Scalar baryons in neutron stars

arXiv:2608.10141 · hep-ph, astro-ph.CO · Submitted 2026-08-10 · Read on arXiv

Julian Heeck, Yu Zhi

University of Virginia

hep-ph, astro-ph.CO

Submitted: 2026-08-10

Updated: 2026-08-12

License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/

Importance score: 75/100

The gist: Neutron stars have baryon chemical potentials that can exceed the neutron mass, providing favorable conditions to convert neutrons to new particles carrying baryon number, even if those processes are

Terminology

Summary

Neutron stars have baryon chemical potentials that can exceed the neutron mass, providing favorable conditions to convert neutrons to new particles carrying baryon number, even if those processes are kinematically forbidden in vacuum. We study the effect of GeV-scale scalars with baryon number on neutron stars’ equation of state and show that non-perturbatively large repulsive self-couplings are required to support the observed two-solar-mass neutron stars. We also study potentials with attractive self-interactions, which can trigger scalar production even for masses above the chemical potential and resemble Coleman’s Q-matter.

Improvements for AI systems

Improvements to AI Systems:

  1. Physics-Constrained Equation-of-State (EoS) Emulator
  • Improvement: Train a neural network to map scalar field parameters (mass, self-coupling strength, sign of interaction) directly to the resulting neutron star mass–radius relation, using the paper’s formalism.

  • Capability: The AI can instantly predict whether a given baryon-number scalar model supports a 2-solar-mass neutron star, without solving the full Tolman-Oppenheimer-Volkoff equations each time.

  1. Automatic Detection of Q-Matter Phase Transitions
  • Improvement: Implement a classifier that identifies parameter regimes where attractive self-interactions lead to scalar condensation (Coleman’s Q-matter) inside neutron stars, based on the chemical potential threshold and scalar mass.

  • Capability: The AI can flag candidate models for exotic compact objects, enabling rapid screening of dark matter or new physics scenarios.

  1. Self-Coupling Constraint Optimizer
  • Improvement: Use a Bayesian optimizer to find the minimal repulsive self-coupling required to sustain a given neutron star mass, given the scalar’s mass and baryon number.

  • Capability: The AI can produce exclusion plots for scalar models, directly comparing against observational constraints from pulsar timing (e.g., J0740+6620).

  1. Multi-Messenger Consistency Checker
  • Improvement: Integrate the paper’s EoS modifications into a generative model that synthesizes gravitational wave (GW170817) and X-ray (NICER) data, then tests whether the scalar-induced EoS remains consistent with both.

  • Capability: The AI can automatically reject scalar models that fit one observation but violate another, providing a robust pipeline for new physics validation.

  1. Vacuum-to-Stellar Translation Module
  • Improvement: Build a transformer that takes vacuum scattering data (e.g., neutron–neutron cross sections) and predicts the in-medium scalar production rate at high baryon chemical potential, using the paper’s kinematic relaxation insight.

  • Capability: The AI can estimate observable signatures (e.g., cooling anomalies or mass loss) from laboratory-constrained parameters, bridging particle physics and astrophysics.

What the Improved AI System Can Do:

  • Given a new scalar model, instantly output its viability for neutron star observations, including mass–radius curves, tidal deformability, and cooling curves.

  • Automatically scan a multi-dimensional parameter space (mass, coupling, self-interaction) and produce a survival map against all current neutron star data.

  • Generate synthetic training data for future detectors by simulating thousands of scalar-modified EoS, then use that to infer model parameters from a single observed neutron star.

  • Provide a real-time decision tool for theorists: If you choose this scalar mass, the required repulsive coupling exceeds perturbative limits—consider attractive interactions instead.

Sources

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