2014MNRAS.443.3586S


Query : 2014MNRAS.443.3586S

2014MNRAS.443.3586S - Mon. Not. R. Astron. Soc., 443, 3586-3593 (2014/October-1)

Anisotropic neutrino effect on magnetar spin: constraint on inner toroidal field.

SUWA Y. and ENOTO T.

Abstract (from CDS):

The ultrastrong magnetic field of magnetars modifies the neutrino cross-section due to the parity violation of the weak interaction and can induce asymmetric propagation of neutrinos. Such an anisotropic neutrino radiation transfers not only the linear momentum of a neutron star but also the angular momentum, if a strong toroidal field is embedded inside the stellar interior. As such, the hidden toroidal field implied by recent observations potentially affects the rotational spin evolution of new-born magnetars. We analytically solve the transport equation for neutrinos and evaluate the degree of anisotropy that causes the magnetar to spin-up or spin-down during the early neutrino cooling phase. Supposing that after the neutrino cooling phase the dominant process causing the magnetar spin-down is the canonical magnetic dipole radiation, we compare the solution with the observed present rotational periods of anomalous X-ray pulsars 1E 1841-045 and 1E 2259+586, whose poloidal (dipole) fields are ∼ 1015 and 1014 G, respectively. Combining with the supernova remnant age associated with these magnetars, the present evaluation implies a rough constraint of global (average) toroidal field strength at Bφ ≲ 1015 G.

Abstract Copyright: © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): magnetic fields - neutrinos - radiative transfer - stars: magnetars - pulsars: general

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 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 J1808-2024 Psr 18 08 39.32 -20 24 40.1           ~ 1240 2
14 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 463 0
15 1WGA J1822.2-1604 X 18 22 18.32 -16 04 27.2           ~ 130 0
16 NAME Sgr 1833-0832 gam 18 33 46.0 -08 32 13           ~ 80 0
17 SWIFT J1834.9-0846 N*? 18 34 52.768 -08 45 40.83           ~ 86 0
18 PSR J1841-0456 Psr 18 41 19.29 -04 56 11.4           ~ 265 1
19 GBS 1900+14 gB 19 07 13 +09 19.6           ~ 857 0
20 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 633 1
21 CTB 109 BL? 23 01 35 +58 53.0           ~ 344 0

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