2013ApJ...769..119X


Query : 2013ApJ...769..119X

2013ApJ...769..119X - Astrophys. J., 769, 119 (2013/June-1)

Search for gamma-ray emission from four accreting millisecond pulsars with Fermi/LAT.

XING Y. and WANG Z.

Abstract (from CDS):

We report our search for γ-ray emission in the energy range from 100 MeV to 300 GeV from four accreting millisecond pulsars (AMPs), SAX J1808.4-3658, IGR J00291+5934, XTE J1814-338, and XTE J0929-314. The data are from four-year observations carried out by the Large Area Telescope on board the Fermi Gamma-Ray Space Telescope. The AMPs were not detected, and the γ-ray luminosity upper limits we obtain are 5.1x1033 erg/s for SAX J1808.4-3658, 2.1 x1033 erg/s for IGR J00291+5934, 1.2x1034 erg/s for XTE J1814-338, and 2.2x1033 erg/s for XTE J0929-314. We compare our results with γ-ray irradiation luminosities required for producing optical modulations seen from the companions in the AMPs, which has been suggested by Takata et al., and our upper limits have excluded γ-ray emission as the heating source in these systems except XTE J0929-314, the upper limit of which is not deep enough. Our results also do not support the model proposed by Takata et al. that relatively strong γ-ray emission could arise from the outer gap of a high-mass neutron star controlled by the photon-photon pair creation for the AMPs. Two AMPs, SAX J1808.4-3658 and IGR J00291+5934, have measurements of their spin-down rates, and we derive the upper limits of their γ-ray conversion efficiencies, which are 57% and 3%, respectively. We discuss the implications to the AMP systems by comparing the efficiency upper limit values with that of 20 γ-ray millisecond pulsars (MSP) detected by Fermi and the newly discovered transitional MSP binary J1023+0038.

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Journal keyword(s): binaries: close - gamma rays: stars - pulsars: general - stars: neutron

Simbad objects: 25

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Number of rows : 25
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 V* V1037 Cas LXB 00 29 03.06 +59 34 19.0           ~ 283 1
2 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
3 PSR J0034-05 Psr 00 34 21.8281 -05 34 36.620           ~ 201 0
4 PSR J0101-6422 Psr 01 01 11.1163 -64 22 30.171           ~ 63 0
5 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
6 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
7 PSR J0610-2100 Psr 06 10 13.602953 -21 00 27.74435           ~ 116 0
8 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
9 PSR J0614-3329 Psr 06 14 10.3479 -33 29 54.116           ~ 134 1
10 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
11 V* BW Ant LXB 09 29 20.19 -31 23 03.2   18.50 18.63     ~ 194 0
12 PSR J1023+0038 Psr 10 23 47.6841824712 +00 38 41.005893516     17.31     GV 470 0
13 PSR J1231-1411 Psr 12 31 11.3069 -14 11 43.628           ~ 139 0
14 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
15 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
16 SAX J1808.4-3658 LXB 18 08 27.58 -36 58 43.9           ~ 1051 0
17 V* V5511 Sgr LXB 18 13 39.03 -33 46 22.3   18.61 18.33 18.05   ~ 215 0
18 PSR J1820-30A Psr 18 23 40.4842 -30 21 39.920           ~ 168 1
19 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 854 3
20 PSR J2017+0603 Psr 20 17 22.7048 +06 03 05.585           ~ 120 1
21 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 129 1
22 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
23 PSR J2214+3000 Psr 22 14 38.8480 +30 00 38.209           ~ 136 0
24 PSR J2241-5236 Psr 22 41 42.03161 -52 36 36.2492           ~ 143 1
25 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 124 0

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