2011ApJ...728L..19R


Query : 2011ApJ...728L..19R

2011ApJ...728L..19R - Astrophys. J., 728, L19 (2011/February-2)

A non-radial oscillation model for pulsar state switching.

ROSEN R., McLAUGHLIN M.A. and THOMPSON S.E.

Abstract (from CDS):

Pulsars are unique astrophysical laboratories because of their clock-like timing precision, providing new ways to test general relativity and detect gravitational waves. One impediment to high-precision pulsar timing experiments is timing noise. Recently, Lyne et al. showed that the timing noise in a number of pulsars is due to quasi-periodic fluctuations in the pulsars' spin-down rates and that some of the pulsars have associated changes in pulse profile shapes. Here we show that a non-radial oscillation model based on asteroseismological theory can explain these quasi-periodic fluctuations. Application of this model to neutron stars will increase our knowledge of neutron star emission and neutron star interiors and may improve pulsar timing precision.

Abstract Copyright: ∼

Journal keyword(s): pulsars: general - stars: neutron - stars: oscillations (including pulsations) - white dwarfs

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 - 2026
#notes
1 PSR B0740-28 Psr 07 42 49.0730 -28 22 43.510           ~ 445 0
2 PSR B0809+74 Psr 08 14 59.500 +74 29 05.70           ~ 425 0
3 PSR B0919+06 Psr 09 22 13.85000 +06 38 19.0000           ~ 329 1
4 PSR B0943+10 Psr 09 46 07.31 +09 51 57.3           ~ 364 1
5 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
6 V* GW Vir WD* 12 01 45.9731868264 -03 45 40.628670300   14.87 15.04     DOQZ1 505 0
7 PSR B1540-06 Psr 15 43 30.1373 -06 20 45.332           ~ 131 1
8 PSR B1642-03 Psr 16 45 02.0330 -03 17 57.200           ~ 394 0
9 GD 358 WD* 16 47 18.3925183824 +32 28 32.862804384 12.511 13.530 13.653 13.752 13.852 DB2 364 0
10 PSR B1714-34 Psr 17 17 20.30000 -34 25 00.3100           ~ 55 0
11 PSR B1818-04 Psr 18 20 52.5920 -04 27 37.120           ~ 230 0
12 PSR B1822-09 Psr 18 25 30.62000 -09 35 22.0000           ~ 382 0
13 PSR B1826-17 Psr 18 29 43.15000 -17 51 13.0000           ~ 136 0
14 PSR B1828-10 Psr 18 30 47.566 -10 59 27.90           ~ 190 1
15 PSR B1839+09 Psr 18 41 55.92100 +09 12 07.2900           ~ 134 0
16 PSR B1903+07 Psr 19 05 53.62 +07 09 19.4           ~ 43 0
17 PSR B1907+00 Psr 19 09 35.25200 +00 07 56.8400           ~ 91 0
18 PSR B1930+20 Psr 19 32 08.023 +20 20 46.41           ~ 87 0
19 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 801 0
20 PSR J1933+2421 Psr 19 33 37.83 +24 36 39.6           ~ 157 0
21 PSR J2037+3621 Psr 20 37 27.44 +36 21 24.1           ~ 62 0
22 PSR J2043+2740 Psr 20 43 43.5 +27 40 56           ~ 137 0
23 PSR B2148+63 Psr 21 49 58.7033 +63 29 44.277           ~ 96 0

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