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From Decoherence to Coherent Intelligence: A Hypothesis on the Emergence of AI Structure Through Recursive Reasoning
Jordan Barton
Posted: 23 April 2025
Deriving the Pontecorvo–Maki–Nakagawa–Sakata Matrix from Koide’s Mass Formula and Brannen’s Neutrino Mass Hypothesis: Resolving the Mystery of the θ13 Rotation
Stafy Nem
Posted: 16 April 2025
Mass Law of Leptons and Quarks based on Hypercomplex Algebra: Topological Scaling and Generation Geometry
Jau Tang,
Qiang Tang
Posted: 11 April 2025
Photon-Field Interactions: A Relativistic and Quantum Approach
M. M. Shamshiri
Posted: 31 March 2025
Origin of the Gravitational Force
Shangqing Liu
Posted: 31 March 2025
Explanation of the Mass Pattern of the Low-Lying Scalar Nonet
Mihail Chizhov,
Emanuil Chizhov,
Momchil Naydenov,
Daniela Kirilova
Posted: 31 March 2025
The Hill-Wheeler Equation as a Quantum Mechanical Fermi Distribution: A New Statistical Framework for Elementary Particles
Hirokazu Maruyama
Posted: 26 March 2025
A New Paradigm for Single-Particle Double-Slit Interference: Cavity-Induced Nonlocal Quantized Momentum Transfer with no Need for Schrödinger’s Wavefunction, Self-Interference, and Wavefunction Collapse
Jau Tang
Posted: 24 March 2025
Possible Modification of Standard Model Classification of Particles and Fields
Henryk Wojciechowski
Posted: 20 March 2025
Finite Algebraic Quantum Field Theory
Abdulaziz D. Alhaidari
Posted: 20 March 2025
Description of the Electron in the Electromagnetic Field: The Dirac Type Equation and the Equation for the Wave Function in Spinor Coordinate Space
Pavel Gorev
Posted: 13 March 2025
Symmetry Extensions in High-Energy Physics via Fermion–Boson Duality and Extended Gamma Matrices: A Unified Perspective on Gauge Invariance, Quantum Gravity, and Anomalous Magnetic Moments
Hirokazu Maruyama
Posted: 10 March 2025
On a Conjecture on the Cosmological Origin of Quarks and Leptons By Spontaneous Fractionation of a Pair of Heavy Leptons
Massimo Auci
Posted: 03 March 2025
Negative Energy Density: Pulsars and Kerr Rotating Black Holes
Matthew Loccisano
This paper will explain how negative energy density, the same kind of negative energy density that is used in theoretical frameworks that explain wormholes, interact with rotating black holes in spacetime. Wormholes are particularly significant since they can be a route for time travel. As sci-fi as it seems, it is indeed a possibility, thanks to Kerr rotating black holes. Penrose process is key in understanding how negative energy density comes into play, and ergospheres in rotating black holes are also crucial. NASA data and Chandra telescope data were extracted to look at particle anomalies, which strongly suggest energy leakage and exotic matter. EHT (Event Horizon Telescope) data was also extracted, which solidifies the negative energy density argument. I will explain how this occurs using past theoretical models and real-world scientific observations. Jets, cone particles formed by hardons and other quark particles, leave the rotational black hole, from which it is produced, to create a forward force in space. Particles split, and the weaker one goes into the rotational black hole becoming negative, and the other one extracts energy from the black hole, making it exotic. These factors contribute to negative density since negative density fills the void left by the jets once they are carried away.
This paper will explain how negative energy density, the same kind of negative energy density that is used in theoretical frameworks that explain wormholes, interact with rotating black holes in spacetime. Wormholes are particularly significant since they can be a route for time travel. As sci-fi as it seems, it is indeed a possibility, thanks to Kerr rotating black holes. Penrose process is key in understanding how negative energy density comes into play, and ergospheres in rotating black holes are also crucial. NASA data and Chandra telescope data were extracted to look at particle anomalies, which strongly suggest energy leakage and exotic matter. EHT (Event Horizon Telescope) data was also extracted, which solidifies the negative energy density argument. I will explain how this occurs using past theoretical models and real-world scientific observations. Jets, cone particles formed by hardons and other quark particles, leave the rotational black hole, from which it is produced, to create a forward force in space. Particles split, and the weaker one goes into the rotational black hole becoming negative, and the other one extracts energy from the black hole, making it exotic. These factors contribute to negative density since negative density fills the void left by the jets once they are carried away.
Posted: 03 March 2025
On a Higgs-Mediated Relation Between Elementary Particles and Spacetime and Its Physical Consequences
Ignazio Licata,
Leonardo Chiatti
Posted: 17 February 2025
Starobinsky Inflation with T-Model Kähler Geometries
Constantinos Pallis
We present novel implementations of Starobisky-like inflation within Supergravity adopting Kahler potentials for the inflaton which parameterize hyperbolic geometries known from the T-model inflation. The associated superpotentials are consistent with an R and a global or gauge U(1)X symmetries. The inflaton is represented by a gauge singlet or non-singlet superfield and is accompanied by a gauge-singlet superfield successfully stabilized thanks to its compact contribution into the total Kahler potential. Keeping the Kahler manifold intact, a conveniently violated shift symmetry is introduced which allows for a slight variation of the predictions of Starobinsky inflation: The (scalar) spectral index exhibits an upper bound which lies close to its central observational value whereas the constant scalar curvature of the inflaton-sector Kahler manifold increases with the tensor-to-scalar ratio.
We present novel implementations of Starobisky-like inflation within Supergravity adopting Kahler potentials for the inflaton which parameterize hyperbolic geometries known from the T-model inflation. The associated superpotentials are consistent with an R and a global or gauge U(1)X symmetries. The inflaton is represented by a gauge singlet or non-singlet superfield and is accompanied by a gauge-singlet superfield successfully stabilized thanks to its compact contribution into the total Kahler potential. Keeping the Kahler manifold intact, a conveniently violated shift symmetry is introduced which allows for a slight variation of the predictions of Starobinsky inflation: The (scalar) spectral index exhibits an upper bound which lies close to its central observational value whereas the constant scalar curvature of the inflaton-sector Kahler manifold increases with the tensor-to-scalar ratio.
Posted: 06 February 2025
Quarks and Leptons Formation from the Spontaneous Fractionation of a Pair of Elementary Particles with Proton Charge Units
Massimo Auci
Posted: 03 February 2025
Higgs Physics at Muon Collider
Luca Castelli
Posted: 21 January 2025
Energy Renormalization in a Berry Geometrical Phase: Low-Energy Perturbations of the Strong Interaction and the QCD Mass Gap
Mark Gibbons
A Berry geometrical phase is identified in a strongly metastable system containing dynamically responsive nanoscale clathrate hydrate structures within a crystal-fluid material. High energy degeneracy in the associated chemistry produces local stability and false vacuum conditions that lead to non-extensive and non-additive contributions in the fundamental thermodynamic relation. Application of Ginzburg-Landau theory and the scaling laws reveals a coherence length (3.05 m) and a penetration depth (2.2 m) that characterize a macro-scale dual superconductor. The coherence length describes a magnetic condensate whilst its inverse gives the Higgs mass (0.33 kg) and non-extensive volume changes (± 0.5 l). The penetration depth determines the extent of QCD vacuum suppression whilst its inverse gives an effective vector boson mass (≤ 0.46 kg), resulting in non-additive hyperbolic curvature. Simultaneous emergence of the Ginzburg-Landau superconducting phase transition is consistent with gauge-invariant coupling of the scalar field (≤ 3.6 ks-1) to the Yang-Mills action in QCD. The discovery of an energy gap in the gradient energy term of the system Lagrangian is associated with a critical correlation length (3.05 m) revealed in the transition from a gapped to a gapless superconducting state. Together with the emergence and reabsorption of the Higgs-like scalar field, a mechanism for describing a renormalized QCD mass gap arises. The phenomena reported are only relevant to a coordinated U(2) Lie symmetry group having scale-invariance across micro- and macro-scale QCD dual superconductivity. Under normal, non-critical conditions the symmetry is broken and separated into SU(2) Abelian condensed matter and SU(3) non-Abelian QCD elements that are effectively isolated. Energy and momentum cannot be transferred across the QCD mass gap and TeV confinement energies dominate as conservation of energy and momentum are confined to each individual symmetry group. It is proposed that where these symmetries are decomposed and synchronized then the QCD mass gap with associated TeV threshold dissipates.
A Berry geometrical phase is identified in a strongly metastable system containing dynamically responsive nanoscale clathrate hydrate structures within a crystal-fluid material. High energy degeneracy in the associated chemistry produces local stability and false vacuum conditions that lead to non-extensive and non-additive contributions in the fundamental thermodynamic relation. Application of Ginzburg-Landau theory and the scaling laws reveals a coherence length (3.05 m) and a penetration depth (2.2 m) that characterize a macro-scale dual superconductor. The coherence length describes a magnetic condensate whilst its inverse gives the Higgs mass (0.33 kg) and non-extensive volume changes (± 0.5 l). The penetration depth determines the extent of QCD vacuum suppression whilst its inverse gives an effective vector boson mass (≤ 0.46 kg), resulting in non-additive hyperbolic curvature. Simultaneous emergence of the Ginzburg-Landau superconducting phase transition is consistent with gauge-invariant coupling of the scalar field (≤ 3.6 ks-1) to the Yang-Mills action in QCD. The discovery of an energy gap in the gradient energy term of the system Lagrangian is associated with a critical correlation length (3.05 m) revealed in the transition from a gapped to a gapless superconducting state. Together with the emergence and reabsorption of the Higgs-like scalar field, a mechanism for describing a renormalized QCD mass gap arises. The phenomena reported are only relevant to a coordinated U(2) Lie symmetry group having scale-invariance across micro- and macro-scale QCD dual superconductivity. Under normal, non-critical conditions the symmetry is broken and separated into SU(2) Abelian condensed matter and SU(3) non-Abelian QCD elements that are effectively isolated. Energy and momentum cannot be transferred across the QCD mass gap and TeV confinement energies dominate as conservation of energy and momentum are confined to each individual symmetry group. It is proposed that where these symmetries are decomposed and synchronized then the QCD mass gap with associated TeV threshold dissipates.
Posted: 20 January 2025
The Great Tao Model: The Theory of Elementary Particles and Their Interactions
Jiqing Zeng,
Tianhe Zeng
Posted: 14 January 2025
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