2015ApJ...800...76S


Query : 2015ApJ...800...76S

2015ApJ...800...76S - Astrophys. J., 800, 76 (2015/February-2)

On the origin of radio emission from magnetars.

SZARY A., MELIKIDZE G.I. and GIL J.

Abstract (from CDS):

Magnetars are the most magnetized objects in the known universe. Powered by the magnetic energy, and not by the rotational energy as in the case of radio pulsars, they have long been regarded as a completely different class of neutron stars. The discovery of pulsed radio emission from a few magnetars weakened the idea of a clean separation between magnetars and normal pulsars. We use the partially screened gap (PSG) model to explain radio emission of magnetars. The PSG model requires that the temperature of the polar cap is equal to the so-called critical value, i.e., the temperature at which the thermal ions outflowing from the stellar surface screen the acceleration gap. We show that a magnetar has to fulfill the temperature, power, and visibility conditions in order to emit radio waves. First, in order to form PSG, the residual temperature of the surface has to be lower than the critical value. Second, since the radio emission is powered by the rotational energy, it has to be high enough to enable heating of the polar cap by backstreaming particles to the critical temperature. Finally, the structure of the magnetic field has to be altered by magnetospheric currents in order to widen a radio beam and increase the probability of detection. Our approach allows us to predict whether a magnetar can emit radio waves using only its rotational period, period derivative, and surface temperature in the quiescent mode.

Abstract Copyright:

Journal keyword(s): pulsars: general - stars: magnetars - stars: neutron

Simbad objects: 23

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Number of rows : 23
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 J0100-7211 Psr 01 00 42.86 -72 11 33.3   17.69 17.82     B3V 95 0
2 PSR J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 570 0
3 NAME Sgr J0418+5729 gam 04 18 33.867 +57 32 22.91           ~ 223 0
4 2XMM J050106.5+451634 X 05 01 08.0 +45 16 31           ~ 122 0
5 PSR B0525-66 Psr 05 26 00.7 -66 04 35           ~ 545 1
6 2E 2336 HXB 10 50 08.93 -59 53 19.9           Be 405 0
7 PSR J1550-5418 Psr 15 50 54.18 -54 18 23.9           ~ 409 1
8 PSR J1622-4950 Psr 16 22 44.80 -49 50 54.4           ~ 145 0
9 GRB 980618A gB 16 35 52 -47 35.2           ~ 263 0
10 PSR J1647-4552 Psr 16 47 10.18 -45 52 16.7           ~ 198 1
11 PSR J1708-4008 Psr 17 08 49.0 -40 09 10           ~ 293 0
12 [AAB2008] 1 X 17 14 05.758 -38 10 31.32           ~ 60 1
13 PSR J1745-2900 Psr 17 45 40.1640 -29 00 29.818           ~ 315 0
14 PSR J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1240 2
15 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 463 0
16 1WGA J1822.2-1604 X 18 22 18.32 -16 04 27.2           ~ 130 0
17 NAME Sgr 1833-0832 gam 18 33 46.0 -08 32 13           ~ 80 0
18 SWIFT J1834.9-0846 N*? 18 34 52.768 -08 45 40.83           ~ 86 0
19 PSR J1841-0456 Psr 18 41 19.29 -04 56 11.4           ~ 265 1
20 3XMM J185246.6+003317 Psr 18 52 46.60 +00 33 20.9           ~ 37 0
21 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 857 0
22 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 633 1
23 CTB 109 BL? 23 01 35 +58 53.0           ~ 344 0

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