2023MNRAS.526.1287C


Query : 2023MNRAS.526.1287C

2023MNRAS.526.1287C - Mon. Not. R. Astron. Soc., 526, 1287-1297 (2023/November-3)

The common fundamental plane of X-ray emissions from pulsars and magnetars in quiescence.

CHU C.-Y. and CHANG H.-K.

Abstract (from CDS):

Magnetars are a unique class of neutron stars characterized by their incredibly strong magnetic fields. Unlike normal pulsars whose X-ray emission was driven by rotational energy loss, magnetars exhibit distinct X-ray emissions thought to be driven by their strong magnetic fields. Here, we present the results of magnetar X-ray spectra analysis in their quiescent state. In the sample studied in this paper, spectra of 17 magnetars can be fitted well with a model consisting of a power-law and a blackbody component. We found that the luminosity of the power-law component can be described by a function of blackbody temperature and emission-region radius. The same relation was seen in pulsars whose X-ray emission mechanism is thought to be different. The fact that these magnetars and pulsars share a common fundamental plane in the space spanned by non-thermal X-ray luminosity, surface temperature, and the radius of the thermally emitting region presents both challenges and hints to theoretical models for a complete comprehension of the magnetospheric emissions from these two classes of neutron stars.

Abstract Copyright: © The Author(s) 2023. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): stars: magnetars - pulsars: general - X-rays: stars

Simbad objects: 33

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Number of rows : 33
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 J0100-7211 Psr 01 00 42.86 -72 11 33.3   17.69 17.82     B3V 101 0
2 PSR J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
3 NAME Per Arm PoG 03 30 +45.0           ~ 1672 0
4 NAME Sgr J0418+5729 gam 04 18 33.867 +57 32 22.91           ~ 244 0
5 PSR J0501+4516 Psr 05 01 06.600 +45 16 33.96           ~ 142 0
6 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
7 SNR J052559-660453 SNR 05 26 00.4 -66 05 02     12.71     ~ 456 2
8 PSR B0525-66 Psr 05 26 00.7 -66 04 35           ~ 569 1
9 2E 2336 HXB 10 50 08.93 -59 53 19.9           Be 419 0
10 PSR J1119-6127 Psr 11 19 14.30 -61 27 49.5           ~ 439 1
11 PSR J1550-5418 Psr 15 50 54.18 -54 18 23.9           ~ 463 1
12 NAME SGR J1555.2-5402 X 15 55 08.556 -54 03 38.74           ~ 35 0
13 PSR J1622-4950 Psr 16 22 44.80000 -49 50 54.5000           ~ 169 0
14 GRB 980618A gB 16 35 52 -47 35.2           ~ 270 0
15 PSR J1647-4552 Psr 16 47 10.18 -45 52 16.7           ~ 217 1
16 PSR J1708-4008 Psr 17 08 46.1 -40 08 56           ~ 315 0
17 [AAB2008] 1 X 17 14 05.7 -38 10 31           ~ 69 1
18 PSR J1745-2900 Psr 17 45 40.1640 -29 00 29.818           ~ 358 0
19 PSR J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1316 2
20 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 532 0
21 SWIFT J1818.0-1607 N* 18 18 00.23 -16 07 53.0           ~ 109 0
22 1WGA J1822.2-1604 X 18 22 18.32 -16 04 27.2           ~ 141 0
23 GRB 201010A X 18 30 41.66 -06 45 17.2           ~ 47 0
24 NAME Sgr 1833-0832 gam 18 33 46.0 -08 32 13           ~ 87 0
25 PSR J1834-0845 Psr 18 34 52.1 -08 45 56           ~ 98 0
26 SNR G027.3+00.0 SNR 18 41 17.8 -04 56 12           ~ 345 3
27 PSR J1841-0456 Psr 18 41 19.29 -04 56 11.4           ~ 296 1
28 SNR G029.7-00.3 SNR 18 46 22.8 -02 59 47           ~ 375 2
29 PSR J1846-0258 Psr 18 46 24.75 -02 58 29.6           ~ 388 2
30 PSR J1852+0033 Psr 18 52 46.60 +00 33 20.9           ~ 51 0
31 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 906 0
32 NAME Sgr 1935+2154 * 19 34 55.68 +21 53 48.2           ~ 820 1
33 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 673 1

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