2013ApJ...775...47C


Query : 2013ApJ...775...47C

2013ApJ...775...47C - Astrophys. J., 775, 47 (2013/September-3)

Pulsar state switching from Markov transitions and stochastic resonance.

CORDES J.M.

Abstract (from CDS):

Markov processes are shown to be consistent with metastable states seen in pulsar phenomena, including intensity nulling, pulse-shape mode changes, subpulse drift rates, spin-down rates, and X-ray emission, based on the typically broad and monotonic distributions of state lifetimes. Markovianity implies a nonlinear magnetospheric system in which state changes occur stochastically, corresponding to transitions between local minima in an effective potential. State durations (though not transition times) are thus largely decoupled from the characteristic timescales of various magnetospheric processes. Dyadic states are common but some objects show at least four states with some transitions forbidden. Another case is the long-term intermittent pulsar B1931+24 that has binary radio-emission and torque states with wide, but non-monotonic duration distributions. It also shows a quasi-period of 38±5 days in a 13 yr time sequence, suggesting stochastic resonance in a Markov system with a forcing function that could be strictly periodic or quasi-periodic. Nonlinear phenomena are associated with time-dependent activity in the acceleration region near each magnetic polar cap. The polar-cap diode is altered by feedback from the outer magnetosphere and by return currents from the equatorial region outside the light cylinder that may also cause the neutron star to episodically charge and discharge. Orbital perturbations of a disk or current sheet provide a natural periodicity for the forcing function in the stochastic-resonance interpretation of B1931+24. Disk dynamics may introduce additional timescales in observed phenomena. Future work can test the Markov interpretation, identify which pulsar types have a propensity for state changes, and clarify the role of selection effects.

Abstract Copyright: ∼

Journal keyword(s): acceleration of particles - instabilities - magnetic fields - plasmas - pulsars: general - stars: neutron

Simbad objects: 25

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Number of rows : 25
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 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
4 PSR B0809+74 Psr 08 14 59.500 +74 29 05.70           ~ 425 0
5 PSR B0818-13 Psr 08 20 26.40700 -13 50 56.3200           ~ 229 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 B0834+06 Psr 08 37 05.64620 +06 10 15.8700           ~ 472 0
9 PSR B0835-41 Psr 08 37 21.1943 -41 35 14.563     12.69     ~ 149 0
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 B1112+50 Psr 11 15 38.400 +50 30 12.29           ~ 154 0
14 PSR B1133+16 Psr 11 36 03.09460 +15 51 15.9000           ~ 715 0
15 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
16 PSR B1822-09 Psr 18 25 30.62000 -09 35 22.0000           ~ 382 0
17 PSR J1832+0029 Psr 18 32 50.7 +00 29 27           ~ 59 0
18 PSR J1841-0500 Psr 18 41 18.14 -05 00 19.5           ~ 54 0
19 PSR J1933+2421 Psr 19 33 37.83 +24 36 39.6           ~ 157 0
20 PSR B1944+17 Psr 19 46 53.044 +18 05 41.24           ~ 252 0
21 PSR B2021+51 Psr 20 22 49.8730 +51 54 50.233           ~ 288 1
22 PSR B2034+19 Psr 20 37 14.54 +19 42 54.3           ~ 41 0
23 PSR B2111+46 Psr 21 13 24.3295 +46 44 08.844           ~ 226 1
24 PSR B2303+30 Psr 23 05 58.3212 +31 00 01.281           ~ 216 0
25 PSR B2319+60 Psr 23 21 55.213 +60 24 30.71     13.80     ~ 200 0

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