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Fracture Network Mathematics
Daniel S. Brox
Posted: 20 January 2026
The Riemann-Moebius-Enneper Structure: A Geometric Framework for Fundamental Constants
Felipe Oliveira Souto
Posted: 20 January 2026
Dynamic Phase-Transition Cosmological Model Based on Path-Integral Definition of Xuan-Liang: Complete Theory and Observational Tests
Jianchao Hou
Posted: 20 January 2026
Mass Model and Calculation Methods for Charged Leptons
Tongsheng Xia
Posted: 16 January 2026
Quantum Information Copy-Time as a Microscopic Principle for Emergent Hydrodynamics, Inertial Spectral Mass, and a Predictive Higgs-Portal Dark-Matter Corridor
Sacha Mohamed
Posted: 14 January 2026
Stability of Self-Gravitating Bosonic Configurations
Gilbert Reinishc
,José Antonio de Freitas Pacheco
Posted: 13 January 2026
Discrete Vacuum Geometry Predicts the Hierarchical Mass Spectrum of Standard Model Fermions
Yuxuan Zhang
,Weitong Hu
,Wei Zhang
Posted: 13 January 2026
The Primal Energy Scale: Derivation and Physical Significance of E0 and ℓ0 from Riemann Zeta Zeros
Felipe Oliveira Souto
Posted: 12 January 2026
Self-Variation Dynamics and Particle Masses from First Principles
Emmanuil Manousos
Posted: 12 January 2026
A Mechanical Formulation for Resistive Network Analysis: The Spring-Conductance Matrix Method
Faiçal Barzi
,Kaoutar Fethi
Posted: 08 January 2026
Inverting the Dimensional Hierarchy: Advocating for a 4D-Native Framework for Quantum Geometry
Faical Barzi
Posted: 06 January 2026
Conformally Compactified Minkowski Space: A Re-Examination with Emphasis on the Double Cover and Conformal Infinity
Arkadiusz Jadczyk
This paper presents a detailed re-examination of the conformal compactification of Minkowski space, \( \overline{M} \), constructed as the projective null cone of the six-dimensional space \( \mathbb{R}^{4,2} \). We provide an explicit and basis-independent formulation, emphasizing geometric clarity. A central result is the explicit identification of \( \overline{M} \) with the unitary group U(2) via a diffeomorphism, offering a clear matrix representation for points in the compactified space. We then systematically construct and analyze the action of the full conformal group \( \mathrm{O}(4,2) \) and its connected component \( \mathrm{SO}_0(4,2) \) on this manifold. A key contribution is the detailed study of the double cover, \( \overline{\overline{M}} \), which is shown to be diffeomorphic to \( S^3 \times S^1 \). This construction resolves the non-effectiveness of the \( \mathrm{SO}(4,2) \) action on \( \overline{M} \), yielding an effective group action on the covering space. A significant portion of our analysis is devoted to a precise and novel geometric characterization of the conformal infinity. Moving beyond the often-misrepresented ``double cone'' description, we demonstrate that the infinity of the double cover, \( \overline{\overline{M}}_\infty \), is a squeezed torus (specifically, a horn cyclide), while the simple infinity, \( \overline{M}_\infty \), is a needle cyclide. We provide explicit parametrizations and graphical representations of these structures. Finally, we explore the embedding of five-dimensional constant-curvature spaces, whose boundary is the compactified Minkowski space, and discuss the interpretation of geodesics within these domains. The paper aims to clarify long-standing misconceptions in the literature and provides a robust, coordinate-free geometric foundation for conformal compactification, with potential implications for cosmology and conformal field theory.
This paper presents a detailed re-examination of the conformal compactification of Minkowski space, \( \overline{M} \), constructed as the projective null cone of the six-dimensional space \( \mathbb{R}^{4,2} \). We provide an explicit and basis-independent formulation, emphasizing geometric clarity. A central result is the explicit identification of \( \overline{M} \) with the unitary group U(2) via a diffeomorphism, offering a clear matrix representation for points in the compactified space. We then systematically construct and analyze the action of the full conformal group \( \mathrm{O}(4,2) \) and its connected component \( \mathrm{SO}_0(4,2) \) on this manifold. A key contribution is the detailed study of the double cover, \( \overline{\overline{M}} \), which is shown to be diffeomorphic to \( S^3 \times S^1 \). This construction resolves the non-effectiveness of the \( \mathrm{SO}(4,2) \) action on \( \overline{M} \), yielding an effective group action on the covering space. A significant portion of our analysis is devoted to a precise and novel geometric characterization of the conformal infinity. Moving beyond the often-misrepresented ``double cone'' description, we demonstrate that the infinity of the double cover, \( \overline{\overline{M}}_\infty \), is a squeezed torus (specifically, a horn cyclide), while the simple infinity, \( \overline{M}_\infty \), is a needle cyclide. We provide explicit parametrizations and graphical representations of these structures. Finally, we explore the embedding of five-dimensional constant-curvature spaces, whose boundary is the compactified Minkowski space, and discuss the interpretation of geodesics within these domains. The paper aims to clarify long-standing misconceptions in the literature and provides a robust, coordinate-free geometric foundation for conformal compactification, with potential implications for cosmology and conformal field theory.
Posted: 01 January 2026
Assembly Theory - Formalizing Assembly Spaces, Discovering Patterns and Bounds
Wawrzyniec Bieniawski
,Andrzej Tomski
,Szymon Łukaszyk
,Piotr Masierak
,Szymon Tworz
Posted: 29 December 2025
The Kuznetsov Tensor as a Foundation of the Electric Double Layer Theory at the Metal–Electrolyte Interface
Vyacheslav Kuznetsov
This paper presents a generalized theoretical framework for describing the electric double layer (EDL) at the metal–electrolyte interface based on the introduction of the Kuznetsov tensor. In contrast to classical EDL models, which rely on a scalar electrostatic potential and assume integer ionic charges, the proposed approach accounts for the tensorial nature of interactions arising from specific ion adsorption and partial charge transfer between ions and the metal surface. The Kuznetsov tensor is formulated as a generalized interfacial field tensor that incorporates contributions from energy and momentum transport, charge density, adsorption effects, and entropy fluxes. It is shown that the equilibrium state of the electric double layer corresponds to the condition of vanishing divergence of the Kuznetsov tensor, allowing the EDL to be interpreted as a stationary tensor field rather than a simple superposition of compact and diffuse layers. Within this formalism, fractional effective ionic charges, ion competition in multicomponent electrolytes, and the influence of the chemical nature of the electrode surface are naturally captured. It is demonstrated that classical Poisson–Nernst–Planck equations and Stern-type models can be recovered as limiting cases of the tensor description under appropriate simplifying assumptions. The proposed theory provides a unified mathematical foundation for multiscale modeling of electrochemical interfaces and offers a consistent framework for analyzing charge storage, capacitance, and interfacial phenomena in batteries, supercapacitors, and electrocatalytic systems.
This paper presents a generalized theoretical framework for describing the electric double layer (EDL) at the metal–electrolyte interface based on the introduction of the Kuznetsov tensor. In contrast to classical EDL models, which rely on a scalar electrostatic potential and assume integer ionic charges, the proposed approach accounts for the tensorial nature of interactions arising from specific ion adsorption and partial charge transfer between ions and the metal surface. The Kuznetsov tensor is formulated as a generalized interfacial field tensor that incorporates contributions from energy and momentum transport, charge density, adsorption effects, and entropy fluxes. It is shown that the equilibrium state of the electric double layer corresponds to the condition of vanishing divergence of the Kuznetsov tensor, allowing the EDL to be interpreted as a stationary tensor field rather than a simple superposition of compact and diffuse layers. Within this formalism, fractional effective ionic charges, ion competition in multicomponent electrolytes, and the influence of the chemical nature of the electrode surface are naturally captured. It is demonstrated that classical Poisson–Nernst–Planck equations and Stern-type models can be recovered as limiting cases of the tensor description under appropriate simplifying assumptions. The proposed theory provides a unified mathematical foundation for multiscale modeling of electrochemical interfaces and offers a consistent framework for analyzing charge storage, capacitance, and interfacial phenomena in batteries, supercapacitors, and electrocatalytic systems.
Posted: 26 December 2025
Wigner Functions of Time-Dependent Cat-Like Even/Odd Superpositions of Nonlinear Coherent States
Miguel Citeli de Freitas
,Viktor V. Dodonov
Posted: 24 December 2025
Conjugation of Colored Compositions
Augustine O. Munagi
Posted: 23 December 2025
Improving Coating Stability Using Slip Conditions: A Maxwell Fluid Analysis via the Langlois Recursive Method
Laraib Mehboob
,Khadija Maqbool
,Abdul Majeed Siddiqui
,Zaheer Abbas
Posted: 23 December 2025
(p, q)-String Junctions as Interstitial Fields on a Modal Lightcone
Ryan Buchanan
Posted: 22 December 2025
The 168 Monads: Derivation of the Standard Model Particle Spectrum from Fano Plane Walk-States
Christian R. Macedonia
Posted: 22 December 2025
The Kuznetsov Tensor for Describing Differential Equations of Motion of Mechanical
Vyacheslav A. Kuznetsov
This paper presents a method for describing the differential equations of motion of mechanical systems using the Kuznetsov tensor. Traditional approaches to solving equations of motion rely on vector and matrix methods, but the proposed approach allows for significant simplification and generalization of problems by using a system state tensor. The paper discusses the main principles of working with the Kuznetsov tensor, which describes the evolution of the system in a unified context. Specifically, it outlines a method for integrating the equations of motion for various mechanical systems, such as oscillations in a two-mass spring system. Conditions for damping oscillations and controlling amplitude are also considered, expanding the applicability of the Kuznetsov tensor in engineering calculations. The advantages of the proposed approach include a more compact representation of the system of equations, ease of analyzing invariants and symmetries, and the ability to apply the method to multi-linked and multi-component systems. The use of the Kuznetsov tensor for modeling the dynamics of various systems represents a step toward a more universal approach in mechanics and engineering.
This paper presents a method for describing the differential equations of motion of mechanical systems using the Kuznetsov tensor. Traditional approaches to solving equations of motion rely on vector and matrix methods, but the proposed approach allows for significant simplification and generalization of problems by using a system state tensor. The paper discusses the main principles of working with the Kuznetsov tensor, which describes the evolution of the system in a unified context. Specifically, it outlines a method for integrating the equations of motion for various mechanical systems, such as oscillations in a two-mass spring system. Conditions for damping oscillations and controlling amplitude are also considered, expanding the applicability of the Kuznetsov tensor in engineering calculations. The advantages of the proposed approach include a more compact representation of the system of equations, ease of analyzing invariants and symmetries, and the ability to apply the method to multi-linked and multi-component systems. The use of the Kuznetsov tensor for modeling the dynamics of various systems represents a step toward a more universal approach in mechanics and engineering.
Posted: 19 December 2025
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