Timing and evolution of PSR B0950+08

We present timing solutions of PSR B0950+08, using 14 years of observations from the Nanshan 26-m Radio Telescope of Xinjiang Astronomical Observatory. The braking index of PSR B0950+08 varies from -367 392 to 168 883, which shows an oscillation with large amplitude (∼105) and uncertainty. Consideri...

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Bibliographic Details
Main Authors: Huang, H.-T (Author), Yuan, J.-P (Author), Zheng, X.-P (Author), Zhou, X. (Author)
Format: Article
Language:English
Published: Oxford University Press 2022
Subjects:
Online Access:View Fulltext in Publisher
LEADER 02826nam a2200385Ia 4500
001 10.1093-mnras-stac703
008 220510s2022 CNT 000 0 und d
020 |a 00358711 (ISSN) 
245 1 0 |a Timing and evolution of PSR B0950+08 
260 0 |b Oxford University Press  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1093/mnras/stac703 
520 3 |a We present timing solutions of PSR B0950+08, using 14 years of observations from the Nanshan 26-m Radio Telescope of Xinjiang Astronomical Observatory. The braking index of PSR B0950+08 varies from -367 392 to 168 883, which shows an oscillation with large amplitude (∼105) and uncertainty. Considering the variation of braking indices and the most probable kinematic age of PSR B0950+08, a model with long-term magnetic field decay modulated by short-term oscillations is proposed to explain the timing data. With this magnetic field decay model, we discuss the spin and thermal evolution of PSR B0950+08. The uncertainties of its age are also considered. The results show that three-component oscillations are the more reasonable for the spin-frequency derivative distributions of PSR B0950+08, and the initial spin period of PSR B0950+08 must be shorter than 97 ms when the age is equal to the lower bound of its kinematic age. The standard cooling model could explain the surface temperature of PSR B0950+08 with its most probable kinematic age. Vortex creep heating with a long-term magnetic field decay could maintain a relatively high temperature at the later stages of evolution and explain the thermal emission data of old and warm pulsars. Coupling with the long-term magnetic field decay, an explanation of the temperature of PSR B0950+08 with roto-chemical heating needs an implausibly short initial rotation period (P0 ≤17ms). The spin and thermal evolution of pulsars should be studied simultaneously. Future timing, ultraviolet or X-ray observations are essential for studying the evolution and interior properties of pulsars. © 2022 The Author(s). 
650 0 4 |a Field decays 
650 0 4 |a Kinematics 
650 0 4 |a Magnetic fields 
650 0 4 |a Magnetic-field 
650 0 4 |a Pulsar: individual: PSR b0950+08 
650 0 4 |a Pulsars 
650 0 4 |a pulsars: individual: PSR B0950+08 
650 0 4 |a Pulsars:individual 
650 0 4 |a Spin evolution 
650 0 4 |a Star: evolution 
650 0 4 |a Stars: evolution 
650 0 4 |a stars: magnetic field 
650 0 4 |a Stars: magnetic field 
650 0 4 |a stars: neutron 
650 0 4 |a Stars: neutrons 
650 0 4 |a Thermal evolution 
650 0 4 |a Timing circuits 
650 0 4 |a Uncertainty 
700 1 |a Huang, H.-T.  |e author 
700 1 |a Yuan, J.-P.  |e author 
700 1 |a Zheng, X.-P.  |e author 
700 1 |a Zhou, X.  |e author 
773 |t Monthly Notices of the Royal Astronomical Society