Testing Models of Magnetic Field Evolution of Neutron Stars with the Statistical Properties of Their Spin Evolutions

TL;DR

This paper evaluates models of neutron star magnetic field evolution by analyzing pulsar spin data, finding that a power-law decay model best explains observed spin derivatives and discussing implications for magnetic decay mechanisms.

Contribution

It introduces a phenomenological model with a power-law magnetic field decay and short-term oscillations, improving understanding of pulsar spin evolution and magnetic field decay.

Findings

Standard magnetosphere model fails to predict spin derivative signs.

Exponential magnetic decay is inconsistent with observed data.

Power-law decay model successfully explains spin derivative statistics.

Abstract

We test models for the evolution of neutron star (NS) magnetic fields (B). Our model for the evolution of the NS spin is taken from an analysis of pulsar timing noise presented by Hobbs et al. (2010). We first test the standard model of a pulsar's magnetosphere in which B does not change with time and magnetic dipole radiation is assumed to dominate the pulsar's spin-down. We find this model fails to predict both the magnitudes and signs of the second derivatives of the spin frequencies ($\ddot{\nu}$). We then construct a phenomenological model of the evolution of $B$, which contains a long term decay (LTD) modulated by short term oscillations (STO); a pulsar's spin is thus modified by its B-evolution. We find that an exponential LTD is not favored by the observed statistical properties of $\ddot{\nu}$ for young pulsars and fails to explain the fact that $\ddot{\nu}$ is negative for roughly half of the old pulsars. A simple power-law LTD can explain all the observed statistical properties of $\ddot{\nu}$. Finally we discuss some physical implications of our results to models of the B-decay of NSs and suggest reliable determination of the true ages of many young NSs is needed, in order to constrain further the physical mechanisms of their B-decay. Our model can be further tested with the measured evolutions of $\dot{\nu}$ and $\ddot{\nu}$ for an individual pulsar; the decay index, oscillation amplitude and period can also be determined this way for the pulsar.