2014MNRAS.437.2957J


Query : 2014MNRAS.437.2957J

2014MNRAS.437.2957J - Mon. Not. R. Astron. Soc., 437, 2957-2965 (2014/January-3)

Phase-averaged gamma-ray spectra from rotation-powered millisecond pulsars.

JIANG Z.J., CHEN S.B., LI X. and ZHANG L.

Abstract (from CDS):

Fermi Large Area Telescope (LAT) has detected pulsed gamma-ray emissions with high confidences from more than 40 millisecond pulsars (MSPs). Here we study the phase-averaged gamma-ray properties of MSPs by using revised version of a self-consistent outer gap model. In this model, a strong multipole magnetic field near the stellar surface for an MSP is assumed and such a field will be close to the surface magnetic fields ( ∼ 1011-1012 G) of young pulsars; the outer gap of an MSP is controlled by photon-photon pair production process, where the effects of magnetic inclination angle (α) and magnetic geometry have been taken into account. Therefore, the fractional size of the outer gap is a function of not only pulsar's period and magnetic field strength but also magnetic inclination angle and radial distance to the neutron star; the inner boundary of the outer gap can be estimated by the pair production process of the gamma-ray photons which are produced by the back-flowing particles through the null charge surface; inside the outer gap, a Gaussian distribution of the parallel electric field along the trans-field thickness is assumed, and the gamma-ray emission is represented by the emission from the average radial distance along the central field lines of the outer gap. Using this model, the phase-averaged gamma-ray spectra are calculated and compared with the observed spectra of 37 MSPs given by the second Fermi-LAT catalogue of gamma-ray pulsars; our results show that the Fermi-LAT results can be well explained by this model. The thermal X-ray emission properties from MSPs are also investigated.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): radiation mechanisms: non-thermal - pulsars: general

CDS comments: PSR J1648-5324 is not identified (probable misprint).

Simbad objects: 41

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Number of rows : 41
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 PSR J0023+0923 Psr 00 23 16.890 +09 23 24.18           ~ 108 0
2 PSR J0030+0451 Psr 00 30 27.4277 +04 51 39.710           ~ 462 1
3 PSR J0034-05 Psr 00 34 21.8281 -05 34 36.620           ~ 182 0
4 PSR J0101-6422 Psr 01 01 11.1163 -64 22 30.171           ~ 53 0
5 PSR J0103+48 Psr 01 02 50.6687164 +48 39 42.769776           ~ 34 0
6 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 336 2
7 PSR J0340+41 Psr 03 40 23.2887 +41 30 45.300           ~ 75 0
8 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 906 0
9 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5261 0
10 PSR J0610-2100 Psr 06 10 13.5921 -21 00 28.016           ~ 89 0
11 PSR B0613-02.0 Psr 06 13 43.9759 -02 00 47.228           ~ 269 1
12 PSR J0614-3329 Psr 06 14 10.3479 -33 29 54.116           ~ 100 1
13 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 289 1
14 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 241 1
15 PSR J1124-36 Psr 11 24 01.1169434 -36 53 19.108887           ~ 49 0
16 PSR J1125-58 Psr 11 25 44.3654 -58 25 16.896           ~ 46 1
17 PSR J1231-1411 Psr 12 31 11.3069 -14 11 43.628           ~ 113 0
18 PSR J1446-4701 Psr 14 46 35.7143 -47 01 26.762           ~ 62 1
19 PSR J1514-4946 Psr 15 14 19.1142 -49 46 15.528           ~ 46 0
20 PSR J1600-3053 Psr 16 00 51.903339 -30 53 49.37555           ~ 173 0
21 PSR J1614-2230 Psr 16 14 36.5070 -22 30 31.207           ~ 393 1
22 PSR J1658-5324 Psr 16 58 39.0 -53 24 06           ~ 35 0
23 PSR J1713+0747 Psr 17 13 49.5331917 +07 47 37.492580           ~ 466 1
24 PSR J1741+1351 Psr 17 41 31.1499024 +13 51 44.279709           ~ 95 0
25 PSR J1744-1134 Psr 17 44 29.4172 -11 34 54.710           ~ 271 1
26 PSR J1747-4036 Psr 17 47 48.7133789 -40 36 54.775085           ~ 68 0
27 PSR J1810+17 Psr 18 10 37.2791131488 +17 44 37.425884136           ~ 114 0
28 PSR J1820-30A Psr 18 23 40.4842 -30 21 39.920           ~ 157 1
29 PSR J1858-2216 Psr 18 58 04.42 -22 19 13.7           ~ 30 0
30 PSR J1902-5105 Psr 19 02 02.8476 -51 05 56.969           ~ 47 0
31 PSR B1937+21 Psr 19 39 39.6 +21 37 22           ~ 1067 2
32 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 807 3
33 PSR J2017+0603 Psr 20 17 22.7048 +06 03 05.585           ~ 100 1
34 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 108 1
35 PSR J2047+1053 Psr 20 47 00.000 +10 53 00.00           ~ 36 0
36 V* LY Aqr Psr 20 51 07.5145 -08 27 37.795           ~ 206 2
37 PSR J2124-3358 Psr 21 24 43.8464 -33 58 44.961           ~ 299 1
38 PSR J2214+3000 Psr 22 14 38.8480 +30 00 38.209           ~ 109 0
39 PSR J2215+51 Psr 22 15 32.6869149432 +51 35 36.400854912           ~ 140 0
40 PSR J2241-5236 Psr 22 41 42.03161 -52 36 36.2492           ~ 110 1
41 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 105 0

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