2023ApJ...948..106M


Query : 2023ApJ...948..106M

2023ApJ...948..106M - Astrophys. J., 948, 106 (2023/May-2)

Measuring the Vortex-Nucleus Pinning Force from Pulsar Glitch Rates.

MELATOS A. and MILLHOUSE M.

Abstract (from CDS):

Superfluid vortex avalanches are one plausible cause of pulsar glitch activity. If they occur according to a state-dependent Poisson process, the measured long-term glitch rate is determined by the spin-down rate of the stellar crust, ${\dot{{\rm{\Omega }}}}_{c}$, and two phenomenological parameters quantifying the vortex-nucleus pinning force: a crust-superfluid angular velocity lag threshold, Xcr, and a reference unpinning rate, λ0. A Bayesian analysis of 541 glitches in 177 pulsars, with Ng ≥ 1 events per pulsar, yields ${X}_{\mathrm{cr}}={0.15}_{-0.04}^{+0.09}\,\mathrm{rad}\,{{\rm{s}}}^{-1}$, ${\lambda }_{\mathrm{ref}}={7.6}_{-2.6}^{+3.7}\times {10}^{-8}\,{{\rm{s}}}^{-1}$, and $a=-{0.27}_{-0.03}^{+0.04}$ assuming the phenomenological rate law λ0 = λref[τ/(1 yr)]a, where τ denotes the characteristic spin-down age. The results are broadly similar, whether one includes or excludes quasiperiodic glitch activity, giant glitches, or pulsars with Ng = 0, up to uncertainties about the completeness of the sample and the total observation time per pulsar. The Xcr and λ0 estimates are consistent with first-principles calculations based on nuclear theory, e.g., in the semiclassical local density approximation.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Pulsars - Neutron stars - Stellar rotation - Nuclear astrophysics

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 - 2026
#notes
1 PSR J0537-6910 Psr 05 37 46.66 -69 10 17.1           ~ 309 1
2 PSR J0631+10 Psr 06 31 27.369 +10 37 05.63           ~ 152 0
3 NAME Vela Pulsar Psr 08 35 20.65525 -45 10 35.1545     15.10     ~ 2446 1
4 PSR J1016-58 Psr 10 16 21.266 -58 57 11.70           ~ 129 3
5 PSR J1023-5746 Psr 10 23 02.84 -57 46 06.9           ~ 70 0
6 PSR B1046-58 Psr 10 48 13.10000 -58 32 03.0000           ~ 293 0
7 PSR J1301-6305 Psr 13 02 47.9992676 -63 10 48.001099           ~ 139 2
8 PSR B1338-62 Psr 13 41 42.63 -62 20 20.7           ~ 152 1
9 PSR J1357-6429 Psr 13 57 02.525 -64 29 29.89           ~ 171 1
10 PSR J1420-6048 Psr 14 20 08.190 -60 48 14.85           ~ 214 0
11 PSR J1614-5048 Psr 16 14 11.29 -50 48 03.5           ~ 128 0
12 PSR B1706-44 Psr 17 09 42.62000 -44 29 12.0000     13.30     ~ 670 1
13 PSR B1727-33 Psr 17 30 32.559 -33 50 39.40           ~ 130 1
14 PSR B1737-30.2 Psr 17 40 33.98000 -30 15 22.0000           ~ 236 0
15 PSR B1757-24 Psr 18 01 00.016 -24 51 27.50           ~ 258 1
16 PSR B1800-21 Psr 18 03 51.40000 -21 37 07.0000           ~ 278 1
17 PSR B1823-13 Psr 18 26 13.06 -13 34 48.1           ~ 460 1
18 PSR B1930+22 Psr 19 32 22.8565447656 +22 20 52.063074024     14.52     ~ 149 0
19 PSR J2021+3651 Psr 20 21 05.40 +36 51 04.5           ~ 218 1
20 PSR J2111+4606 Psr 21 11 24.125 +46 06 30.66           ~ 49 0
21 PSR J2229+6114 Psr 22 29 05.262 +61 14 08.48           ~ 252 2

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