THE SPIN-DOWN OF PSR J0821-4300 AND PSR J1210-5226: CONFIRMATION OF CENTRAL COMPACT OBJECTS AS ANTI-MAGNETARS

被引:129
作者
Gotthelf, E. V. [1 ]
Halpern, J. P. [1 ]
Alford, J. [1 ]
机构
[1] Columbia Univ, Columbia Astrophys Lab, New York, NY 10027 USA
关键词
ISM: individual objects (Puppis A); pulsars: individual (PSR J0821-4300; PSR J1210-5226; PSR J1852+0040); stars: neutron; X-RAY PULSAR; ISOLATED NEUTRON-STAR; GALACTIC SUPERNOVA REMNANT; CYCLOTRON ABSORPTION FEATURE; XMM-NEWTON OBSERVATIONS; VLT OBSERVATIONS; TEMPERATURE DISTRIBUTION; SURFACE-TEMPERATURE; PROPER MOTION; RX J0822-4300;
D O I
10.1088/0004-637X/765/1/58
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Using XMM-Newton and Chandra, we measure period derivatives for the second and third known pulsars in the class of central compact objects (CCOs) in supernova remnants, proving that these young neutron stars have exceptionally weak dipole magnetic field components. For the 112 ms PSR J0821-4300 in Puppis A, (P) over dot = (9.28 +/- 0.36) x 10(-18). Its proper motion, mu = 61 +/- 9 mas yr(-1), was also measured using Chandra. This contributes a kinematic term to the period derivative via the Shklovskii effect, which is subtracted from (P) over dot to derive dipole B-s = 2.9 x 10(10) G, a value similar to that of the first measured CCO, PSR J1852 + 0040 in Kes 79, which has B-s = 3.1 x 10(10) G. Antipodal surface hot spots with different temperatures and areas are deduced from the X-ray spectrum and pulse profiles. Paradoxically, such nonuniform surface temperature appears to require strong crustal magnetic fields, probably toroidal or quadrupolar components much stronger than the external dipole. A spectral feature, consisting of either an emission line at approximate to 0.75 keV or an absorption line at approximate to 0.46 keV, is modulated in strength with the rotation. It may be due to a cyclotron process in a magnetic field on the surface that is slightly stronger than the dipole deduced from the spin-down. We also timed anew the 424 ms PSR J1210-5226, resolving previous ambiguities about its spin-down rate. Its (P) over dot is (2.22 +/- 0.02) x 10(-17), corresponding to B-s = 9.8 x 10(10) G. This is also compatible with a cyclotron resonance interpretation of its prominent absorption line at 0.7 keV and its harmonics. These results deepen the mystery of the origin and evolution of CCOs: Why are their numerous descendants not evident?
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