutron star only if the inclination angle is < 0 degrees.1, an a priori unlikely orientation. We conclude that if the observed flux variations are due to precession, our model incompletely describes the relative precession phase offsets (e.g. the surface intensity map is oversimplified). We are still able to place an upper limit on epsilon of 3.0 x 10(-9) independently of our model, and estimate the phase-independent tilt angle theta to lie roughly between 5 degrees and 10 degrees. On the other hand, if the observed flux variations are not due to precession, the detected signal serves as a firm upper limit for any underlying precession signal. We then place an upper limit on the product epsilon cos theta of <= 9.9 x 10(-10). The first scenario translates into a maximum gravitational wave strain of 10(-27) from XTE J1814-338 (assuming a distance of 8 kpc), and a corresponding signalto-noise ratio of <= 10(-3) (for a 120 d integration time) for the advanced Laser Interferometer Gravitational-Wave Observatory ground-based gravitational wave detector.
引用
收藏
页码:254 / 267
页数:14
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