A dynamical approach to General Relativity based on proper time
Jaume de Haro

TL;DR
This paper presents a dynamical interpretation of proper time as fundamental to gravity, deriving the weak-field limit of Einstein's equations from variational principles and invariance, emphasizing energy conservation and self-consistency.
Contribution
It introduces a novel dynamical approach to General Relativity based on proper time, deriving Einstein's equations from variational principles rather than geometric postulates.
Findings
Derives the weak-field limit of GR from proper time extremization.
Shows Einstein's equations emerge from energy conservation and self-consistency.
Links linearized gravity to the non-linear structure involving Ricci tensor.
Abstract
This work places the invariant at the center of the gravitational interaction, interpreting it not as a purely geometric object but as the differential of proper time, endowed with direct physical meaning. Starting from the extension of Fermat's principle to massive particles--namely, the requirement that freely falling bodies follow trajectories that extremize proper time, which for timelike motion corresponds to a local maximum--and invoking the universality of Galilean free fall, we derive the form of in a static gravitational field. Lorentz invariance then provides the natural framework to extend this result to systems involving moving matter. The invariant derived through this procedure matches the weak-field limit of General Relativity formulated in the harmonic gauge. Within this linearized regime, we show that the structure of the theory already contains the…
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Taxonomy
TopicsRelativity and Gravitational Theory · Noncommutative and Quantum Gravity Theories · Quantum and Classical Electrodynamics
