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2408.01260

Relativistic Effects in the Dynamics of a Particle in a Coulomb Field

Rafael Ortega, David Rojas

correcthigh confidence
Category
math.DS
Journal tier
Strong Field
Processed
Sep 28, 2025, 12:56 AM

Audit review

The paper proves that in special-relativistic central-force dynamics with real-analytic V and V′>0, no potential has the Bertrand property (periodicity of all trajectories near every circular orbit). This is stated as Theorem 2.1 and developed in Section 3 via a reduction to a relativistic oscillator for ρ=1/r and an isochrony argument that yields an overdetermined set of analytic constraints on V, culminating in a contradiction except for a degenerate case that still fails to give closed noncircular orbits . The candidate model arrives at the same conclusion by a different local argument: linearizing about a circular orbit to obtain the radial epicyclic frequency and then proving that the exact apsidal angle Δθ(E,ℓ) is strictly decreasing in the energy E near the circular energy (for fixed ℓ), which precludes periodicity for all nearby initial conditions. The two approaches agree on the main claim but use distinct techniques (period-function/isochrony vs. apsidal-angle monotonicity), so the appropriate verdict is that both are correct, with different proofs.

Referee report (LaTeX)

\textbf{Recommendation:} minor revisions

\textbf{Journal Tier:} strong field

\textbf{Justification:}

The paper answers a natural and important question about the relativistic analogue of Bertrand’s property by a careful reduction to a relativistic oscillator and an isochrony argument. The logic is coherent and the result is significant for the qualitative theory of relativistic central forces. Minor improvements in exposition would make the arguments even more accessible.