2021MNRAS.504.5741G


Query : 2021MNRAS.504.5741G

2021MNRAS.504.5741G - Mon. Not. R. Astron. Soc., 504, 5741-5753 (2021/July-2)

Rapid modification of neutron star surface magnetic field: a proposed mechanism for explaining radio emission state changes in pulsars.

GEPPERT U., BASU R., MITRA D., MELIKIDZE G.I. and SZKUDLAREK M.

Abstract (from CDS):

The radio emission in many pulsars shows sudden changes, usually within a period, that cannot be related to the steady state processes within the inner acceleration region (IAR) above the polar cap. These changes are often quasi-periodic in nature, where regular transitions between two or more stable emission states are seen. The durations of these states show a wide variety ranging from several seconds to hours at a time. There are strong, small-scale magnetic field structures and huge temperature gradients present at the polar cap surface. We have considered several processes that can cause temporal modifications of the local magnetic field structure and strength at the surface of the polar cap. Using different magnetic field strengths and scales, and also assuming realistic scales of the temperature gradients, the evolutionary time-scales of different phenomena affecting the surface magnetic field were estimated. We find that the Hall drift results in faster changes in comparison to both Ohmic decay and thermoelectric effects. A mechanism based on the partially screened gap (PSG) model of the IAR has been proposed, where the Hall and thermoelectric oscillations perturb the polar cap magnetic field to alter the sparking process in the PSG. This is likely to affect the observed radio emission resulting in the observed state changes.

Abstract Copyright: © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): stars: interiors - stars: magnetic field - stars: neutron - pulsars: general

Simbad objects: 31

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Number of rows : 31
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 B0031-07 Psr 00 34 08.9100 -07 21 56.000           ~ 350 0
2 PSR B0329+54 Psr 03 32 59.3370698592 +54 34 45.028206408           ~ 690 1
3 PSR B0355+54 Psr 03 58 53.7165 +54 13 13.727           ~ 465 1
4 PSR B0611+22 Psr 06 14 17.0324288405 +22 29 57.017874999           ~ 285 0
5 PSR B0809+74 Psr 08 14 59.500 +74 29 05.70           ~ 425 0
6 PSR B0823+26 Psr 08 26 51.5068 +26 37 21.297           ~ 541 1
7 PSR B0826-34 Psr 08 28 16.6 -34 17 07           ~ 167 0
8 PSR B0844-35 Psr 08 46 06.07120 -35 33 40.9100           ~ 89 0
9 PSR B0919+06 Psr 09 22 13.85000 +06 38 19.0000           ~ 329 1
10 PSR J0941-39 Psr 09 42 -39.7           ~ 26 0
11 PSR B0943+10 Psr 09 46 07.31 +09 51 57.3           ~ 364 1
12 PSR J1107-5907 Psr 11 07 34.46 -59 07 18.7           ~ 42 0
13 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
14 PSR B1322-66 Psr 13 26 02.70600 -67 00 50.1000           ~ 55 0
15 PSR B1358-63 Psr 14 01 52.45000 -63 57 42.0000           ~ 83 0
16 PSR J1658-4306 Psr 16 58 16.6 -43 06 50           ~ 7 0
17 PSR B1658-37 Psr 17 01 18.45000 -37 26 27.2000           ~ 45 0
18 PSR J1703-4902 Psr 17 03 54.54100 -48 52 01.0400           ~ 42 0
19 PSR J1752+2359 Psr 17 52 35.42 +23 59 48.2           ~ 64 0
20 PSR B1819-22 Psr 18 22 58.95000 -22 56 29.0000           ~ 123 0
21 PSR B1822-09 Psr 18 25 30.62000 -09 35 22.0000           ~ 382 0
22 PSR J1843-0211 Psr 18 43 30.33 -02 11 02.8           ~ 20 0
23 PSR B1859+07 Psr 19 01 39.02000 +07 16 33.6000     14.03     ~ 88 0
24 PSR B1918+19 Psr 19 21 03.799 +19 48 44.70           ~ 119 0
25 PSR B1926+18 Psr 19 29 16.78 +18 44 59.5           ~ 35 0
26 PSR J1938+2213 Psr 19 38 14.180 +22 13 12.68           ~ 24 0
27 PSR B1944+17 Psr 19 46 53.044 +18 05 41.24           ~ 252 0
28 PSR B2003-08 Psr 20 06 16.36500 -08 07 02.1600           ~ 113 0
29 PSR B2020+28 Psr 20 22 37.0671 +28 54 23.104           ~ 330 1
30 PSR B2303+30 Psr 23 05 58.3212 +31 00 01.281           ~ 216 0
31 PSR B2319+60 Psr 23 21 55.213 +60 24 30.71     13.80     ~ 200 0

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