A First-Principles Derivation of Newton's Gravitational Constant from an Eleven-Dimensional Covariant Master Action

Newton's gravitational constant relates conserved stress to spacetime curvature, but its magnitude is not selected by classical general relativity. We derive the native gravitational response on a regular branch of an eleven-dimensional covariant master action. On the information–projection domain, the seven action terms are combined before their shared auxiliary variables are eliminated. The reduced spin-2 response is then normalized by a conserved unit stress source. The result is \[2A_{\star}G_{\mu\nu}^{(1)}=T_{\mu\nu}^{\mathrm{phys}},\qquadC_u=\frac{1}{16\pi A_{\star}}=0.0497534\ldots .\] No observed Newton constant, measured particle mass, or reference-clock frequency selects this native coefficient. The normalized response is preserved through the four-dimensional readout hierarchy. The electron, muon, tau, up and down quarks, proton, and neutron return the same tensor coefficient at linear Einstein/stress order on the stated branch; additional scalar forces remain distinct observables. With the physical-time and action sections, the native response defines one dimensional Newton quantity, \[\boldsymbol{G}=C_u\frac{c^5\boldsymbol{t}_0^{\,2}}{\boldsymbol{\mathfrak{a}}_{\star}}=C_{\phi}\frac{c^5\boldsymbol{\tau}_G^{\,2}}{\boldsymbol{\mathfrak{a}}_{\star}},\qquad\boldsymbol{\tau}_G=\bar{\tau}\,\boldsymbol{t}_0,\qquadC_{\phi}=\frac{C_u}{\bar{\tau}^{\,2}}.\] Its weak-field restriction gives the Newton–Einstein response. On the declared leading atomic-current branch, a sixteen-dimensional caesium hyperfine operator fixes the dimensionless ratio \(r_{\mathrm{Cs}/e}=\omega_{\mathrm{Cs}}/\omega_e\). The atomic factor-through theorem places every remaining absolute component of this atomic-to-SI map on one electron–gravity frequency ratio: \[\chi_{eG}=\frac{\omega_e}{\Omega_G}>0,\qquadB_G^{(\mathrm{Cs})}=r_{\mathrm{Cs}/e}\chi_{eG},\qquadG_{N,\mathrm{atomic}}^{[\mathrm{SI}]}=K_{eG}\chi_{eG}^{\,2}.\] Here \(K_{eG}\) is the specified forward coefficient; \(\chi_{eG}\) remains uncomputed. The atomic route is therefore a one-scalar family, not an independent numerical SI prediction. The declared canonical local chart closes at \(6.67430\times10^{-11}\,\mathrm{m^3\,kg^{-1}\,s^{-2}}\), whereas the specified Friedmann input set gives \(6.72048\times10^{-11}\,\mathrm{m^3\,kg^{-1}\,s^{-2}}\) as a branch-conditioned cosmological consistency test. These are not averaged. An admissible bound-system selector removes the leading Friedmann update, while residual exchange must satisfy the same covariant conservation law. Newton's coupling is thus the dimensional realization of a conserved-stress-normalized geometric inverse stiffness.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-05
DOI
https://doi.org/10.5281/zenodo.23157148
Primary Topic
Relativity and Gravitational Theory
Type
preprint
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preprint

A First-Principles Derivation of Newton's Gravitational Constant from an Eleven-Dimensional Covariant Master Action

Dohyeong Lee
Zenodo (CERN European Organization for Nuclear Research)
Relativity and Gravitational Theory
preprint

A First-Principles Derivation of Newton's Gravitational Constant from an Eleven-Dimensional Covariant Master Action

Dohyeong Lee
preprint en

Abstract

Newton's gravitational constant relates conserved stress to spacetime curvature, but its magnitude is not selected by classical general relativity. We derive the native gravitational response on a regular branch of an eleven-dimensional covariant master action. On the information–projection domain, the seven action terms are combined before their shared auxiliary variables are eliminated. The reduced spin-2 response is then normalized by a conserved unit stress source. The result is \[2A_{\star}G_{\mu\nu}^{(1)}=T_{\mu\nu}^{\mathrm{phys}},\qquadC_u=\frac{1}{16\pi A_{\star}}=0.0497534\ldots .\] No observed Newton constant, measured particle mass, or reference-clock frequency selects this native coefficient. The normalized response is preserved through the four-dimensional readout hierarchy. The electron, muon, tau, up and down quarks, proton, and neutron return the same tensor coefficient at linear Einstein/stress order on the stated branch; additional scalar forces remain distinct observables. With the physical-time and action sections, the native response defines one dimensional Newton quantity, \[\boldsymbol{G}=C_u\frac{c^5\boldsymbol{t}_0^{\,2}}{\boldsymbol{\mathfrak{a}}_{\star}}=C_{\phi}\frac{c^5\boldsymbol{\tau}_G^{\,2}}{\boldsymbol{\mathfrak{a}}_{\star}},\qquad\boldsymbol{\tau}_G=\bar{\tau}\,\boldsymbol{t}_0,\qquadC_{\phi}=\frac{C_u}{\bar{\tau}^{\,2}}.\] Its weak-field restriction gives the Newton–Einstein response. On the declared leading atomic-current branch, a sixteen-dimensional caesium hyperfine operator fixes the dimensionless ratio \(r_{\mathrm{Cs}/e}=\omega_{\mathrm{Cs}}/\omega_e\). The atomic factor-through theorem places every remaining absolute component of this atomic-to-SI map on one electron–gravity frequency ratio: \[\chi_{eG}=\frac{\omega_e}{\Omega_G}>0,\qquadB_G^{(\mathrm{Cs})}=r_{\mathrm{Cs}/e}\chi_{eG},\qquadG_{N,\mathrm{atomic}}^{[\mathrm{SI}]}=K_{eG}\chi_{eG}^{\,2}.\] Here \(K_{eG}\) is the specified forward coefficient; \(\chi_{eG}\) remains uncomputed. The atomic route is therefore a one-scalar family, not an independent numerical SI prediction. The declared canonical local chart closes at \(6.67430\times10^{-11}\,\mathrm{m^3\,kg^{-1}\,s^{-2}}\), whereas the specified Friedmann input set gives \(6.72048\times10^{-11}\,\mathrm{m^3\,kg^{-1}\,s^{-2}}\) as a branch-conditioned cosmological consistency test. These are not averaged. An admissible bound-system selector removes the leading Friedmann update, while residual exchange must satisfy the same covariant conservation law. Newton's coupling is thus the dimensional realization of a conserved-stress-normalized geometric inverse stiffness.

Zenodo (CERN European Organization for Nuclear Research)
Relativity and Gravitational Theory
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