Neutron Force on Proton Vortices in the Cores of Neutron Stars ✛ ✎ ✦

Original: "Neutron contribution to the force on a proton vortex in superconducting neutron-star matter"
arXiv:2607.09468 · 2026-07-10 · arXiv non-exclusive · independent analysis · 2 min
Taking into account the Fermi-liquid interaction between neutrons and protons reveals a new force component acting on proton vortices in superconducting neutron stars.

Context

In the cores of neutron stars, protons become superconducting, forming vortices with quantized magnetic flux. The forces acting on these vortices determine magnetic field evolution and oscillation damping. Traditionally, only the electron contribution was considered, but at finite temperatures, neutrons, as the normal component of the plasma, can also exert a force. This work fills that gap, using Fermi-liquid theory and quantum thermodynamics to describe neutron-proton interactions.

Methods

The authors applied the Boltzmann-Landau kinetic equation for neutrons, neglecting collisions (ballistic regime). The energy of neutron quasiparticles, obeying Fermi-Dirac statistics, is modified by Fermi-liquid coupling with the proton condensate, leading to scattering on the spatial gradient of the condensate momentum. The model assumes an infinitely thin vortex core and extreme type-II superconductivity (ξ ≪ λ). The calculation is done within the framework of Landau theory and the Bardeen–Cooper–Schrieffer (BCS) theory, using Maxwell's equations for electromagnetic fields.

Results

It is found that neutrons create a longitudinal force proportional to the transport scattering cross-section, which is mainly determined by the vortex core structure. Unlike electrons, the transverse (Magnus) force component is strictly zero, because the circulation of the effective 'magnetic' field induced by Fermi-liquid coupling vanishes due to the Meissner effect. Estimates of the ratio of the new force to the electron one give $D_n$/$D_e$ ~ (m*_n $γ_{np}$)^2 ($n_{n0}$/$n_{e0}$) ($p_{Fe}$/$p_{Fn}$) (λ/ξ) and in typical neutron star conditions is 0.01–0.1. Remarkably, the force disappears if neutron-proton interaction is turned off.

Implications

The result fundamentally changes the understanding of vortex dynamics: now the velocity difference between electrons and neutrons can be sustained without external forces, which is important for magnetic field evolution and oscillation damping. For magnetars and accreting neutron stars, where the core temperature can be fairly high, accounting for the neutron force becomes critically important.

Future development

In the future, it is necessary to move beyond the infinitely thin core approximation and consider the case of comparable ξ and λ, more typical of the interior. Also, the formalism needs to be extended to the case of superfluid neutrons and include the contribution of collective excitations.

Impact

The new force will affect cooling models of neutron stars, interpretation of pulsar glitches, and magnetic flux transport in the core.

Next steps

Planned are numerical simulations of the core structure including non-local effects and solving the self-consistent problem for realistic equations of state.

Key open problems

The work directly addresses the problem of the origin of ultra-strong magnetic fields in magnetars and the anomalously rapid cooling of some neutron stars, deepening the microscopic understanding of dissipative processes in superconducting matter.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

The paper examines the force exerted on proton vortices in the superconducting core of a neutron star by normal neutrons. Using the Boltzmann–Landau kinetic equation and Fermi liquid theory, it is shown that neutrons produce a longitudinal force proportional to the transport cross section, while the transverse (Magnus) component is strictly zero. Estimates of the ratio of this force to the electronic one are obtained, which can reach 0.01–0.1 under typical conditions.

Where its strength is

The strength of the work lies in the microscopic derivation of a new contribution to vortex dynamics that was previously neglected, and in demonstrating that the velocity difference between electrons and neutrons can be maintained without external forces. This provides a concrete mechanism for revising the evolution of magnetic fields and the dissipation of oscillations in neutron stars.

Where it could go next

Worth trying

  • Test whether the presence of the neutron force alters the characteristic damping times of r-modes as a function of core temperature.
  • Estimate the contribution of the new force to the magnetic field evolution of magnetars, using data on the thermal history from the work on heavy nuclei in the magnetar's fire.

Why this may matter

Refining the forces on vortices is important for understanding the observational manifestations of neutron stars, from glitches to thermal evolution. If the neutron force is significant at moderate temperatures, it could change predictions for a whole class of objects.

If you could hold a sugar-cube-sized piece of neutron star material, it would weigh as much as Mount Everest: that's how dense it is. And the superconducting vortices inside carry magnetic fields billions of times stronger than any Earth-made magnet.

\varepsilon_p = \frac{p Q}{m} + \sqrt{(\epsilon_p - E_F)^2 + \Delta^2}
quasiparticle energy including condensate momentum and superconducting gap
\mathbf{F}_{m\to v} = D'_e [\hat{z} \times (\mathbf{V}_e - \mathbf{V}_L)] - D_e \hat{z} \times [\hat{z} \times (\mathbf{V}_e - \mathbf{V}_L)] - D_n \hat{z} \times [\hat{z} \times (\mathbf{V}_n - \mathbf{V}_L)]
sum of contributions from electrons (transverse and longitudinal) and neutrons (longitudinal only)
D_n = (m_p\kappa)^2 \frac{3\pi}{8} \frac{n_{n0}}{p_{Fn}} L_n^{-1}
depends on the circulation quantum, neutron density, and transport cross-section

Key numbers

  • superconducting condensate circulation κ: ≈ 2×10-4 cm²/s
  • ratio of London depth to coherence length λ/ξ: 30–50
  • neutron density in the core: ~1038 cm⁻³
  • proton superconducting transition temperature: several ×109 K
  • relative force magnitude D_n/D_e: 0.01–0.1
Scientists
Paul DiracEnrico FermiSubrahmanyan ChandrasekharHendrik LorentzIsidor Isaac RabiAlbert Einstein
Concepts
neutron neutron star superfluidity nuclear force particle interaction strong interaction electron neutrino weak force superfluid vortex nuclear matter magnetic vortex electron liquid proton structure fermi liquid proton dynamics antiproton nucleon quark core hyperon crust baryon