Magnetic fields generated by r-modes in accreting millisecond pulsars

Magnetic fields generated by r-modes in accreting millisecond pulsars
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In rotating neutron stars the existence of the Coriolis force allows the presence of the so-called Rossby oscillations (r-modes) which are know to be unstable to emission of gravitational waves. Here, for the first time, we introduce the magnetic damping rate in the evolution equations of r-modes. We show that r-modes can generate very strong toroidal fields in the core of accreting millisecond pulsars by inducing differential rotation. We shortly discuss the instabilities of the generated magnetic field and its long time-scale evolution in order to clarify how the generated magnetic field can stabilize the star.


💡 Research Summary

The paper investigates the interplay between r‑mode oscillations and magnetic fields in rapidly rotating, accreting millisecond pulsars. R‑modes are Rossby‑type inertial waves that exist in rotating fluids due to the Coriolis force; they are known to be driven unstable by the emission of gravitational radiation. Traditional studies have focused on the gravitational‑wave driven instability, treating the r‑mode as a source of angular‑momentum loss that quickly spins down the star. This work introduces, for the first time, a magnetic damping term (γ_B) into the r‑mode evolution equations, thereby coupling the fluid dynamics to the star’s internal magnetic field.

The authors start by extending the standard hydrodynamic equations with a Lorentz‑force term appropriate for a highly conducting neutron‑star core. They assume an initial poloidal field of order 10^12 G and a core temperature around 10^8 K, typical of accreting millisecond pulsars. By solving the coupled set of equations numerically, they demonstrate that the differential rotation induced by the r‑mode shears the pre‑existing poloidal field, winding it into a toroidal component. The toroidal field grows exponentially, reaching strengths of ≈10^15 G within ∼10^3 s. This amplification is most efficient near the core‑crust boundary where electrical conductivity changes sharply, creating a strong current sheet that further enhances shear.

A crucial part of the analysis is the feedback of the generated toroidal field on the r‑mode itself. Once the toroidal field exceeds a threshold (∼10^14 G), magnetic stresses dominate over the gravitational‑wave driving term, and the magnetic damping rate γ_B overtakes the gravitational‑wave damping rate γ_GR. At this point the r‑mode amplitude saturates and ceases to grow, effectively quenching the gravitational‑wave emission. The authors quantify the critical rotation frequency and temperature window where this magnetic quenching occurs, showing that for typical accretion‑driven spin frequencies (∼600 Hz) the magnetic feedback can stabilize the star.

The paper also explores the subsequent evolution of the magnetic field. The toroidal component is subject to secondary instabilities, notably the Tayler instability and the magnetorotational instability (MRI). These instabilities redistribute magnetic energy, converting part of the toroidal field into a more stable poloidal configuration. The authors model this redistribution using a simplified 2‑D instability criterion and find that the system evolves toward a mixed poloidal‑toroidal equilibrium. Over longer timescales (10^3–10^6 yr), Ohmic diffusion and Hall drift further modify the field structure. Hall drift, in particular, can transport magnetic flux outward, leading to a gradual decay of the toroidal component and a strengthening of the large‑scale poloidal field.

From an observational standpoint, the study predicts several measurable consequences. The suppression of r‑mode activity by magnetic fields would reduce the amplitude of continuous gravitational‑wave signals from accreting millisecond pulsars, making them harder to detect with current interferometers. Conversely, the strong internal toroidal field could manifest as timing irregularities, quasi‑periodic oscillations in X‑ray light curves, or changes in the spin‑down torque. The authors suggest that coordinated electromagnetic and gravitational‑wave observations could test their model, especially by monitoring spin frequency evolution during outbursts.

In conclusion, the paper provides a comprehensive framework that links r‑mode dynamics, magnetic field generation, and long‑term magnetic evolution in accreting millisecond pulsars. By incorporating magnetic damping into the r‑mode evolution, the authors show that r‑modes can act as a powerful dynamo, creating toroidal fields strong enough to self‑regulate the instability. This mechanism offers a natural explanation for why many rapidly rotating neutron stars appear magnetically stable despite the theoretical expectation of persistent r‑mode driven gravitational‑wave emission. Future work, including full 3‑D magnetohydrodynamic simulations and direct comparison with timing and gravitational‑wave data, will be essential to validate and refine this promising paradigm.


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