Submitted:
13 August 2026
Posted:
14 August 2026
Read the latest preprint version here
Abstract
We present a rigorous mathematical proof that the spacetime metric \(g_{\mu\nu}\) of General Relativity and the fundamental kinetic field \(\nu^\mu\) of the Fundamental Speed Theory (FST) are not two distinct entities, but rather two mathematically equivalent descriptions of the same underlying physical reality. Starting from the foundational FST paper---validated on 171 SPARC galaxies with \(\chi^2_\nu = 0.170\) across five hierarchical validation levels---we establish six central theorems: 1. The Metric--Kinetic Map (Theorem 1): The spacetime metric \(g_{\mu\nu}\) is uniquely determined by the kinetic field \(\tilde{\nu}\) and its gradients via an explicit, closed-form expression derived from the FST velocity relation (Eq.28 of the foundational paper). 2. The Einstein Correspondence (Theorem 2): The Einstein tensor \(G_{\mu\nu}\) computed from this metric satisfies \(G_{\mu\nu} = \frac{8\pi G}{c^4} T_{\mu\nu}^{(V)}\) exactly when \(\tilde{\nu}\) obeys the FST field equation, with \(T_{\mu\nu}^{(V)}\) given by Eq. (6) of the foundational paper. The proof establishes that this correspondence requires the fundamental relation \(\beta_{\text{eff}} = |\lambda|\nu_0^2/(6c_1)\), which is precisely Eq. (18) of the foundational paper. 3. The Invertibility Theorem (Theorem 3): The map from \(\tilde{\nu}\) to \(g_{\mu\nu}\) is bijective in the weak-field regime; no two distinct field configurations produce the same metric, and every weak-field spherically symmetric metric corresponds to a unique field configuration. 4. The Cosmological Extension (Theorem 4): For a homogeneous, time-dependent kinetic field, the same map generates the FLRW cosmological metric. The modified Friedmann equations emerge naturally, with the kinetic field providing both an effective dark energy density and a slowly evolving equation of state. 5. The Gravitational Wave Correspondence (Theorem 5): Linear perturbations of the kinetic field produce metric perturbations satisfying the wave equation \(\Box h_{\mu\nu}^{\text{TT}} = 0\). Gravitational waves are thus identified as propagating perturbations of the kinetic field. 6. The Gravitational Lensing Theorem (Theorem 6): Weak lensing masses equal FST dynamical masses without dark matter. For 19 SPARC galaxies with published weak lensing masses, the median lensing-to-dynamical mass ratio at 300 kpc is \(\mathbf{1.09}\) (all galaxies), while the median for the 15-galaxy reliable subset is \(\mathbf{0.88}\). This demonstrates that FST explains gravitational lensing without dark matter for the majority of well-measured galaxies. We further present the exact static spherical reduction of the coupled Einstein-FST system and prove a screened near--Schwarzschild limit showing that the kinetic-field stress is parametrically suppressed in the high-density phase, yielding an exterior metric that is a controlled perturbation of Schwarzschild in all Solar-System regimes. Complete dimensional analysis in SI units is given throughout, and the detailed component-level reductions (including the spherical reduction of \(T_{\mu\nu}^{(V)}\) from the master formula Eq. (10) are provided in the appendices. The results establish that spacetime is not a fundamental entity but the perceptual manifestation of the kinetic field.
Keywords:
fundamental speed theory
; emergent spacetime
; modified gravity
; vector-tensor theory
; canonical lift
; screening mechanism
; MONDModified gravity
; spacetime emergence
; galactic rotation curves
; gravitational lensing
; dark matter
; kinetic field
; Einstein equations
; cosmology
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