2013ApJ...765...58G


Query : 2013ApJ...765...58G

2013ApJ...765...58G - Astrophys. J., 765, 58 (2013/March-1)

The spin-down of PSR J0821-4300 and PSR J1210-5226: confirmation of central compact objects as anti-magnetars.

GOTTHELF E.V., HALPERN J.P. and ALFORD J.

Abstract (from CDS):

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, {dot}P = (9.28 ± 0.36) x 10–18. Its proper motion, µ = 61±9 mas/yr, was also measured using Chandra. This contributes a kinematic term to the period derivative via the Shklovskii effect, which is subtracted from {dot}P to derive dipole Bs= 2.9 x1010 G, a value similar to that of the first measured CCO, PSR J1852+0040 in Kes 79, which has Bs= 3.1x1010 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 ~0.75 keV or an absorption line at ~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 {dot}P is (2.22±0.02)x10–17, corresponding to Bs= 9.8x1010 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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Journal keyword(s): ISM: individual: Puppis A - pulsars: individual (PSR J0821-4300, PSR J1210-5226, PSR J1852+0040) - stars: neutron

Simbad objects: 29

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Number of rows : 29
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 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
2 UCAC2 13302738 * 08 21 46.2952324080 -43 02 03.632131320   14.881 13.937 13.582   ~ 4 0
3 PSR J0821-4300 Psr 08 21 58.2 -43 00 22           ~ 129 2
4 NAME Pup A SNR 08 24 07 -42 59.8           ~ 636 1
5 NAME Vela Jr SN SNR 08 52.0 -46 20           ~ 507 2
6 2XMM J085201.4-461753 X 08 52 01.4 -46 17 53           ~ 52 1
7 NGC 3372 HII 10 45 02.23 -59 41 59.8           ~ 1071 2
8 CXOGNC J104608.71-594306.4 N* 10 46 08.719 -59 43 06.48           ~ 23 0
9 SNR G296.8-00.3 SNR 11 58 30 -62 35.0           ~ 64 0
10 2XMMi J115836.1-623516 X 11 58 36.1 -62 35 16           ~ 1 1
11 SNR G295.5+09.7 SNR 12 09 40 -52 25.0           ~ 301 1
12 PSR J1210-5226 Psr 12 10 00.88 -52 26 28.4           ~ 230 1
13 NAME Calvera N* 14 12 56.126 +79 22 03.54           ~ 47 0
14 CXOU J160103.1-513353 X 16 01 03.14 -51 33 53.6           ~ 20 1
15 SNR G330.2+01.0 SNR 16 01.1 -51 34           ~ 93 1
16 SNR G347.3-00.5 SNR 17 12 27 -39 41.2     12.27     ~ 761 1
17 RX J1713.4-3949 X 17 13 28 -39 49.8           ~ 44 0
18 XMMU J172054.5-372652 * 17 20 54.5 -37 26 52           ~ 21 0
19 SNR G350.1-00.3 SNR 17 21 06 -37 26.9     13.60     ~ 84 0
20 SNR G353.6-00.7 SNR 17 31 55.0 -34 42 36           ~ 172 0
21 XMMU J173203.3-344518 X 17 32 03.3 -34 45 18           ~ 40 0
22 CXOU J181852.0-150213 X 18 18 52.0 -15 02 13           ~ 20 0
23 SNR G015.9+00.2 SNR 18 18 52 -15 02.0           ~ 105 0
24 SNR G033.6+00.1 SNR 18 52 29.000 +00 38 42.00           ~ 302 2
25 PSR J1852+0040 Psr 18 52 38.5963516169 +00 40 20.164383034           ~ 98 1
26 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
27 SNR G039.7-02.0 SNR 19 12 20 +04 55.0           ~ 378 1
28 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1
29 CXOU J232327.8+584842 X 23 23 27.85 +58 48 42.8           ~ 42 1

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