Covariant theory predicts dynamics and weak lensing effects in gravitational fields, suggesting new insights.
We present a covariant “inertia-first” response theory in which local inertia is controlled by a reservoir state variable photons and matter propagate on a single physical metric gμν=A^2(χ)\,gμν. In the weak-field limit this yields a Helmholtz–Poisson response equation for the scalar perturbation and a modified physical potential Φ=Φ_N+α_0φ. A key consequence of the minimal conformal class is the absence of gravitational slip at leading order, gₗₑₙₛ=gdyn, so weak-lensing directly constrains the same response that governs matter dynamics. We derive analytic spherical solutions, with a fully worked Hernquist example including closed expressions for the response function ν(r)=gₗₑₙₛ/g_N, and we provide a formally correct projection pipeline to the observable excess surface density ΔΣ(R). The framework replaces halo additivity by a nonlocal response structure in the effective lensing source and naturally accommodates outer relaxation to GR via coupling damping α(χbg)→ 0 and/or mass screening m_χ(χbg)↑. The Zenodo archive includes the manuscript, figure files, and a self-contained notebook that reproduces Figs. 1–4.
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Jan-Frederik Flügge (2026) studied this question.
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