2014ApJS..213....6J


Query : 2014ApJS..213....6J

2014ApJS..213....6J - Astrophys. J., Suppl. Ser., 213, 6 (2014/July-0)

Constraints on the emission geometries and spin evolution of gamma-ray millisecond pulsars.

JOHNSON T.J., VENTER C., HARDING A.K., GUILLEMOT L., SMITH D.A., KRAMER M., CELIK O., DEN HARTOG P.R., FERRARA E.C., HOU X., LANDE J. and RAY P.S.

Abstract (from CDS):

Millisecond pulsars (MSPs) are a growing class of gamma-ray emitters. Pulsed gamma-ray signals have been detected from more than 40 MSPs with the Fermi Large Area Telescope (LAT). The wider radio beams and more compact magnetospheres of MSPs enable studies of emission geometries over a broader range of phase space than non-recycled radio-loud gamma-ray pulsars. We have modeled the gamma-ray light curves of 40 LAT-detected MSPs using geometric emission models assuming a vacuum retarded-dipole magnetic field. We modeled the radio profiles using a single-altitude hollow-cone beam, with a core component when indicated by polarimetry; however, for MSPs with gamma-ray and radio light curve peaks occurring at nearly the same rotational phase, we assume that the radio emission is co-located with the gamma rays and caustic in nature. The best-fit parameters and confidence intervals are determined using a maximum likelihood technique. We divide the light curves into three model classes, with gamma-ray peaks trailing (Class I), aligned (Class II), or leading (Class III) the radio peaks. Outer gap and slot gap (two-pole caustic) models best fit roughly equal numbers of Class I and II, while Class III are exclusively fit with pair-starved polar cap models. Distinguishing between the model classes based on typical derived parameters is difficult. We explore the evolution of the magnetic inclination angle with period and spin-down power, finding possible correlations. While the presence of significant off-peak emission can often be used as a discriminator between outer gap and slot gap models, a hybrid model may be needed.

Abstract Copyright: ∼

Journal keyword(s): acceleration of particles - gamma rays: stars - pulsars: general

Simbad objects: 46

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Number of rows : 46
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 J0023+0923 Psr 00 23 16.890 +09 23 24.18           ~ 137 0
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 J0103+48 Psr 01 02 50.6687164 +48 39 42.769776           ~ 41 0
6 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
7 PSR J0340+41 Psr 03 40 23.2887 +41 30 45.300           ~ 91 0
8 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
9 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
10 PSR J0610-2100 Psr 06 10 13.602953 -21 00 27.74435           ~ 116 0
11 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
12 PSR J0614-3329 Psr 06 14 10.3479 -33 29 54.116           ~ 134 1
13 PSR J0633+1746 Psr 06 33 54.153 +17 46 12.91           ~ 1308 0
14 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
15 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 286 1
16 PSR J1124-36 Psr 11 24 01.1169434 -36 53 19.108887           ~ 63 0
17 PSR J1125-58 Psr 11 25 44.352943 -58 25 16.85965           ~ 55 1
18 PSR J1231-1411 Psr 12 31 11.3069 -14 11 43.628           ~ 139 0
19 PSR J1446-4701 Psr 14 46 35.709721 -47 01 26.79678           ~ 82 1
20 PSR J1514-4946 Psr 15 14 19.1142 -49 46 15.528           ~ 55 0
21 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
22 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
23 PSR J1658-5324 Psr 16 58 39.343556 -53 24 06.97315           ~ 47 0
24 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
25 PSR J1741+1351 Psr 17 41 31.1499024 +13 51 44.279709           ~ 122 0
26 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
27 PSR J1747-4036 Psr 17 47 48.715690 -40 36 54.79950           ~ 83 0
28 PSR J1810+17 Psr 18 10 37.2791131488 +17 44 37.425884136           ~ 147 1
29 PSR J1820-30A Psr 18 23 40.4842 -30 21 39.920           ~ 168 1
30 NGC 6624 GlC 18 23 40.51 -30 21 39.7           ~ 939 1
31 PSR J1824-2452A Psr 18 24 32.009 -24 52 11.10           ~ 529 2
32 IGR J18245-2452 LXB 18 24 32.50 -24 52 07.8           ~ 253 0
33 M 28 GlC 18 24 32.89 -24 52 11.4           ~ 821 0
34 PSR J1858-2216 Psr 18 58 04.42 -22 19 13.7           ~ 39 0
35 PSR J1902-5105 Psr 19 02 02.8476 -51 05 56.969           ~ 64 0
36 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
37 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 854 3
38 PSR J2017+0603 Psr 20 17 22.7048 +06 03 05.585           ~ 120 1
39 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 129 1
40 PSR J2047+1053 Psr 20 47 00.000 +10 53 00.00           ~ 47 0
41 V* LY Aqr Psr 20 51 07.52058 -08 27 37.6100           ~ 236 2
42 PSR J2124-3358 Psr 21 24 43.834930 -33 58 45.49195           ~ 337 1
43 PSR J2214+3000 Psr 22 14 38.8480 +30 00 38.209           ~ 136 0
44 PSR J2215+51 Psr 22 15 32.6869149432 +51 35 36.400854912           ~ 176 0
45 PSR J2241-5236 Psr 22 41 42.03161 -52 36 36.2492           ~ 143 1
46 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 124 0

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