Modelling annual and orbital variations in the scintillation of the relativistic binary PSR J1141-6545

被引:41
|
作者
Reardon, D. J. [1 ,2 ,3 ]
Coles, W. A. [4 ]
Hobbs, G. [3 ]
Ord, S. [3 ]
Kerr, M. [5 ]
Bailes, M. [1 ]
Bhat, N. D. R. [6 ]
Krishnan, V. Venkatraman [1 ,7 ]
机构
[1] Swinburne Univ Technol, Ctr Astrophys & Supercomp, POB 218, Hawthorn, Vic 3122, Australia
[2] Monash Univ, Sch Phys & Astron, Monash Ctr Astrophys MoCA, Clayton, Vic 3800, Australia
[3] CSIRO Astron & Space Sci, Australia Telescope Natl Facil, POB 76, Epping, NSW 1710, Australia
[4] Univ Calif San Diego, Elect & Comp Engn, La Jolla, CA 92093 USA
[5] Naval Res Lab, Space Sci Div, Washington, DC 20375 USA
[6] Curtin Univ, Int Ctr Radio Astron Res, Bentley, WA 6102, Australia
[7] Max Planck Inst Radioastron, Hugel 69, D-53121 Bonn, Germany
关键词
astrometry; scattering; pulsars: general; pulsars: individual (PSR J1141-6545); ISM: general; ISM: structure; INTERSTELLAR SCINTILLATION; PULSARS J1141-6545; PARABOLIC ARCS; SCATTERING; VELOCITY; PLASMA; TESTS;
D O I
10.1093/mnras/stz643
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We have observed the relativistic binary pulsar PSR J1141-6545 over a period of similar to 6 yr using the Parkes 64mradio telescope, with a focus on modelling the diffractive intensity scintillations to improve the accuracy of the astrometric timing model. The long-term scintillation, which shows orbital and annual variations, allows us to measure parameters that are difficult to measure with pulsar timing alone. These include: the orbital inclination i, the longitude of the ascending node Omega, and the pulsar system transverse velocity. We use the annual variations to resolve the previous ambiguity in the sense of the inclination angle. Using the correct sense, and a prior probability distribution given by a constraint from pulsar timing (i = 73 +/- 3.), we find Omega = 24.8 +/- 1.8 degrees and we estimate the pulsar distance to be D = 10(-3)(+4) kpc. This then gives us an estimate of this pulsar's proper motion of mu(alpha)cos delta = 2.9 +/- 1.0 mas yr(-1) in right ascension and mu(delta) = 1.8 +/- 0.6 mas yr(-1) in declination. Finally, we obtain measurements of the spatial structure of the interstellar electron-density fluctuations, including: the spatial scale and anisotropy of the diffraction pattern, the distribution of scattering material along the line of sight, and spatial variation in the strength of turbulence from epoch to epoch. We find that the scattering is dominated by a thin screen at a distance of (0.724 +/- 0.008) D, with an anisotropy axial ratio A(r) = 2.14 +/- 0.11.
引用
收藏
页码:4389 / 4403
页数:15
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