Preprint Article Version 4 Preserved in Portico This version is not peer-reviewed

General Quantum Gravity

Version 1 : Received: 15 June 2023 / Approved: 20 June 2023 / Online: 21 June 2023 (10:01:50 CEST)
Version 2 : Received: 3 October 2023 / Approved: 5 October 2023 / Online: 5 October 2023 (10:51:05 CEST)
Version 3 : Received: 15 October 2023 / Approved: 16 October 2023 / Online: 17 October 2023 (08:00:13 CEST)
Version 4 : Received: 21 November 2023 / Approved: 21 November 2023 / Online: 22 November 2023 (12:12:12 CET)
Version 5 : Received: 25 December 2023 / Approved: 26 December 2023 / Online: 26 December 2023 (09:58:36 CET)

How to cite: Vadurie, S. General Quantum Gravity. Preprints 2023, 2023061472. https://doi.org/10.20944/preprints202306.1472.v4 Vadurie, S. General Quantum Gravity. Preprints 2023, 2023061472. https://doi.org/10.20944/preprints202306.1472.v4

Abstract

Quantum Gravity is not sufficient to predict the properties of particles (baryonic and non-baryonic) to a great extent. So, we develop General Quantum Gravity (GQG), which is a renormalizable formalization of quantized gravity that emerges from General Relativity through a new scenario of Quantum Mechanics. Inside every observable $(3+1)D$ spacetime in this new scenario of Quantum Mechanics, there must contain an internal hidden $(n+1)D$ spacetime, which immediately yields extra hidden dimensions by a closed continuous mapping, so that the overall spacetime must acquire Supersymmetry. We have also found that Superstrings are inevitably natural and universal but hidden inside every $(3+1)D$ observable spacetime. Superstrings are found eleven-dimensional (rather than lower dimensional) within this quantum spacetime. Consequently, eleven-dimensional Supergravity is necessarily a natural phenomenon within the GQG spacetime. GQG is formalized here in two different aspects. The first one gives an Einstein field equation in a semi-quantum Minkowski spacetime with semi-quantum Lorentzian metric tensor, whereas, the second one yields a purely Quantum Mechanical Einstein field equation in a quantum non-Minkowski spacetime with non-Lorentzian metric tensor. Dark Energy (as well as Dark Matter) appears from GQG quite naturally. We develop here Gravitational Electroweak Dark Energy interactions, where gravity and Dark Energy are allowed to combine with electroweak symmetry. Likewise, in Gravitational Chromodynamic Dark Energy interactions, we combine QCD with gravitational and Dark Energy symmetries. In a Dark Matter gauge symmetry model, we combine Dark matter with all possible gauge symmetries. A Universal Model $SU(7)_{UM}$ combines entire baryonic and non-baryonic particle interactions all together.

Keywords

Quantum Gravity; M-theory; Dark Energy; Dark Matter

Subject

Physical Sciences, Particle and Field Physics

Comments (1)

Comment 1
Received: 22 November 2023
Commenter: Shashwata Vadurie
Commenter's Conflict of Interests: Author
Comment: The paper is thoroughly revised, rearranged, rewritten and expanded. Some errors are removed.
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