2012ApJ...744...34V


Query : 2012ApJ...744...34V

2012ApJ...744...34V - Astrophys. J., 744, 34 (2012/January-1)

Modeling phase-aligned gamma-ray and radio millisecond pulsar light curves.

VENTER C., JOHNSON T.J. and HARDING A.K.

Abstract (from CDS):

Since the discovery of the first eight gamma-ray millisecond pulsars (MSPs) by the Fermi Large Area Telescope, this population has been steadily expanding. Four of the more recent detections, PSR J0034-0534, PSR J1939+2134 (B1937+21; the first MSP ever discovered), PSR J1959+2048 (B1957+20; the first discovery of a black widow system), and PSR J2214+3000, exhibit a phenomenon not present in the original discoveries: nearly phase-aligned radio and gamma-ray light curves (LCs). To account for the phase alignment, we explore models where both the radio and gamma-ray emission originate either in the outer magnetosphere near the light cylinder or near the polar caps. Using a Markov Chain Monte Carlo technique to search for best-fit model parameters, we obtain reasonable LC fits for the first three of these MSPs in the context of "altitude-limited" outer gap (alOG) and two-pole caustic (alTPC) geometries (for both gamma-ray and radio emission). These models differ from the standard outer gap (OG)/two-pole caustic (TPC) models in two respects: the radio emission originates in caustics at relatively high altitudes compared to the usual conal radio beams, and we allow both the minimum and maximum altitudes of the gamma-ray and radio emission regions to vary within a limited range (excluding the minimum gamma-ray altitude of the alTPC model, which is kept constant at the stellar radius, and that of the alOG model, which is set to the position-dependent null charge surface altitude). Alternatively, phase-aligned solutions also exist for emission originating near the stellar surface in a slot gap scenario ("low-altitude slot gap" (laSG) models). We find that the alTPC models provide slightly better LC fits than the alOG models, and both of these give better fits than the laSG models (for the limited range of parameters considered in the case of the laSG models). Thus, our fits imply that the phase-aligned LCs are likely of caustic origin, produced in the outer magnetosphere, and that the radio emission for these pulsars may come from close to the light cylinder. In addition, we were able to constrain the minimum and maximum emission altitudes with typical uncertainties of ∼30% of the light cylinder radius. Our results therefore describe a third gamma-ray MSP subclass, in addition to the two previously found by Venter et al.: those with LCs fit by standard OG/TPC models and those with LCs fit by pair-starved polar cap models.

Abstract Copyright:

Journal keyword(s): acceleration of particles - gamma rays: stars - pulsars: individual (PSR J0034-0534, PSR J1939+2134, PSR J1959+2048) - radiation mechanisms: non-thermal

Simbad objects: 21

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Number of rows : 21
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 J0030+0451 Psr 00 30 27.4277 +04 51 39.710           ~ 462 1
2 PSR J0034-05 Psr 00 34 21.8281 -05 34 36.620           ~ 182 0
3 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 336 2
4 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 906 0
5 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5261 0
6 PSR B0613-02.0 Psr 06 13 43.9759 -02 00 47.228           ~ 269 1
7 PSR J0614-3329 Psr 06 14 10.3479 -33 29 54.116           ~ 100 1
8 PSR J0737-3039A Psr 07 37 51.24720 -30 39 40.6700           ~ 280 1
9 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 289 1
10 PSR J1025-07 Psr 10 24 38.6991893112 -07 19 19.045523388     19.81 18.78 18.00 ~ 241 1
11 PSR J1231-1411 Psr 12 31 11.3069 -14 11 43.628           ~ 113 0
12 PSR J1614-2230 Psr 16 14 36.5070 -22 30 31.207           ~ 393 1
13 PSR J1744-1134 Psr 17 44 29.4172 -11 34 54.710           ~ 271 1
14 PSR J1824-2452A Psr 18 24 32.009 -24 52 11.10           ~ 500 2
15 PSR B1919+21 Psr 19 21 44.815 +21 53 02.25           ~ 384 0
16 PSR B1937+21 Psr 19 39 39.6 +21 37 22           ~ 1067 2
17 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 807 3
18 PSR J2017+0603 Psr 20 17 22.7048 +06 03 05.585           ~ 100 1
19 PSR J2124-3358 Psr 21 24 43.8464 -33 58 44.961           ~ 299 1
20 PSR J2214+3000 Psr 22 14 38.8480 +30 00 38.209           ~ 109 0
21 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 105 0

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