2000MNRAS.311..555H


Query : 2000MNRAS.311..555H

2000MNRAS.311..555H - Mon. Not. R. Astron. Soc., 311, 555-564 (2000/January-3)

Polarization evolution in strong magnetic fields.

HEYL J.S. and SHAVIV N.J.

Abstract (from CDS):

Extremely strong magnetic fields change the vacuum index of refraction. Although this polarization-dependent effect is small for typical neutron stars, it is large enough to decouple the polarization states of photons travelling within the field. The photon states evolve adiabatically and follow the changing magnetic field direction. The combination of a rotating magnetosphere and a frequency-dependent-state decoupling predicts polarization phase lags between different wavebands, if the emission process takes place well within the light cylinder. This QED effect may allow observations to distinguish between different pulsar-emission mechanisms and to reconstruct the structure of the magnetosphere.

Abstract Copyright: 2000, Royal Astronomical Society

Journal keyword(s): magnetic fields - polarization - stars: neutron

Simbad objects: 12

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Number of rows : 12
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 J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
2 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
3 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
4 PSR B0540-69 Psr 05 40 11.2000490438 -69 19 54.198559829           ~ 976 3
5 RX J0720.4-3125 N* 07 20 24.961 -31 25 50.21   26.1   27.0   ~ 316 0
6 NAME Vela Pulsar Psr 08 35 20.65525 -45 10 35.1545     15.10     ~ 2446 1
7 PSR B1509-58 Psr 15 13 47.6 -59 07 54     13.06     ~ 879 1
8 PSR J1820-30A Psr 18 23 40.4842 -30 21 39.920           ~ 168 1
9 PSR J1824-2452A Psr 18 24 32.009 -24 52 11.10           ~ 529 2
10 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
11 PSR B1951+32 Psr 19 52 58.181 +32 52 40.98           ~ 615 2
12 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 854 3

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