2022ApJ...927..233A


Query : 2022ApJ...927..233A

2022ApJ...927..233A - Astrophys. J., 927, 233-233 (2022/March-2)

Measuring the Nonaxially Symmetric Surface Temperature Distribution of the Central Compact Object in Puppis A.

ALFORD J.A.J., GOTTHELF E.V., PERNA R. and HALPERN J.P.

Abstract (from CDS):

The surface temperature distributions of central compact objects (CCOs) are powerful probes of their crustal magnetic field strengths and geometries. Here we model the surface temperature distribution of RX J0822-4300, the CCO in the Puppis A supernova remnant, using 471 ks of XMM-Newton data. We compute the energy-dependent pulse profiles in 16 energy bands, fully including the general relativistic effects of gravitational redshift and light bending, to accurately model the two heated surface regions of different temperatures and areas, in addition to constraining the viewing geometry. This results in precise measurements of the two temperatures: {{kT}}_warm=(1+z)×{0.222}_{-0.019}^{+0.018} keV and kThot = (1 + z) x 0.411 ± 0.011 keV. The two heated surface regions are likely located very close to the rotational poles, with the most probable position of the hotter component ≃ 6° from the rotational pole. For the first time, we are able to measure a deviation from a pure antipodal hot-spot geometry, with a longitudinal offset δ_γ=11○ / . {7}_{-2○ / .  5}^{+2○ / .  6}. The discovery of this asymmetry, along with the factor of ≃2 temperature difference between the two emitting regions, may indicate that RX J0822-4300 was born with a strong, tangled crustal magnetic field.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): X-ray sources - Neutron stars - Magnetic fields

Simbad objects: 6

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Number of rows : 6
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 PSR J0821-4300 Psr 08 21 58.2 -43 00 22           ~ 129 2
2 RX J0822.0-4300 X 08 22 26.84204 -43 10 26.2350           ~ 48 1
3 NAME Pup A SNR 08 24 07 -42 59.8           ~ 636 1
4 PSR J1210-5226 Psr 12 10 00.88 -52 26 28.4           ~ 230 1
5 SNR G033.6+00.1 SNR 18 52 29.000 +00 38 42.00           ~ 302 2
6 PSR J1852+0040 Psr 18 52 38.5963516169 +00 40 20.164383034           ~ 98 1

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