Vector Perturbations in Ghost-Free Quasidilaton Massive Gravity

arXiv:2608.13529 · gr-qc, astro-ph.CO, hep-th · Submitted 2026-08-13 · Read on arXiv

Ekapob Kulchoakrungsun, Daris Samart

Khon Kaen University

gr-qc, astro-ph.CO, hep-th

Submitted: 2026-08-13

Updated: 2026-08-14

Comments: 9 pages. Mathematica notebook supplement is enclosed in the source file

License: http://creativecommons.org/licenses/by/4.0/

Importance score: 75/100

The gist: We study transverse vector perturbations in ghost-free extended quasidilaton massive gravity without a quasidilaton kinetic term, in the presence of minimal matter.

Terminology

Summary

We study transverse vector perturbations in ghost-free extended quasidilaton massive gravity without a quasidilaton kinetic term, in the presence of minimal matter. In vacuum, we recover the known result that the kinetic coefficient KV of the gravitational vector modes vanishes on the self-accelerating branch J = 0, so those modes are infinitely strongly coupled at linear order. We then add a canonical scalar field and a single Abelian vector (Maxwell or Proca). After integrating out the auxiliary shift, we find the same KV as in vacuum. The scalar matter has no transverse perturbation; it enters the unsimplified shift constraint, but those terms cancel once the Friedmann equation is used. A Maxwell or Proca field with vanishing isotropic background does not mix with the gravitational vectors at quadratic order. Minimal matter therefore leaves KV = 0 on Branch II. We do not claim that the modes are absent from the nonlinear theory. We do conclude that ordinary minimal matter is not enough to make the vector sector perturbatively healthy on this branch. If we need healthy gravitational vector modes at the linear level, Branch I is the branch to use.

Improvements for AI systems

Improvements to AI Systems Based on This Paper:

  1. Causal Inference for Constraint-Solving in Field Theories
  • Improvement: Train an AI to automatically detect when auxiliary fields (like the shift vector) can be integrated out, and to track whether their elimination introduces spurious terms that cancel via background equations (e.g., Friedmann equation).

  • Capability: The AI can systematically simplify complex gravitational actions, avoiding redundant calculations and identifying hidden cancellations—reducing errors in modified gravity research.

  1. Automated Stability Analysis of Perturbation Sectors
  • Improvement: Build a model that classifies kinetic coefficients (e.g., K V) across branches (Branch I vs. II) and matter content (scalar, vector, Proca) to predict strong-coupling or ghost instabilities without manual derivation.

  • Capability: The AI can rapidly scan parameter spaces of massive gravity theories, flagging branches where linear perturbations are unhealthy, and recommending viable alternatives (e.g., Branch I) for cosmological model building.

  1. Matter-Coupling Impact Predictor
  • Improvement: Develop a transformer that learns which matter fields (minimal vs. non-minimal, canonical vs. Proca) can or cannot resolve kinetic-term vanishing, based on symmetry and background isotropy.

  • Capability: The AI can pre-screen proposed matter couplings in modified gravity, saving researchers from pursuing models where vector modes remain strongly coupled—accelerating theory selection.

  1. Cross-Branch Consistency Checker
  • Improvement: Implement a logical verifier that ensures conclusions drawn from one branch (e.g., K V=0 on Branch II) are not overgeneralized to nonlinear regimes, and that flags when a claim is only linear-order valid.

  • Capability: The AI can generate precise, caveat-aware summaries for papers, preventing misinterpretation of perturbative results in nonperturbative contexts.

  1. Automated Literature-to-Constraint Mapping
  • Improvement: Use the paper’s result (minimal matter cannot fix vector strong coupling) to train a retrieval-augmented system that maps similar findings across massive gravity papers into a structured knowledge graph of branch-specific health conditions.

  • Capability: The AI can answer queries like Which matter fields make Branch II vector modes healthy? with evidence-based, branch-specific answers, and suggest unexplored non-minimal couplings.

  1. Symbolic Regression for Effective Actions
  • Improvement: Apply symbolic regression to the paper’s derived quadratic actions to learn general patterns of when matter terms decouple from gravitational perturbations (e.g., isotropic background condition).

  • Capability: The AI can propose new matter-gravity interaction terms that might cure strong coupling, generating testable hypotheses for future work.

What the Improved AI System Can Do Specifically:

  • Given a massive gravity action, it can automatically compute the vector kinetic coefficient for any matter content and branch, and output a health verdict (healthy/strongly coupled/ghost) with the exact cancellation steps.

  • It can generate a decision tree: If you need healthy linear vector modes, use Branch I; if Branch II is required, avoid minimal matter and consider non-minimal couplings (e.g., derivative interactions).

  • It can write a referee-style report on a new paper, checking whether the authors correctly handled auxiliary field elimination and branch-specific claims.

Abstract

We study transverse vector perturbations in ghost-free extended quasidilaton massive gravity without a quasidilaton kinetic term, in the presence of minimal matter. In vacuum, we recover the known result that the kinetic coefficient K V of the gravitational vector modes vanishes on the self-accelerating branch J=0, so those modes are infinitely strongly coupled at linear order. We then add a canonical scalar field and a single Abelian vector (Maxwell or Proca). After integrating out the auxiliary shift, we find the same K V as in vacuum. The scalar matter has no transverse perturbation; it enters the unsimplified shift constraint, but those terms cancel once the Friedmann equation is used. A Maxwell or Proca field with vanishing isotropic background does not mix with the gravitational vectors at quadratic order. Minimal matter therefore leaves K V=0 on Branch II. We do not claim that the modes are absent from the nonlinear theory. We do conclude that ordinary minimal matter is not enough to make the vector sector perturbatively healthy on this branch. If we need healthy gravitational vector modes at the linear level, Branch I is the branch to use.

Sources

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