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astro-ph.GA 2026-04-21 MDPI Entropy 9 theorems

Golden-ratio exponent fixes a gravity kernel

by Megan Simons, Elshad Allahyarov +1 more

A Discrete Informational Framework for Classical Gravity: Ledger Foundations and Galaxy Rotation Curve Constraints

A discrete ledger argument pins α≈0.191 with no free knobs; SPARC rotation curves give median χ²/N≈3.06.

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The weak-field, quasi-static regime of gravity is commonly described by the Newton–Poisson equation as an effective response law. We construct this response within a cost-first discrete variational framework. The Recognition Composition Law (RCL) uniquely selects a reciprocal closure cost within the restricted quadratic symmetric composition class; together with the discrete ledger axioms AX1–AX5 (including conservation) and standard DEC refinement, the Newton–Poisson baseline is then recovered in the instantaneous-closure limit. Conditional on Assumption AS1 (scale-free latency) and Assumption AS2 (causal frequency–wavenumber ansatz), allowing finite equilibration introduces fractional memory into the response, yielding a scale-free modification of the source–potential relation characterized by a power-law kernel w ker ( k ) = 1 + C ( k 0 / k ) α in Fourier space. The kernel exponent α = 1 2 ( 1 − φ − 1 ) ≈ 0.191 , where φ = ( 1 + 5 ) / 2 , is derived from self-similarity of the discrete ledger closure; the amplitude C = φ − 2 ≈ 0.382 is identified as a hypothesis from a three-channel factorization argument. We evaluate this quasi-static kernel-motivated response against SPARC galaxy rotation curves under a strict global-only protocol (fixed M / L = 1 , no per-galaxy tuning, conservative σ tot ), using a controlled multiplicative surrogate for the full nonlocal disk operator implied by the kernel. In this deliberately over-constrained setting, the surrogate interface achieves median ( χ 2 / N ) = 3.06 over 147 galaxies (2933 points), outperforming a strict global-only NFW benchmark and remaining less efficient than MOND under identical constraints. The analysis is restricted to the non-relativistic, quasi-static sector and should be read as a falsifier-oriented galactic-regime consistency check of the scaling window, not as a relativistic completion or a claim of Solar System viability without additional UV regularization/screening.
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physics.gen-ph 2026-07-03

Niche construction unifies biosignatures with technosignatures

by Lukáš Likavčan

Substrate-Agnostic 3x: Biosignatures, Technosignatures, Ecologies

Substrate-agnostic ecologies remove terrestrial bias by treating both as products of the same agent-environment relations.

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Substrate-agnostic perspectives are currently attracting increased attention. For example, it has become customary to refer to agnostic biosignatures to reflect the range of alternative extraterrestrial biospheres and to account for the deeper philosophical dependence of candidate biosignatures on the underlying theory of life. Analogously, one can formulate a concept of agnostic technosignatures, reflecting that the more we expand the search for technosignatures, the more we invite theories of technology that undo the terrestrial bias. For this reason, this paper argues that there exists a strong theoretical justification for an integrated study of technosignatures and biosignatures, articulated in a unified perspective on substrate-agnostic ecologies. The paper introduces the concept of substrate-agnostic ecology as an abstraction unconstrained by terrestrial circumstances, anchored instead in a functional understanding of agent-ecology coupling provided by niche construction theory.
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physics.gen-ph 2026-07-03

94500 emissivity values tabulated for CO2-H2O mixtures

by Osama A. Marzouk

Computed emissivity of carbon dioxide, water vapor, and their mixtures for a wide range of temperatures and pressure-pathlengths

Covers 300-2900 K and 0.01-50 atm.m for ten compositions using the statistical narrow band model

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This article describes a dataset of total (spectrally-integrated rather than wavelength-dependent) emissivity values pertaining to gaseous media containing carbon dioxide (CO2) and/or water vapor (H2O) with the sum of their partial pressures being near the atmospheric level. These conditions may be particularly relevant to flue gases resulting from oxy-fuel combustion. The emissivities here are computed using the EM2C implementations of the statistical narrow band (SNB), and they are made conveniently available as 10 separate plain text files having a unified layout. Each data file in the dataset corresponds to a specific chemical composition (from pure CO2 to pure H2O), with eight intermediate H2O:CO2 molar ratios being 1:20, 1:8, 1:4, 1:2, 1:1, 2:1, 5:1, and 20:1. In addition, pure CO2 corresponds to the extreme lower-bound for the H2O:CO2 molar (as 0:1), and pure H2O corresponds to the extreme upper-bound for the H2O:CO2 molar ratio (1:0 or infinity). For each chemical composition, the total emissivity values are provided for different pressure-pathlengths and different absolute gas temperatures as two independent variables. The pressure-pathlength range spans about three orders of magnitude, from 0.01 atm.m to 50 atm.m, with 90 nonuniformly-distributed pressure-pathlength values. The absolute gas temperature spans a wide range from 300 K (room temperature) to 2900 K (high-temperature flames) with a uniform step of 25 K separating 105 temperature values. For each data file, there are 90 x 105 (9450) emissivity values; and the entire dataset contains 94500 emissivity values.
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physics.gen-ph 2026-06-26

WOH G64 shows red supergiants keep surprising us

by Jacco Th. van Loon

Another one bites the dust -- how red supergiants keep surprising us

Latest observations placed in context with Betelgeuse and supernova progenitors highlight unexpected mass loss and evolution.

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Extreme red supergiant WOH G64 has led researchers a merry dance these last few years, but what does it reveal about the secret lives of these beasts? This article sets the latest observations of WOH G64 in the context of what has been observed in other supergiants such as Betelgeuse and what we are learning from the massive stars that have been identified to explode as a supernova.
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physics.gen-ph 2026-06-25

Coriolis cancellation cost rises as r to the minus four near merry-go-round center

by Mario J. Pinheiro

Why does walking to the center of a merry-go-round feel so hard? Coriolis stabilization and the metabolic cost of staying on track

Model of active force cancellation shows cost scales steeply with falling radius depending on the chosen exponent

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A standard undergraduate problem has a student walk radially inward on a rotating, frictionless merry-go-round. The textbook analysis -- angular momentum is conserved, so the kinetic energy rises and the student does work -- is exactly correct for a point mass. Yet anyone who has tried it knows the effort is dominated by something the point-mass model never mentions: the muscular work of \emph{not} being thrown sideways. We make that effort quantitative with a deliberately minimal model. Treating the student as an active controller that cancels the Coriolis force at a metabolic cost $P \propto F_C^{\,n}$, we show that the cost scales as $r^{-2n}$ as the axis is approached. The widely used quadratic cost ($n=2$) gives a steep $r^{-4}$ rise; a linear cost ($n=1$) gives $r^{-2}$. We argue that this \emph{sensitivity of the prediction to the cost model} is the most useful thing in the problem: it forces students to see how a modeling assumption, not just an algebraic step, drives a physical conclusion. We give an order-of-magnitude estimate (explicitly flagged as such), a one-line entropy-production / efficiency argument that connects the exercise to non-equilibrium thermodynamics, a feedback (PD-controller) reformulation that reproduces the same scaling, and a back-of-the-envelope experiment students can do on a playground with a phone and a heart-rate strap. The material is aimed at an intermediate-mechanics or biophysics elective and is designed to teach model validity, assumption sensitivity, and the idea that staying alive and on-course has a thermodynamic price.
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physics.gen-ph 2026-06-23

Entropy maximization yields one equation for Schrödinger and waves

by Shahid Nawaz, Muhammad Saleem +2 more

Unified Entropic Dynamics Framework for Classical, and Quantum Wave Equations

A universal covariant field equation from information constraints reproduces quantum, electromagnetic and gravitational dynamics as special

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Entropic Dynamics (ED) provides a statistical-inferential foundation for physical laws, deriving motion and field equations from principles of entropy maximization rather than quantization postulates. ED reconstructs quantum mechanics by treating the evolution of probability distributions on configuration space as driven by information constraints, yielding the Schrodinger equation as a non-dissipative diffusion process. Building on this foundation, the present work extends the ED framework into a Unified Entropic Dynamics (UED) formulation that encompasses classical, quantum, relativistic, thermodynamic, and gravitational phenomena within a single information geometric principle. By maximizing entropy subject to constraints on diffusion, drift, and gauge covariance over a manifold endowed with a supermetric H_ab, we derive a universal field equation that merges the Fokker-Planck and Hamilton-Jacobi structures into one covariant form. When specialized to different dynamical variables, this equation reproduces the harmonic oscillator, Schrodinger, Maxwell, Klein-Gordon, and gravitational wave equations, thereby revealing a deep equivalence between probabilistic inference and dynamical law. The UED framework demonstrates that spacetime geometry, quantum coherence and thermodynamic diffusion emerge as complementary expressions of the same entropic process, establishing a unified inferential foundation for both microscopic and macroscopic physics. In this formulation, energy, probability, and entropy are intertwined aspects of information geometry, providing a consistent inferential foundation for understanding classical, quantum, and gravitational dynamics as complementary expressions of a single entropic law.
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physics.gen-ph 2026-06-22

Lindblad terms generate fluctuations in formerly conserved observables

by G. Modanese

Statistics of non-conserved observables in Lindblad master equations

Formulas from the adjoint equation quantify how collapse operators break Hamiltonian conservation and drive variance growth.

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We study the dynamics of observables that are conserved under the Hamiltonian evolution of a closed quantum system, but cease to be conserved when the system is coupled to a Markovian environment and described by a Lindblad master equation. Starting from the adjoint Lindblad equation, we derive elementary expressions for the time derivatives of the expectation value and second moment of an observable $O$, with particular emphasis on the case $[H,O]=0$ but $\mathcal L^\dagger(O)\neq 0$. These formulae provide a direct assessment of how collapse operators break Hamiltonian conservation laws and generate fluctuations of formerly conserved quantities. The discussion is illustrated by analytic examples: one-qubit amplitude damping, a two-qubit excitation-number model, a momentum-diffusion model in which the mean is conserved while the variance grows, and the Jaynes-Cummings model. The latter also shows the complementary case of a reservoir coupled through a conserved quantity, where dephasing can occur without changing the statistics of that quantity. We finally comment on the relation between Lindblad source terms and idealized wave-function reduction models in which local conservation may hold only statistically.
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physics.gen-ph 2026-06-22

Factor (1+z_t)^{-3} aligns CCC+TL with chronometer data

by Rajendra P. Gupta

Testing the CCC+TL cosmology with cosmic-chronometer measurements of the Hubble parameter

The correction motivated by gas cooling timescales reduces alpha tension from 6 sigma to 0.13 sigma without recomputing stellar models.

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In a recent paper, it was shown that the Covarying Coupling Constants and Tired Light (CCC+TL) hybrid model yields the Hubble parameter $H(z)$ that is substantially different from its measured value using differential aging of quiescent galaxies as cosmic chronometers (CC). It was claimed that the fit of the CCC+TL model to the $H(z)$ data results in a best-fit value for the parameter $\alpha$, defining the strength of the co-variation of the constants, disagreeing with that for the SN~Ia data at the $\sim 6\sigma$ level. In this paper we re-examine the assumptions underlying such a comparison. Cosmic-chronometer measurements are designed to be independent of cosmological priors, but they nevertheless rely on stellar population synthesis models, isochrones, and age-dating calibrations developed within standard stellar-evolution physics. Therefore, even before introducing any specific correction factor, the present CC compilation cannot be regarded as a model-independent falsification of CCC+TL without recomputing the relevant stellar population models in that framework. In the absence of such a recalculation, we ask a more limited question: what type and magnitude of modification to the effective differential-age relation would be sufficient to remove the claimed tension? We show that a phenomenological factor of the form $\sim (1+z_t)^{-3}$ with $z_t$ being the TL contribution to the observed redshift, motivated by the scaling of gas cooling times for galaxy formation in the CCC+TL framework compared to $\Lambda\text{CDM}$, is sufficient to reduce the apparent discrepancy in $\alpha$ to $\sim 0.13\sigma$. Since $z_t = 0$ for the stellar model primarily developed from local stellar observations, the stellar-aging methods may be unable to verify $\sim (1+z_t)^{-3}$ dependence.
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physics.gen-ph 2026-06-19

Sputtering turns olivine rock into CO2-capturing nanoparticles

by Brendan Matulis, Greyson Wells +8 more

Magnetron Sputtering Formation of Nanoparticles from Natural Olivine Rock for Atmospheric CO2 Capture

Natural mineral processed at nanoscale shows room-temperature uptake of atmospheric carbon, confirmed by multiple measurements.

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The two-birds-one-stone mineralization of CO2 by olivine, is a promising method to both capture carbon directly from the atmosphere and at the same time locking it for storage or utilization. Converting olivine to the nanoscale considerably enhances the kinetics without the need for high temperatures or pressures. Here we present the fabrication of olivine nanoparticles from a natural rock that were fabricated in a gas aggregation magnetron nanoparticle generator. The nanoparticle yield was optimized by enhancing the argon plasma sputter plasma by hydrogen introduction and varying the aggregation distance. The hysteresis of the argon sputter plasma with respect to power is a promising property towards energy efficiency. The formation of well-defined olivine nanoparticles and their subsequent absorption of atmospheric CO2 was confirmed by a suite of techniques. The olivine sputter target surface revealed an intricate interplay between the sputter plasma and olivine composition in terms of crystallinity and morphology. More broadly, this work forms the next step in the practical application of Olivine nanoparticles for economical carbon capture and storage, it also is the starting point for the use of this specific nanoparticle technology for mineral-to-nanoparticle conversion.
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physics.gen-ph 2026-06-18

Degenerate wormholes solve modified vacuum equations at throat

by Juri Dimaschko

Non-degenerate and degenerate wormholes: a unified approach

Einstein-Rosen and Klinkhamer configurations fit the g squared framework as global vacuum solutions, unlike non-degenerate cases that need e

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A generalized notion of degenerate wormholes is introduced, defined by the vanishing of the metric determinant g at the throat. It is described by the polynomial, g^2 modified Einstein field equations. Building on this framework, we show that both the Einstein Rosen bridge and the Klinkhamer defect wormhole are exact vacuum solutions of the g^2 modified equations, valid globally including at the degenerate throat, while the Klinkhamer configuration additionally admits traversable geometries with b>2M, where b sets the length scale of the wormhole throat and M is a mass parameter. In contrast, standard Morris Thorne and thin shell wormholes, governed by the conventional (non regularized) Einstein equations, are intrinsically non degenerate and necessarily supported by exotic stress energy. Within a unified regularized system with matter, both thin shell and Klinkhamer wormholes appear as two qualitatively distinct classes of states: non degenerate with exotic matter versus degenerate with vacuum sharing the Einstein Rosen bridge as a common limiting configuration. This unified viewpoint clarifies why classical null energy condition no go theorems apply only to the non degenerate sector and suggests the possibility of stationary degenerate traversable wormholes that do not require NEC violation.
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physics.gen-ph 2026-06-18

Critical chemical potential divides Fermi gas gravity regimes

by Pattarapon Tanalikhit, Wittaya Kanchanapusakit

An ideal Fermi gas under uniform gravity

Zero-temperature ideal gas shows separate weak and strong gravity energy expressions.

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We consider an ideal Fermi gas in a container subject to a uniform gravitational field at absolute zero temperature. Under a semiclassical approximation, we examine the density profile of the particles and derive an expression for the chemical potential. A critical value of the chemical potential separates the weak- and strong-gravity regimes, and the kinetic and potential energies of the Fermi gas are determined in both regimes.
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physics.gen-ph 2026-06-18

Power-law f(R) gravity boosts structure growth

by Murli Manohar Verma

Cosmic Structure Formation in a Viable Power-Law f(R) Gravity Model: Growth Dynamics, Stability, and Observational Signatures

A single deviation parameter enhances perturbation growth while satisfying stability and matching acceleration data.

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We investigate the evolution of cosmic structures in the power-law modified gravity model $f(R)=R+R^{1+\delta}/R_c^\delta$, where the dimensionless parameter $\delta$ characterizes deviations from General Relativity. The background cosmological dynamics and the evolution of linear matter density perturbations are studied within the framework of metric $f(R)$ gravity. The modified perturbation equation is derived by introducing an effective gravitational coupling associated with the additional scalar degree of freedom, and the evolution of the growth factor, logarithmic growth rate, growth index, and the observable quantity $f\sigma_8(z)$ are investigated. The results show that the curvature correction enhances the growth of matter perturbations while remaining compatible with the observed late-time accelerated expansion for suitable values of the model parameter. The theoretical viability of the model is established through the ghost-free condition, Dolgov--Kawasaki stability criterion, positive scalaron mass, stable de Sitter solution, and chameleon screening mechanism. Comparison with representative viable $f(R)$ gravity models shows that the present theory achieves a consistent cosmological evolution with a single deviation parameter. The predicted modifications in the growth of structures and the effective gravitational coupling provide observable signatures that can be tested by forthcoming large-scale structure and weak-lensing surveys, providing a means to test curvature-induced modifications of gravity.
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physics.gen-ph 2026-06-17

Local tests force swampland scalars into ultra-slow motion

by Suraj Gavhale, Maxim Khlopov +2 more

Solar System and Atomic Clock Bounds on Locally Coupled Swampland Scalars

This blocks order-one de Sitter gradients from visible couplings alone, requiring screening or hidden sectors.

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We study how local measurements can constrain light scalar fields that are relevant for late time cosmic acceleration and are often discussed in connection with swampland criteria. Starting from a scalar-tensor framework, we define the relevant swampland quantities in the canonically normalized Einstein frame and relate them to Solar System, Lunar Laser Ranging, equivalence principle, and atomic clock bounds. These probes do not constrain the scalar velocity by itself but rather products of the scalar motion with microscopic couplings to matter, gravity and atomic parameters. For coupling directions that are visible to local experiments, the scalar is driven into an ultra slow present regime and this leads to severely restricting the possibility of realizing an $\mathcal{O}(1)$ de Sitter gradient through unscreened visible sector couplings alone. The refined de Sitter alternative remains viable only in restricted regions of parameter space, such as near a hilltop or under tuned dynamical evolution.
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physics.gen-ph 2026-06-16

Nonlocal QFT replaces points with finite phase-space cells

by E. J. Thompson

On the Meaning of Localization in Non-Local Quantum Field Theory and On the Limits of a Space-Time Description and the Physical Meaning of Phase Space in a Nonlocal Continuum

Variance addition from the detector kernel plus Heisenberg gives a cell size set by the regulator that survives the ultraviolet limit.

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First: In this paper we explore and derive an uncertainty principle for an ultraviolet complete nonlocal quantum field theory where under our hypothesises of an induced equal time detector response kernel, we then prove that the observed localization width obeys an exact variance addition law. Then when we combine this with the ordinary Heisenberg inequality and we obtain a nonlocal uncertainty relation. The bound reduces to the usual local relation in the infrared or local limit when $E_M \to \infty$, while in the ultraviolet it implies a minimal localization length of order $L_M$. We go on to explain what this means for locality, microcausality, the interpretation of spacetime points, and the ultraviolet structure of quantum field theory. In this formulation we note and prove that spacetime will remain a Lorentz covariant continuum at the level of the manifold description but pointlike localization ceases to be a physically realizable observable notion below the nonlocality scale. Second: In a previous paper we derived an uncertainty relation for nonlocal fields by showing that the physical localization width in nonlocal quantum field theory is broadened by the response kernel generated from the entire-function regulator. In this follow up we will reinterpret that result as just the position-sector limit of a more symmetric statement as we did not take into account the inherent nonlocality of momentum. We find under normalized, centered response kernels for both position and momentum, we prove the variance laws and derive the corresponding nonlocal phase-space uncertainty relation. The result still preserves the conclusions of the original paper all while strengthening the interpretation as nonlocal quantum field theory implies not merely a minimal measurable length, but a finite phase-space cell. We also explore experimental routes to test the theory.
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physics.gen-ph 2026-06-15

Weyl transform recasts QFT as Gaussian zero-point addition

by Emilio Santos

Quantum field theory in the Weyl-Wigner representation

Standard operator quantization of Bose fields becomes equivalent to superposing a Gaussian distribution on the classical vacuum.

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The Wigner representation for quantum mechanics of particles is generalized to Bose fields. The standard Hilbert space quantization becomes, via the Weyl transform, a quantization method that consists of adding a Gaussian zeropoint field distribution to the vacuum. I comment on the possible advantages of the method in order to study quantum fields in curved spaces. I study a unified formulation of non-relativistic quantum electrodynamics in the Weyl-Wigner formalism, in terms of (classical-like) c-numbers.
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physics.gen-ph 2026-06-11

Codazzi defect loop selects standard model symmetry and one-generation package

by Piotr Ogonowski

Self-Reconstructing Codazzi Defects, mathbb{CP}¹ Quantization, and the Minimal Standard-Model Carrier

Reconstruction fixes E3 ⊕ E2 support and degree-one line, then yields S(U(3)×U(2))/Z6 with conventional hypercharge and anomalies.

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A filtered local reconstruction scheme is formulated for codimension-three Codazzi defects in four-dimensional Lorentzian branches. The closure defect of the self-reconstruction loop is organized as a lexicographic residual whose entries fix, in order, the projective link, Gauss-local charges, Toeplitz support, determinant carrier, finite shadow, torsor response, and Schur completion. For a worldline defect with resolved link $\mathbb{CP}^1_\Gamma$, the scalar two-jet leaves two principal non-scalar types, $V_1$ and $V_2$. Faithful reconstruction of these Gauss-local charges, together with $\mathbb{CP}^1$ Toeplitz visibility, selects the separated support $E_3\oplus E_2$; reduced finite visibility fixes the degree-one line. After this carrier has been selected, the split top-form condition gives the familiar $S(U(3)\times U(2))/\mathbb Z_6$ global form and the standard one-generation exterior package, with the usual hypercharge normalization and anomaly checks. This determinant package is used as the structural comparison layer for the reconstructed carrier. The remaining construction keeps the full $\mathbb Z_6$ finite shadow, realizes its projective-color projection as a boundary torsor, and organizes the locked low sector by a $B-L$-filtered Schur-Kuranishi completion. Yukawa, neutrino, mixing, running, and contact coefficients are thereby treated as completed-branch data rather than as inputs to the carrier selection. A scale-free charged-lepton balance residual is recorded as a Schur-layer diagnostic; its zero-correction form gives the Koide-type singlet-torsor balance, while the observed deviation is left as a finite Schur-tensor datum.
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physics.gen-ph 2026-06-11

Higher-D unimodular gravity reduces to cosmology with continuous equilibria

by A. M. Velásquez-Toribio, J. C. Fabris

Dynamical systems analysis of unimodular cosmology in D=4+d dimensions

The vacuum phase space after reduction contains a continuous family of equilibrium points at λ=dH, unlike the discrete structure of general

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We investigate the effective four-dimensional cosmology induced by unimodular gravity in $D=4+d$ dimensions, where the internal extra-dimensional volume is encoded in a scalar degree of freedom. After dimensional reduction, we show that the resulting FLRW equations admit a natural autonomous formulation whose phase-space structure differs qualitatively from that of general relativity. In the vacuum sector, the reduced system exhibits a continuous family of finite equilibrium points, $\lambda=dH$, together with well-defined asymptotic Poincar\'e directions. In the matter sector, we focus on the five-dimensional case $d=1$ and use the reduced Bianchi relation as the consistency condition that links the ordinary matter component to the internal-volume degree of freedom. The system is then closed by adopting the minimal higher-dimensional conservation prescription, according to which matter is diluted by both the external volume and the internal-volume modulus. This leads to a reduced matter--geometry dynamics with isolated critical points and a globally organized compactified flow. Numerical examples illustrate how the internal-volume degree of freedom affects the background evolution and the global phase-space structure. The comparison with $\Lambda$CDM is used only as a benchmark, while a full observational analysis and more general matter--geometry exchange prescriptions are left for future work.
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physics.gen-ph 2026-06-10

Superconductivity theory contradicts second law

by A.V. Nikulov

Belief in thermodynamics has provoked false thermodynamics of superconductors

Meissner effect performs negative surplus work in Gorter cycle, violating thermodynamics.

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Belief in thermodynamics has forced superconductivity experts to forget basics of thermodynamics due to a contradiction of superconductivity phenomena to laws of thermodynamics. Because of this belief no one drew reader's attention during many years that the conventional theory of superconductivity contradicts to the second law of thermodynamics. The common belief that the superconducting transition occurs when the free energy of the superconducting state becomes less than of the normal state has provoked a false claim that a power source of a solenoid creates the energy of magnetization rather than of magnetic field. The authors of only a few books on superconductivity, mostly future Nobel prize winners, did not follow this false claim. No one for many years has noticed that the equality of free energies at the superconducting transition in the critical magnetic field cannot be obtained without contradicting the second law of thermodynamics. The Meissner effect violates the second law of thermodynamics because of the negative surplus work performed in the closed Gorter cycle. The desire to avoid contradiction of superconductivity phenomena with the second law of thermodynamics provoked the false thermodynamics of superconductors, contradicting the law of conservation of energy.
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physics.gen-ph 2026-06-10

MeV gap blocks gamma-ray progress on nucleosynthesis and dark matter

by Alessandro de Angelis

MeV-GeV Gamma-Ray Astrophysics in the Multimessenger Era

Review shows the few-hundred-keV to few-GeV range remains the main sensitivity limit for transients, positrons, and multimessenger counterpa

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Gamma-ray astrophysics probes the most extreme particle accelerators and explosive transients in the Universe. From pioneering theoretical predictions in the 1950s and the first space-borne detections in the 1960s, mostly exploring the sub-MeV region, the field has evolved into a mature, multi-decade enterprise that spans nine orders of magnitude in photon energy up to PeV energies and interfaces naturally with neutrino and gravitational-wave astronomy. Yet the energy range from a few hundred keV to a few GeV -- the "MeV gap", constraining progress on nucleosynthesis, positron annihilation, transient physics, dark-matter signatures, and electromagnetic counterparts to high-energy neutrinos and gravitational waves - remains sensitivity-limited. In this paper, we survey the scientific motivations for gamma-ray astrophysics, sketch a concise history from the first ideas to key milestones in space- and ground- based gamma-ray astronomy, and discuss programmatic attempts to close the MeV gap.
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physics.gen-ph 2026-06-10

VCDM matches ΛCDM background expansion under Padé analysis

by Soumya Kanta Bhoi, Sai Swagat Mishra +1 more

Kinematic Probes of Type-II MMG: Pad\'e Cosmographic Analysis of VCDM

Joint chronometer, BAO and supernova constraints give jerk near 1 with no transition feature.

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We study the late-time expansion history of the Universe within the VCDM model, a Type-II MMG realization that preserves the successes of General Relativity while extending beyond constant vacuum energy through a minimal Hamiltonian modification, generating a time-dependent vacuum sector without introducing additional degrees of freedom. We investigate this framework within a cosmographic approach by employing a Pad\'e $P_{(2,1)}$ approximation for the Hubble parameter and luminosity distance, allowing the cosmographic parameters to be expressed directly in terms of the underlying VCDM model parameters and enabling a data-driven reconstruction of the expansion history. The model is constrained within a Bayesian framework using the MCMC technique, implemented via the affine-invariant ensemble sampler, with a joint analysis of cosmic chronometers, DESI BAO, and Type Ia supernova datasets (Union3, Pantheon+, and DESY5). We find that the model parameters are tightly constrained and consistent across different dataset combinations, with the jerk parameter remaining very close to its $\Lambda$CDM value, $j_0 \simeq 1$, indicating no significant deviation at the level of higher-order cosmography. Furthermore, the transition feature previously reported in VCDM is not observed within the Pad\'e $P_{(2,1)}$ cosmographic reconstruction, suggesting that it is not a robust requirement of current observational data but is sensitive to the choice of parametrization. Overall, our results indicate that the VCDM model effectively mimics $\Lambda$CDM at the background level when constrained through a cosmographic approach, underscoring the importance of model-independent reconstructions in assessing alternative cosmological scenarios.
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physics.gen-ph 2026-06-10

Adiabatic photon creation extends cosmic temperature law

by J.A.S. Lima, S.R.G. Trevisani +1 more

Cosmic adiabatic photon creation: Temperature law and blackbody spectrum

Three methods agree the Planck spectrum survives expansion, giving a thermal test of the concordance model and a possible handle on the H0 t

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The temperature-redshift relation (cosmic thermometer) is rediscussed in the framework of gravitationally induced photon production in the expanding universe. It is found that the same extended temperature law can be derived based on three independent methods, namely: (i) through a simple heuristic approach, (ii) based on macroscopic irreversible thermodynamics with photon creation, and (iii) using a kinetic relativistic Boltzmann equation incorporating gravitational photon creation. All these methods yield the same answer. The modified kinetic treatment reveals not only that the Planckian blackbody spectrum endowed with the adiabatic creation is preserved in the course of the expansion but also that CMB anisotropies and distortions can be treated properly. The new cosmic thermometer suggests a crucial test to the standard cosmic concordance model in the thermal sector. It is also argued that the present results may open a new route for scrutinising the H0 Supernovae-CMB tension challenging the LambdaCDM model.
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physics.gen-ph 2026-06-09

Inverse Koide rule parametrizes down quarks to lepton precision

by Alejandro Rivero

New sum rules of the Koide type

The form m_i = M (w0 + wi)^{-2} reaches exactly 2/3 ratio at 280 TeV after Standard Model running.

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We report a mass rule of Koide type with inverse shape, \[m_i=M^{(d)} (w_0+w_i)^{-2}.\] It applies to the down-quark sector with numerical precision comparable to that of the direct charged-lepton sum rule $m_i=M^{(l)} (z_0+z_i)^{2}$. For central mass values, Koide ratio reaches exactly $2/3$ near 280 TeV under Standard Model renormalisation-group running. We also review other rules of the direct kind involving quarks.
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physics.gen-ph 2026-06-09

Diagnostic framework places six cosmological benchmarks in distinct regions

by Hassan Ugail

Geometric Phase-Space Structure in Cosmological Solutions of Einstein's Field Equations

Standard geometric quantities isolate inhomogeneity, shear and Weyl effects while remaining stable under resolution and domain changes.

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Einstein field equations allow cosmological dynamics to depart from the Friedmann-Lemaitre-Robertson-Walker (FLRW) idealisation in several physically different ways. Matter may become spatially inhomogeneous, the local expansion scalar may vary across a hypersurface, the expansion may acquire anisotropic components through shear, and the free gravitational field may be encoded in nonzero Weyl curvature. The key question is not only how far a model is from FLRW, but which geometric mechanism is responsible. A single departure from FLRW number cannot distinguish these mechanisms. This paper introduces a compact geometric diagnostic framework that keeps them separate while using standard quantities in general relativity. The framework is observer-explicit and domain-explicit, intended as a practical tool for comparing analytic and numerical solution families rather than as a new invariant classification of spacetime. Buchert's kinematical backreaction is retained as a derived explanatory quantity rather than a separate axis, since it is already fixed by the expansion-variance and shear contributions. A single curvature normalisation is used for all Weyl diagnostics. The method is tested on six benchmarks, namely FLRW, Bianchi-I, Kasner, Lemaitre-Tolman-Bondi dust, scalar-perturbed FLRW, and tensor-perturbed FLRW. These benchmarks occupy distinct regions of the diagnostic space, and the magnetic Weyl contribution appears only in the tensor case. The classification remains stable under changes of perturbation amplitude, spatial resolution, averaging domain, constraint reliability, and a leading-order observer tilt. The curvature expressions for the exact benchmarks are verified symbolically against metric-derived Weyl invariants, and the supporting computer code, numerical results, tables, and figures are publicly available.
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physics.gen-ph 2026-06-09

Projective map turns linear Lorentz action into nonlinear transformations

by Abdelmalek Boumali, N. Jafari +1 more

Generalized Fock--Lorentz Transformations from Projective Conformal Coordinates and Their Application to One-Dimensional Relativistic Oscillators

Auxiliary coordinates produce apparent-mass corrections to one-dimensional Klein-Gordon and Dirac oscillator spectra that vanish as deformat

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We present a compact and systematic formulation of the generalized Fock--Lorentz (FL) transformations. The construction is based on a family of auxiliary Minkowski coordinates defined through a projective conformal map, $X^{\mu}=x^{\mu}/[1+a_{\nu}x^{\nu}/R]$, where $R$ denotes a deformation length and $a^{\mu}$ a constant deformation vector. Ordinary Lorentz transformations, acting linearly on $X^{\mu}$, thereby induce nonlinear transformations of the physical coordinates $x^{\mu}$. This formulation renders transparent the structure of the invariant interval, the role of the conformal factor, and the distinct limits associated with the time-like, space-like, and null (light-like) choices of $a^{\mu}$. We further clarify the operational meaning of the coordinate-dependent speed of light, as well as its momentum-space dual, which yields the apparent mass $\mapp(x)=m_{0}/[1+a_{\mu}x^{\mu}/R]$. As a controlled application, we construct a symmetrized one-dimensional Klein--Gordon oscillator and a one-dimensional Dirac oscillator in the time-like sector, for which $\mapp(t)=m_{0}/(1+ct/R)$. Within the adiabatic regime, the associated instantaneous spectra acquire explicit FL corrections and reduce continuously to the standard relativistic oscillator spectra in the limit $R\to\infty$. Finally, we determine the leading weak-gradient anharmonicity induced by a one-dimensional space-like deformation and identify the conditions required for a consistent quantum treatment.
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physics.gen-ph 2026-06-08

Extra-time dimension carries entanglement via bulk field

by Marco Pettini

Quantum Entanglement Beyond Kinematics: A Dynamical Hypothesis in (3,2)-Dimensional Spacetime

A massless field propagating through an additional time coordinate produces equal-time correlations at arbitrary distances without controlla

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Quantum entanglement produces nonlocal correlations for which no local dynamical account is known. In Ref.[1] we proposed that these correlations are mediated through an extra temporal dimension and introduced a $(3,2)$-dimensional spacetime framework on a phenomenological basis; the present paper derives that framework from the bulk geometry. A single extra spatial dimension admits no effective superluminal shortcut on the brane, this rules it out as a candidate mediator and motivates the extra-time setting. Within the warped-product metric ansatz the five-dimensional vacuum Einstein equations fix the warp factor uniquely, leaving no freedom in the geometry once $\mathbb{Z}_2$ symmetry is imposed. A massless bulk field $\mathscr{X}_a(\mathbf{x},t,\tau)$, sourced on the brane by the preparation event and by the measurement interactions, propagates causally through the extra-time dimension; equal-time correlations at arbitrarily large brane separation arise via the $E=0$ null geodesic family, without admitting controllable superluminal signaling. The propagation time and crossed ratios of Ref.~\cite{PRR}, previously postulated, emerge here from the null geodesic kinematics. The Bohm--Bub collapse framework is extended to a bipartite entangled system by replacing the abstract hidden vector with the brane-projected bulk field $\mathscr{X}_a$. At fixed contextual microstate $\lambda$ collapse is deterministic; Born statistics follow upon averaging over an equivariant ensemble. When the framework is extended to two independent Bell pairs, the bulk field sourced by one pair reaches the detectors of the other and induces a cross-pair correlation scaling as the square of the intra-pair to inter-pair separation ratio, a concrete falsifiable prediction with no counterpart in standard quantum mechanics, accessible with existing photonic Bell-test technology.
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physics.gen-ph 2026-06-08

Hyperstatistics yields closed-form q-Boltzmann factor independent of f(beta)

by Abdelmalek Boumali

Hyperstatistical thermodynamics of the one-dimensional Klein-Gordon and Dirac oscillators: a closed-form q-generalized Boltzmann factor and a quantitative comparison with Beck's superstatistics

The expression for 1D Klein-Gordon and Dirac oscillators stays positive at high temperatures and distinguishes degeneracy effects.

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We revisit the thermodynamics of the one-dimensional Klein-Gordon (KGO) and Dirac (DO) oscillators within two frameworks of generalized statistics: Beck's asymptotic superstatistics and the recently introduced hyperstatistics. In hyperstatistics, a $\gamma$-distribution of domain Boltzmann factors yields, after Laplace transformation and averaging over a normalisable density $f(\beta)$, the closed-form q-generalized Boltzmann factor $B_q(\varepsilon) = \exp_q(-\langle\beta\rangle\varepsilon)$, independent of $f(\beta)$. We compute the partition function, entropy $S$, and specific heat $C_v$ for both 1D oscillators using excitation energies $\varepsilon_n = E_n - E_0$ to remove the rest-energy shift and enforce third-law behaviour $C_v \to 0$ as $T = 1/\langle\beta\rangle \to 0$. Appropriate degeneracies ($g_n = 1$ for KGO; $g_0 = 1$, $g_n = 2$ for $n \geq 1$ for DO) are applied. Hyperstatistics successfully (i) reproduces the high-temperature Boltzmann limit $C_v \to 2k_B$, (ii) is structurally independent of $f(\beta)$, (iii) avoids the unphysical negative regions of the Beck polynomial bracket, and (iv) systematically distinguishes KGO from DO by capturing the enhanced entropy and sharper specific-heat structure caused by spin-induced degeneracy. The frameworks agree quantitatively for $q - 1 \ll 1$ and $\langle\beta\rangle E \lesssim 2$, but diverge at high temperatures where Beck's polynomial expansion loses validity and the exact hyperstatistical q-exponential remains positive, monotonic, and analytic. Ultimately, hyperstatistics provides a numerically stable and analytically tractable alternative to asymptotic superstatistics for relativistic oscillators, naturally extensible to higher dimensions and external magnetic fields.
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physics.gen-ph 2026-06-04

Stellar cycles lengthen and weaken with age

by Travis S. Metcalfe (Center for Solar-Stellar Connections)

Stellar Activity Cycles Grow Longer and Weaker Before Disappearing

California Legacy Survey data shows the Sun follows the same trend as other stars rather than being unusual.

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In 2007, Erika Bohm-Vitense published a provocative figure suggesting that the solar rotation period and activity cycle made the Sun an outlier compared to the trends observed for stars in the Mount Wilson HK survey. A decade later, after the discovery of weakened magnetic braking (WMB), an evolutionary scenario was proposed that could account for the properties of the Sun if activity cycles grow longer and weaker in the WMB regime. Recent observations of the gradual onset of WMB suggest that the efficiency of the global stellar dynamo declines by at least two orders of magnitude as the stellar Rossby number approaches a critical point slightly above the solar value. A new sample of activity cycle data from the California Legacy Survey suggests that the Sun is not an outlier, and unambiguously confirms that activity cycles grow longer and weaker on stellar evolutionary timescales.
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physics.gen-ph 2026-06-03

FL dual in momentum space yields time-dependent apparent mass

by Abdelmalek Boumali, N. Jafari +1 more

Klein--Gordon and Dirac Oscillators with an Apparent Mass Induced by the Momentum-Space Dual of the Fock--Lorentz Transformations

The deformed shell produces KG and Dirac operators whose oscillator spectra drift with m_app(t) and collapse to zero at late times.

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We propose a controlled momentum-space dual of the Fock--Lorentz (FL) transformations and use it to derive a deformed relativistic mass shell. Restricting the FL conformal factor to the cosmological-frame world line $\vx=0$, the invariant relation takes the form $(E^{2}-\vp^{2}c^{2})(1+ct/R)^{2}=m_{0}^{2}c^{4}$, which is equivalent to the standard special-relativistic dispersion law with a time-dependent apparent mass $\mapp(t)=m_{0}/(1+ct/R)$. Canonical quantization then yields Klein--Gordon (KG) and Dirac equations containing a slowly varying mass scale. We show explicitly that squaring the Dirac equation reproduces the KG operator, modulo first-order corrections proportional to $\dot\mapp$ that are suppressed by the ratio of the Compton wavelength to the FL scale. The construction is not presented as a unique covariant phase-space theory; rather, it is a world-line ansatz designed to isolate the spectral consequences of the FL conformal factor. As applications, we study the one-dimensional KG and Dirac oscillators. In the adiabatic regime, governed by the small parameter $\epsilon=c/(R\omega)\ll1$, closed-form instantaneous spectra are obtained. The Dirac-oscillator calculation is carried out in component form and then reduced to the physical spinor spectrum, thereby avoiding the double counting of the upper and lower component ladders. Dimensionless plots illustrate the apparent-mass drift, the induced spectral evolution, and the domain of adiabatic validity. For cosmological values of $R$, non-adiabatic corrections are entirely negligible; in the formal limit $t\to\infty$ the apparent mass tends to zero and, for fixed quantum number, the instantaneous levels collapse toward $E=0$.
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physics.gen-ph 2026-06-02

Quadratic f(Q) gravity lowers predicted S8 by weakening gravity

by G.G.L. Nashed, P.V. Tretyakov +1 more

Late-Time Cosmology and Structure Formation in Quadratic f(Q) Gravity

The model damps linear and nonlinear structure growth while remaining compatible with distance data, offering a modified-gravity route to th

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We investigate the cosmological evolution associated with the quadratic symmetric teleparallel gravity framework, \( f(Q)=Q+\alpha Q^{2}+\beta \) where the relation \(Q\propto H^{2}\) generates an additional \(H^{4}\) contribution to the Friedmann equation. Using the exact algebraic solution for $H(z)$, we reconstruct the effective dark-energy sector and compare the background evolution with $\Lambda$CDM using Type Ia supernovae, BAO, and cosmic-chronometer data. At the perturbative level, the model modifies the Poisson equation through a time-dependent effective gravitational coupling $G_{\textrm eff}(z)=G\big[1+\tfrac{2}{3}A E^{2}(z)\big]^{-1}$, where $A=18\alpha H_{0}^{2}$. For $\alpha>0$ this produces a weakened gravitational interaction, suppressing the linear growth factor $D(z)$, the growth rate $f(z)$, and the RSD observable $f\sigma_{8}(z)$. In the nonlinear regime, the reduced gravitational strength increases the spherical-collapse threshold and suppresses the halo mass function, leading to a lower predicted value of $S_{8}=\sigma_{8}\sqrt{\Omega_{m}/0.3}$. Thus, the quadratic $f(Q)$ extension can reproduce mild deviations from $\Lambda$CDM at the background level while naturally alleviating the $S_{8}$ tension, offering a viable modified-gravity explanation for recent observational hints of dynamical dark energy.
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physics.gen-ph 2026-06-01

Gödel universe models superconductor in Meissner state

by Daniel Flores-Alfonso, Cesar S. Lopez-Monsalvo +1 more

The G\"odel Universe as a Superconductor

Exact Einstein-equation solution encodes magnetic-field expulsion through geometry alone.

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Material science and engineering have benefited from the use of geometric and topological tools. A material medium can mimic effective gravitational fields while spacetime metrics serve as geometric models of physical media. Although analog models of optical, acoustic, and viscous media in curved spacetimes are well established, none have yet captured the hallmark constitutive properties of superconductors. In this work we show that the G\"odel universe - an exact solution to Einstein's field equations - serves as the gravitational analog of a superconducting medium in its Meissner state.
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physics.gen-ph 2026-06-01

Many-body GR leads to thermal equivalence principle

by Riccardo Fantoni

Many Body in General Relativity: A thermal equivalence principle

Review traces stress-energy tensor through hydrodynamics and N-body statistics to a unifying thermal rule.

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We review the physics of many bodies in the context of general relativity. Starting from the stress energy tensor for one body, for a swarm of bodies, for a perfect fluid, we review relativistic hydrodynamics, kinetic theory, and statistical physics of $N$ identical bodies. We conclude our excursion with a {\sl thermal equivalence principle} in physics.
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physics.gen-ph 2026-06-01

Physics inequalities map constants to exoplanet biosphere conditions

by Slava G. Turyshev

Quantitative Nonequilibrium Pathway from Fundamental Physics to the Emergence and Persistence of Exoplanetary Biospheres

A chain of gates anchored in nuclear resonances and thermodynamics yields observable margins for emergence and persistence.

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We present a physics-based framework that runs from fundamental interactions and constants to biospheres, using a sequence of quantitative nonequilibrium thresholds ("gates"). Each gate is an inequality in measurable variables-free-energy flux, reaction-transport rates, replication fidelity, coding capacity, ecological closure, and climate feedback gains. Crucially, the gate vector is anchored in fundamental physics: dimensionless constants, nuclear resonance placements (e.g., the $^{12}$C Hoyle state), statistical mechanics (Landauer's bound $k_BT \ln 2$) fix the energetic, kinetic, information-theoretic margins that propagate through the gates. This anchoring lets us propagate sensitivities of the constants into biosphere-level metrics (net primary productivity (NPP), cycle-closure ratios, and climate feedback gain), yielding an end-to-end map from constants to biospheres. The framework is predictive: it yields testable inequalities, margin rankings, and population-level correlations between stellar and planetary boundary conditions and biosphere feasibility. It does not claim point predictions of life prevalence; rather, it specifies which gate margins are observable-bounded versus prior-dominated under explicitly stated chemistry/solvent families and forward models. Darwinian dynamics (heritable variation under selection) appears mid-pipeline; the end of the pipeline is a planet-scale biosphere capable of sustaining positive NPP, closing elemental cycles over geologic time. Questions of prevalence are secondary; our primary objective is to establish a constructive physics->chemistry->biology->genetics->ecosystems pipeline with testable margins and observables. As a result, we recast abiogenesis and biosphere persistence as a gate vector of falsifiable inequalities and map their margins to exoplanet observables, turning the problem into a phase diagram with explicit, testable slack.
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physics.gen-ph 2026-05-29

Dual to inverted oscillator regularizes quantum gravity

by K. Sravan Kumar

The Saddle Point of Everything

Virtual spin-2 sector in four-dimensional theory yields non-singular universe and Starobinsky inflation.

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The harmonic oscillator is the universal Hamiltonian of stable equilibrium. Its counterpart, the inverted harmonic oscillator (IHO), is the Hamiltonian of unstable equilibrium: the saddle point of physical systems. It appears across disciplines, from condensed matter, quantum optics, and quantum chemistry to the Standard Model Higgs instability and quantum field theory near gravitational horizons. Its mathematical depth is further reflected in its relation to the non-trivial zeros of the Riemann zeta function through the Berry-Keating Hamiltonian. Remarkably, a dual Hamiltonian to the IHO has recently been shown to govern the additional spin-2 sector of the unique unitary perturbatively renormalizable theory of quantum gravity in four dimensions, with that sector remaining purely virtual and regularizing gravitational interactions at the Planck scale. This paper argues that the universal physics of the saddle point course-corrects the history of quantum gravity approaches that abandoned renormalizability, uniqueness, and predictivity. Its consequences include a non-singular Universe, Starobinsky inflation, and possible implications for large-scale CMB features and primordial gravitational waves.
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physics.gen-ph 2026-05-28

Constrained scalar-Gauss-Bonnet model gives r ≈ 2.7×10^{-4}

by G.G.L. Nashed, Sudan Hansraj +1 more

Effective Constrained Scalar--Gauss--Bonnet Inflation Motivated by f(R,mathcal{G}) Gravity

Effective slow-roll treatment from f(R,G) gravity yields n_s ≃ 0.958 while the exact theory removes propagating scalar modes.

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We develop an effective framework for inflation in a constrained scalar--Gauss--Bonnet theory motivated by a restricted sector of $f(R,\mathcal{G})$ gravity. Using unified parametrizations of the Hubble expansion rate and the Gauss--Bonnet coupling function within a generalized slow-roll formalism, we derive analytical expressions for the scalar spectral index $n_s$ and tensor-to-scalar ratio $r$, and study their dependence on the model parameters. We show that the Hubble parametrization mainly controls the scalar sector through the slow-roll parameter $\epsilon_1$, while the Gauss--Bonnet-induced contribution $\epsilon_4$ can significantly affect the scalar tilt and strongly suppress primordial tensor modes, naturally leading to very small values of $r$. A representative benchmark solution yields $n_s \simeq 0.958$ and $r \simeq 2.7 \times 10^{-4}$, marginally compatible with current Planck, ACT, and BICEP/Keck constraints. We further investigate the scalar perturbation structure of the exactly constrained theory, where the Lagrange-multiplier constraint forces the lapse perturbation to vanish and, together with the gravitational momentum constraint, implies $\dot{\mathcal{R}}=0$, eliminating the propagating scalar degree of freedom at linear order. This exact result clarifies that the generalized slow-roll treatment should be interpreted as an effective softly constrained description. We also discuss perturbative stability conditions, including the positivity of the relevant kinetic coefficients and propagation speeds. Our results demonstrate that the effective constrained scalar--Gauss--Bonnet framework provides a flexible and observationally viable description of inflation while clarifying the distinction between the exact constrained limit and its effective slow-roll realization.
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physics.gen-ph 2026-05-27

One guided tour gathers math for spacetime and entanglement

by Johanna Barzen, Frank Leymann

Mathematics of Spacetime: A Guided Tour Through The Underlying Differential Topology and Differential Geometry

It consolidates differential topology and geometry to support general relativity and ER=EPR models without multiple textbooks.

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Background in General Relativity (e.g. black holes, wormholes, or spacetime models in general) is needed to comprehend more recent efforts around understanding quantum phenomena like entanglement (e.g. >>It from qubit<< as well as >>ER = EPR<<). The former in turn requires a lot of knowledge from differential topology and differential geometry. While this knowledge is available in very good mathematics textbooks, it is scattered i.e. quite a bunch of sources need to be consulted to acquire it. The goal of this contribution is to provide the major background in a single place; in this sense, this contribution is some sort of guided tour through the corresponding literature.
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physics.gen-ph 2026-05-27

Spin-3/2 field isolated by separating spin-1/2 sector

by Ion I. Cotaescu

Covariant field with unique mass and spin 3/2

Reducible (1,0)⊗(1/2,0) yields pure eight-component (3/2,0)⊕(0,3/2) theory with unique mass and spin

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We present the explicit theory of eight-dimen\-sional massive covariant fields with single spin $\frac{3}{2}$ transforming according to the representation $(\frac{3}{2},0)\oplus(0, \frac{3}{2})$ of the group $SL(2,\mathbb{C})$. This is done starting with the reducible representation $(1,0)\otimes(\frac{1}{2},0)$ instead of the irreducible one $(1,\frac{1}{2})=(1,0)\otimes(0,\frac{1}{2})$ we meet in Rarita-Schwinger or Joss-Weinberg frameworks. The resulting $12$-component covariant field transforming according to the representation $[(1,0)\otimes(\frac{1}{2},0)]\oplus [(0,1)\otimes(0, \frac{1}{2})]$ is maximally reducible, up to subspaces of irreducible representations of the $SU(2)$ group. Consequently, after building the theory in direct product basis of the representation $(1,0)\otimes(\frac{1}{2},0)$, the sector of spin half can be separated revealing thus the genuine $(\frac{3}{2},0)\oplus(0, \frac{3}{2})$ field. In this manner the theory of massive field of single spin $\frac{3}{2}$ can be developed naturally from the field equation and associated matrices, Lagrangian formalism and inner product up to closed expressions of orthonormal mode spinors.
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physics.gen-ph 2026-05-26

R² term completes stability check for cubic gravity de Sitter

by Tuan Q. Do

Effect of R² on the stability of de Sitter solution of the generalized Einsteinian cubic gravity

Only the P interaction sets the de Sitter value; adding Starobinsky R² supplies the missing perturbation equations without altering it.

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In this paper, we would like to investigate whether a generalized Einsteinian cubic gravity, in which three possible cubic interactions ${\cal P}$, ${\cal C}$, and ${\cal C}'$ are treated on an equal footing, admits a de Sitter solution as its stable cosmological solution. As a result, we are able to confirm the existence of the corresponding de Sitter solution for this gravity by solving analytically its field equations. Remarkably, only the cubic interaction ${\cal P}$ gives rise to the existence of the de Sitter solution. Then, we convert the field equations into the corresponding dynamical system for a stability analysis purpose. A fixed point of this dynamical system is found and shown to be equivalent to the obtained de Sitter solution. However, the perturbed dynamical system turns out to be incomplete, leaving undetermined information of the stability of the fixed point (or equivalently the de Sitter solution). Fortunately, we show that this loophole can be cured once the well-known Starobinsky term $R^2$ is introduced into the action of the generalized Einsteinian cubic gravity, despite the fact that it contributes nothing to the value of the de Sitter solution.
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physics.gen-ph 2026-05-25

Hawkes processes stay stationary at criticality under heavy fertility tails

by Didier Sornette

Critical Hawkes Processes with Random Fertilities: Stationarity in Law Beyond Infinite Mean Activity

Infinite mean activity no longer blocks stationarity when fertility exponent lies between 1 and 2 and memory tails decay slower than fertili

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Genuinely critical dynamics have been proposed to organize many natural and social systems, yet exact criticality is usually thought to preclude stationarity because the mean activity diverges. I show that this conclusion is not generally valid for self-exciting Hawkes point processes. At criticality, stationarity in law is controlled not by the mean intensity, but by local finiteness of the infinite-past Poisson-cluster construction. The relevant object is the fixed-window hitting probability \(H_T(u)\), the probability that a cluster born at time \(-u\) contributes at least one event to a window of length \(T\). For memory tails \(\mathbb{P}(T>t)\sim t^{-\theta}\) and fertility tails \(\mathbb{P}(\kappa>x)\sim x^{-\gamma}\), I prove stationarity for \(1<\gamma<2\) and \(\theta>\gamma\) via a finite-mean-lifetime criterion. In the finite-memory, finite-variance regime, \(H_T(u)\) is asymptotically comparable to the cluster-survival probability, and the exact local-finiteness condition fails. A direct asymptotic analysis of \(H_T\) gives the sharper condition \(\theta>\gamma-1\) for stationarity to hold in the infinite-fertility-variance regime. Thus broad fertility fluctuations can stabilize critical Hawkes dynamics in law, producing locally finite stationary sample paths despite infinite mean activity.
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physics.gen-ph 2026-05-21

Single f(Q) model covers inflation and late acceleration

by Moli Ghosh, Can Aktas +1 more

Unified Cosmological Scenario in Holographic f(Q) gravity: From Inflation to Late-Time Acceleration

Power-law f(Q) with Barrow fluid reconstructs Hubble to match Planck early and CC+BAO late while staying close to LambdaCDM at low redshift.

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The present paper reports a study of a unified cosmological scenario in the framework of holographic f(Q) gravity, where, in a single theoretical setup, both the early inflationary epoch and the late-time accelerated epoch are studied. Considering f(Q) = $\zeta Q^n$, we reconstruct the Hubble parameter in the presence of Barrow holographic fluid and study the inflationary behaviour through the slow-roll parameters, scalar spectral index $n_s$, and tensor-to-scalar ratio r. The obtained inflationary predictions are found to be consistent with the latest Planck 2018 observational constraints, with a very small value of the tensor-to-scalar ratio. In the next phase, we extend the study by including the matter sector. The Chevallier-Polarski-Linder (CPL) parametrization is used to connect the theoretical model with observational cosmology. Using combined Cosmic Chronometer (CC) and Baryon Acoustic Oscillation (BAO) datasets, the study constrains the model parameters through Markov Chain Monte Carlo (MCMC) analysis. From the observational results obtained this way, the study concludes that at low redshifts, the holographic f(Q) model considered here remains compatible with the standard LambdaCDM model, while mild deviations are observed at higher redshift. We have also performed the AIC and BIC analysis and commented on the goodness of fit in comparison with the LambdaCDM model. Hence, the present framework provides a viable unified description of inflation and late-time cosmic acceleration within holographic f(Q) gravity.
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physics.gen-ph 2026-05-20 2 theorems

Modified coupling rescales London depth by 1/√2 in bosonic superconductors

by F. Minotti, G. Modanese

Beyond minimal coupling for charged scalars? Modified electrodynamics and London-penetration tests

Independent optical and magnetic measurements in Nb and YBCO show a ratio near 1.4, matching the prediction while standard theory expects 1.

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While standard minimal coupling works well for Dirac fermions, its application to scalar fields features a known ``peculiarity'': the term linear in $A_\mu$ does not coincide with the conserved Noether current of the interacting theory. We recently proposed choosing a different principle for electromagnetic interactions, namely a linear coupling $A_\mu J^\mu$ with $J^\mu$ a (globally) conserved current, accepting the consequence that one must abandon full local gauge invariance in the electromagnetic sector and adopt an extended electrodynamics (of Aharonov--Bohm type) that can couple consistently to non-locally-conserved currents. We present the physical motivations offered for proposing the modified coupling and discuss general consequences of reducing gauge invariance. We then focus on the central condensed-matter claim: for bosonic charged condensates, the modified framework predicts a rescaled magnetic penetration depth $\lambda \to \lambda/\sqrt{2}$, while leaving other key qualitative features of superconducting electrodynamics and the type-I/type-II distinction unchanged (up to an equivalent rescaling of the GL parameter). Finally, we analyze experimental data for a London-length consistency check based on independent measurements of the ratio $n_s/m^\ast$ between carrier density and effective mass. We compare for five materials an ``optical'' penetration depth $\lambda_{\mathrm{opt}}$ inferred from IR/THz superfluid spectral weight with a ``magnetic'' depth $\lambda_{\mathrm{mag}}$ obtained independently (LE-$\mu$SR, TF-$\mu$SR, microwave methods, etc.). Data for Nb, YBCO and Ba(Fe,Co)$_2$As$_2$ confirm the hypothesis $\lambda_{\mathrm{opt}}>\lambda_{\mathrm{mag}}$, with a ratio not far from 1.4; data for Pb are inconclusive while data for MgB$_2$ indicate $\lambda_{\mathrm{opt}}\simeq\lambda_{\mathrm{mag}}$ as predicted by the standard theory.
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physics.gen-ph 2026-05-19 2 theorems

Fine-structure constant form follows from dimensional analysis

by Robi Banerjee

Gravity, Fine-Structure Constant and Natural Units -- some Thoughts based on Dimensional Analysis --

Linking three dimensions to G, c, ħ and e fixes its structure and sets gravity apart from quantum effects.

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Here we discuss direct links of the number of fundamental dimensions to the fundamental natural constants using simple arguments of dimensional analysis \corr{based on Maxwell's dimensions length (L), time (T) and mass (M) as well as the constants $G$, $c$, $\hbar$ and $e$}. We find that the \corr{form} of the fine-structure constant is a direct consequence of this connection. Additionally, our approach emphasises that gravity is a quite distinct area of physics which is not yet successfully quantised, i.e. not yet combined with quantum mechanics. We also discuss different unit systems based on dimensional analysis and natural constants.
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physics.gen-ph 2026-05-19

q-screened potential sets ionization temperature threshold in plasmas

by Abdelmalek Boumali

Non-Extensive Generalization of Double Ionization by Electron Impact: Calculations of Both Cross Sections and Rate Coefficients for H^-, He, and Li^+

Generalized Born treatment for H^-, He and Li^+ yields rate coefficients that vanish below a subextensive critical temperature.

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We generalize Tweed's seminal Born~I formalism for the electron-impact double ionization of two-electron atomic systems ($\text{H}^-$, $\text{He}$, $\text{Li}^+$) to non-extensive plasma environments described by Tsallis $q$-statistics. The bare Coulomb interaction is replaced by a $q$-deformed screened potential, which introduces a unique form factor envelope into the momentum-transfer integrations. We rederive the differential, partial, and total cross sections, demonstrating that this screening regularizes the classical high-energy Bethe logarithm and, in the $q < 1$ regime, induces diffraction-like oscillations in the angular cross sections. The model is calibrated against digitized historical experimental data to quantify how non-extensive screening deforms the vacuum baseline. Finally, coupling these cross sections to a $q$-Maxwellian distribution yields the macroscopic rate coefficients and reveals a novel subextensive critical-temperature threshold below which ionization is energetically forbidden.
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physics.gen-ph 2026-05-19 2 theorems

EV charger optimization scores 0.28 versus 0.65 for actual builds

by Yiwu Hao, Hong Yuan +2 more

Synergetic capacity planning of private and public EV charging piles via city-scale multiobjective optimization

Chongqing model projects 1.8 million units by 2030 to hold a 9:1 private-to-public ratio and reduce core-to-exurban gaps

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Rapid electric vehicle (EV) expansion necessitates optimized charging infrastructure to bridge the persistent gaps between vehicle growth and charger availability. This study develops a demand-driven framework for city-scale EV charging demand assessment and charging pile capacity planning. It employs a bottom-up estimation approach to quantify electricity demand and a Harris Hawks Optimization algorithm to solve capacity planning challenges, capturing spatiotemporal demand variations across powertrain types and guiding allocation over 2022-2030 in Chongqing, China. The results show that (1) compared with June 2022, monthly EV electricity consumption tripled to 57.5 gigawatt-hours by the end of 2024, characterized by significant seasonal volatility and a structural shift in which the combined share of plug-in hybrid electric vehicles and extended-range electric vehicles reached 57.6%, necessitating a transition toward technology-specific infrastructure planning; (2) historical evaluations reveal a marked spatial mismatch, with actual deployment heavily concentrated in the urban core while public charging capacity consistently lagging behind demand, whereas the proposed optimized configuration achieved a superior comprehensive performance score of 0.28, compared to 0.65 for actual deployment, in balancing service adequacy across the "Core-Suburban-Exurban" hierarchy; and (3) by 2030, Chongqing is projected to require approximately 1.8 million charging units to sustain a stable 9:1 private-to-public ratio, a synergetic strategy expects to significantly mitigate urban-rural service disparities and enhance overall system resilience and grid compatibility. Ultimately, this study provides a versatile, spatially explicit tool for policymakers to support sustainable and cost-effective EV infrastructure deployment aligned with long-term electrification targets.
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physics.gen-ph 2026-05-15 2 theorems

Spacetime emerges as spectral sets of functional operators

by S. Srednyak

Flat Bundles on Function Manifolds and Evolution Equations in Quantum Field Theories

Flat bundles on infinite-dimensional time manifolds make particle configurations arise from operator spectra in an extended quantization.

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In this paper we discuss extensions of the canonical quantization procedure in quantum field theories. We focus specifically on S-matrix representation as a T-exponent. This extension involves flat bundles on certain infinite dimensional functional manifolds of local time. The motivating problem is first principles treatment of bound states in quantum chromodynamics as well as precision physics of hydrogen atom and the muonium. Our main results include systematic treatment of flat bundles in an infinite dimensional setting, generalization of Hamiltonian evolution and functional renormalization group evolution equations in quantum field theories. We discuss several results from finite dimensional theory that have analogies in the functional setting. This includes construction of moduli space of flat connections and isomonodromic deformations. One of the outcomes of our analysis is a construction of a rich family of functional flat bundles with rational connections. This class of connections exhibits a rich set of mathematical properties. In particular, we construct examples of spaces fundamental groups of which have a definable continuum of generators. Physical states correspond to points in the moduli space of bundles on these spaces. On the physics side of things, we conclude that spacetime notions, such as spaces of particle configurations, emerge effectively as spectral sets of functional differential operators.
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physics.gen-ph 2026-05-13 1 theorem

Rotation curve of NGC 3198 fits traversable wormhole

by Saibal Ray Aritra Sanyal

Traversable Wormhole Geometry Reconstruction from the Rotation Curve of NGC 3198: A Comparative Study of Dark Matter Halo Profiles

Burkert dark matter profile gives best match to SPARC data and produces the clearest null energy violation near the center.

Figure from the paper full image
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We develop an observation-driven framework that reverses the standard wormhole approach: instead of assuming a Morris--Thorne traversable wormhole geometry and deriving the supporting matter, we reconstruct the wormhole metric directly from the observed rotation curve of the spiral galaxy \mbox{NGC\,3198}. Using SPARC data ($D=13.8\,\mathrm{Mpc}$; 43 measurements over $0.32$--$44.08\,\mathrm{kpc}$), we fit four dark-matter halo profiles -- Hernquist, Navarro--Frenk--White (NFW), Burkert, and Einasto -- through $\chi^2$ minimisation with the Nelder--Mead algorithm. For each best-fit density profile $\rho(r)$, the redshift function is reconstructed from the circular geodesic relation $f'(r)=v^2(r)/r$, while the shape function follows from the Einstein field equations, $b'(r)=8\pi G\rho(r)r^2/c^2$. We define the dimensionless wormhole indicator $\mathcal{W}(r)=b(r)/r$ and evaluate it across the observed galactic domain. All four profiles satisfy $\mathcal{W}(r)\ll1$, implying that the observed region lies entirely within the traversable exterior of the reconstructed wormhole geometry. The flare-out condition $b'(r)<1$ is satisfied everywhere by several orders of magnitude. The cored Burkert and Einasto profiles exhibit null energy condition (NEC) violation near the galactic centre, indicating effective exotic matter compatible with wormhole support, whereas the cuspy Hernquist and NFW profiles preserve the NEC. Among all models, the Burkert profile provides the best fit ($\chi^2_{\rm dof}=2.545$), the largest wormhole indicator ($\mathcal{W}_{\max}=5.62\times10^{-7}$), and the strongest NEC violation, suggesting that the observationally favoured dark-matter distribution can also sustain a traversable wormhole. These results establish galactic rotation curves as a potential observational probe of wormhole physics.
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physics.gen-ph 2026-05-11 2 theorems

Amplitude profile mediates link between Bohm potential and scalar EM mode

by R. Pullano, G. Modanese

A Structural Link Between the Bohm Quantum Potential and the Scalar Mode of Aharonov-Bohm Electrodynamics in a Bosonic Schr\"odinger Model

Boundary conditions in the bosonic model turn the shared dependence on R into a functional relation between the quantum potential and the Ah

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We discuss a formal and physical connection between the Bohm quantum potential and the scalar mode of the Aharonov-Bohm extension of electrodynamics. The analysis is motivated by the effective non-relativistic bosonic model recently proposed by Minotti and Modanese, in which the electromagnetic field is coupled to a conserved current while the field equations contain an additional source term. In the Madelung representation $\psi=R\exp(i\theta/\hbar)$, the Bohm quantum potential $ Q_B=-\frac{\hbar^2}{2m}\frac{\nabla^2 R}{R} $ is determined by the relative curvature $\nabla^2R/R$ of the amplitude profile $R$. In the same bosonic model, the scalar electromagnetic mode $S=\partial_\mu A^\mu$ is sourced by the extra-current $I=\partial_\mu j^\mu$, which contains the density-weighted electromagnetic combination $\nabla\cdot(R^2\mathbf A)$. Thus $Q_B$ does not act as a direct source of $S$; rather, the two quantities probe different differential aspects of the same amplitude profile: $Q_B$ is sensitive to the relative curvature of $R$, whereas the source of $S$ is sensitive to its density and gradient content through $R^2$ and $\nabla R$. We show that, once boundary and normalization data are fixed, this observation may be written as a mediated functional dependence of $S$ on $Q_B$ through $R$. We also clarify the physical status of $Q_B$: although it is state-dependent and should not be interpreted as an autonomous external potential, its density-weighted integral gives the amplitude-gradient energy, equivalently a Fisher-information contribution. This makes $Q_B$ a compact diagnostic of quantum pressure, rigidity, and inhomogeneity of a bosonic condensate. The resulting link with $S$ is therefore best understood as a structural relation between the order-parameter amplitude profile of the condensate and the scalar sector of the extended electromagnetic theory.
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physics.gen-ph 2026-05-11 2 theorems

Neural net data flip suggests closed universe with evolving dark energy

by D. Revanth Kumar, Santosh Kumar Yadav

Constraining Dark Energy Dynamics in Curved Spacetime with Current Observations

Reconstructed Hubble and supernova data push the dark energy parameter farther from a constant and change the sign of spatial curvature.

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We investigate a dark energy (DE) equation of state (EoS) parametrization in a curved spacetime using current observations. We constrain the model parameters by using observational Hubble data from Cosmic Chronometer (CC), Pantheon Plus SH0ES (PPS), and DESI BAO DR2, along with their reconstructed datasets using an Artificial Neural Network (ANN). The parameter $\alpha$ is constrained as $\alpha \approx 0.35 (\approx 0.56)$ from original (reconstructed) data. This means reconstruction pushes the model toward a significant deviation from the standard $\Lambda$CDM framework. We find that the curvature parameter $\Omega_{k0} = 0.068 \pm 0.029$ at 68\% CL with original data, suggests a slightly open universe, whereas with the reconstruction method, $\Omega_{k0} = -0.131 \pm 0.032$ at 68\% CL suggests a closed universe. This shift in the mean value indicates that the reconstruction method is highly sensitive to curvature. We perform statistical model comparison criteria, namely, AIC and BIC to assess the reliability of our framework.
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physics.gen-ph 2026-05-07

Quantum collapses may violate local charge conservation

by F. Minotti, G. Modanese

Quantum collapse, local conservation of charge, and possible experimental consequences

Aharonov-Bohm electrodynamics describes the fields, and diode detectors could register signals from state reductions.

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We investigate the possibility that idealized quantum state-reduction processes may produce a local violation of charge conservation. If this occurs, the corresponding electromagnetic fields cannot be consistently described within Maxwell electrodynamics, and a natural alternative is provided by Aharonov-Bohm electrodynamics, which reduces to Maxwell theory when local charge conservation holds, but remains compatible with non-conserved sources. Within this framework we first analyze how state reduction may generate non-conserved local currents, including statistically compensated cases and biased tunnelling configurations with persistent average current. We then study the interaction of gauge waves with fermionic and bosonic quantum systems, the latter being described by a modified Schr\"odinger equation previously proposed for boson matter. As an application, we discuss the interaction of gauge waves with superconductors and show that they can effectively shield such waves. Finally, we present experimental proposals based on inverse-biased diodes and estimate the expected detector response.
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physics.gen-ph 2026-05-06

Mixed interaction lets fractional dark energy trace full cosmic history

by Qihong Huang, Hao Chen +1 more

Observational Constraints and Cosmological Dynamics of Interacting Fractional Holographic Dark Energy in Light of DESI DR2

Phase space analysis shows only the Q=βHρ_m+γHρ_de term connects early matter era to late acceleration while fitting data.

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Based on the fractional entropy originating from fractional quantum mechanics, the fractional holographic dark energy (FHDE) model has been proposed. In this paper, we consider an interaction between the pressureless matter and FHDE and analyze three different interacting FHDE models. Combining the latest observational data including SNIa, OHD, BAO, and CMB, we estimate the model parameters and find that the interaction forms $Q=\gamma H \rho_{de}$ and $Q=\beta H \rho_{m}+\gamma H \rho_{de}$ show some preference from the observational data. Using phase space analysis, we further find that only interacting FHDE model with $Q=\beta H \rho_{m}+\gamma H \rho_{de}$ can describe the full evolutionary history of the universe. The statefinder diagnostic pair reveals that this model deviates from the $\Lambda$CDM model but converges to the $\Lambda$CDM fixed point and the de Sitter expansion fixed point in the future. Finally, we analyze the evolution of cosmological parameters and demonstrate that this model can drive the late time acceleration of the universe.
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physics.gen-ph 2026-05-05 2 theorems

Arrow of time emerges from confinement-deconfinement transition

by Deepak Vaid

Gauging Time Reversal Symmetry in Quantum Gravity: Arrow of Time from a Confinement--Deconfinement Transition

A Z2 gauge theory on spin networks creates a deconfined phase that carries a uniform cosmological arrow of time with topological protection.

Figure from the paper full image
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The question of the origin of time's arrow is a major outstanding problem in physics. Here we present a mechanism for the emergence of a cosmological arrow of time from a confinement--deconfinement transition in a $ Z_2 $ lattice gauge theory living on the spin-network states of Loop Quantum Gravity. Following Chen and Vishwanath \cite{Chen2015Gauging}, who showed that time-reversal symmetry can be gauged on tensor network states, and using the spin-network/tensor-network correspondence \cite{Qi2013Exact,Han2016Loop}, we introduce a $ Z_2 $ gauge field on spin networks encoding a local time-reversal symmetry. The effective theory of this gauge field contains a confined phase -- corresponding to a pre-geometric ``quantum gravitational foam'' with no coherent arrow of time -- and a deconfined phase -- corresponding to semiclassical spacetime with a uniform cosmological arrow. The emergence of the arrow of time is identified with the confinement--deconfinement transition, detected by the Wilson loop order parameter. The deconfined phase is further shown to correspond to a symmetry-protected topological (SPT) phase of the CZX type, whose topological order provides additional stability of the coherent time orientation against local perturbations. We conjecture that the topologically protected surface excitations of this SPT phase give rise to fermionic matter degrees of freedom.
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physics.gen-ph 2026-05-05

Phase accumulation derives time dilation and energy-momentum

by Emiliano Puddu

Special Relativistic Kinematics from Wave Phase Coherence

Invariant phase counts along trajectories produce the Minkowski interval and mass-frequency link from wave coherence alone.

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We present a phase-based formulation of special relativity in which the kinematical structure of the theory is reconstructed from the requirement of phase coherence of localized wave states. Starting from the assumption that physical propagation is associated with surfaces of constant phase and that matter admits an intrinsic rest-frame oscillation, we show that the relativistic relations for time dilation, energy, and momentum follow from the invariant accumulation of phase along particle trajectories. In this framework, proper time is identified operationally as the phase count of an internal clock, and the Minkowski interval arises as the quadratic form consistent with phase invariance across inertial observers. The relation between mass and rest-frame frequency emerges naturally, providing a unified interpretation of relativistic kinematics in wave-mechanical terms. This formulation does not introduce new dynamics but offers a coherent structural perspective that bridges relativistic kinematics and wave propagation.
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physics.gen-ph 2026-05-04 3 theorems

Thermodynamics distinguishes Newtonian gravity energy densities

by R. Trasarti-Battistoni, M. Pszota +1 more

On the energy balance of Newtonian Gravitation

Three formulas give identical energy balances and boundary conditions but differ in thermodynamic consistency.

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It is shown that the energy density formulas of Newtonian gravity by Maxwell, Bondi and Ohanian cannot be distinguished by boundary conditions, and also the corresponding energy balances are identical. However, they are not equivalent. From a thermodynamic point of view, the Ohanian energy density is distinguished.
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physics.gen-ph 2026-05-04

Narrowing KLJN resistor gap cuts attack success to 0.7

by Mehmet Yildirim, Laszlo B. Kish

Binary Classifier Wire-Resistance Attack on KLJN: Impact of Narrowing the Resistor Gap

Simulations show noise-voltage clouds overlap more as high and low values approach each other, limiting eavesdropper recovery.

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It is shown that narrowing the difference between the high and low resistor values in the Kirchhoff Law-Johnson Noise (KLJN) key exchange strongly affects security against a recently introduced binary classifier-based wire resistance attack. Using time domain simulations of a non-ideal KLJN loop with finite cable resistance, we generate large ensembles of secure (HL/LH) bits and evaluate the mean-square noise voltages at Alice's and Bob's ends. For each bit, these mean-square values form a point in a two-dimensional classifier plane, where the separation between the HL and LH point clouds characterizes the information available to an eavesdropper (Eve). We quantify Eve's success probability p by a simple decision rule based on the sign of the difference between the measured mean-square voltages. For strongly asymmetric resistors (for example RL = 4 kOhm and RH = 10 kOhm) and realistic wire resistances, the HL and LH clouds are fully separable and Eve's p approaches 1, which confirms that the classifier attack can practically recover all secure bits. As the low resistor value approaches the high one (for example RL = 9 kOhm and RH = 10 kOhm) at the same cable resistance, the HL and LH clouds increasingly overlap, and the measured p drops close to 0.7, approaching the ideal limit p = 0.5 as RL approaches RH. A surprising phenomenon is that, in this classifier-based scenario, increasing the wire resistance can decrease the information leak. This counterintuitive effect is strikingly the opposite of the behavior in the classical Bergou-Scheuer-Yariv wire resistance attack, where the mean-square voltages at the two ends of the wire are simply compared.
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physics.gen-ph 2026-04-30

Orbital compute needs launch costs cut by factor of ten

by Slava G. Turyshev

Orbital Data Centers: Spacecraft Constraints and Economic Viability

At 40 kg per kW the allowed budget is 250-1000 dollars per kilogram before communications and lifetime penalties begin.

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Orbital data centers are being evaluated as solar-powered compute constellations and relay-integrated processing platforms. Their feasibility is not set by orbital solar flux alone, but by simultaneous closure of photovoltaic generation, eclipse recharge, radiative heat rejection, sustained space-to-ground communications, utilization, replacement cadence, and delivered compute-years over finite mission life. This paper derives necessary cluster-level competitiveness conditions using delivered information-technology (IT) electrical power $P_{\rm IT}$, deployed mass per delivered IT power $m_{\rm kW}$ in kg/kW, communication intensity $\Gamma=D_{\rm sg}/E_{\rm IT}$, sustained communication ceiling $\Gamma_{\max}$, effective utilization $U_{\rm eff}$, and lifetime penalty $\Pi_{\rm life}$. For a representative $P_{\rm IT}$=1 MW high-sunlight anchor, the base case gives beginning-of-life photovoltaic area $A^{\rm BOL}_{\rm PV}=5.64 \times 10^3 {\rm m}^2$, radiator area $A_{\rm rad}=2.50 \times 10^3 {\rm m^2}$, and 29.4 kg/kW for photovoltaic, storage, and radiator mass; fixed spacecraft mass raises the total to 34-59 kg/kW. At m_kW ~ 40 kg/kW, a terrestrial infrastructure benchmark of 10-40 k\$/kW allows only 250-1000 \$/kg for the combined launch and spacecraft-build cost before space-to-ground communications, operations, utilization, and lifetime terms are included. That allowance is 3.4-13.5 times below the current public Falcon 9 dedicated low-Earth-orbit launch-price benchmark alone, before spacecraft build is included. Space-native preprocessing and communications-integrated edge compute are credible early regimes; terrestrial-user general compute closes only for low Earth-coupled communication intensity, high effective utilization, long delivered lifetime, and very low combined launch-plus-build cost.
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physics.gen-ph 2026-04-30

Rényi entropy yields dark energy matching Planck data

by S. I. Kruglov

The R\'{e}nyi entropy and entropic cosmology

Modified apparent horizon entropy produces a model where matter density and deceleration match observations and Hubble rates agree within 5%

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Entropic cosmology with the R\'{e}nyi entropy of the apparent horizon $S_R=(1/\alpha)\ln(1+\alpha S_{BH})$, where $S_{BH}$ is the Bekenstein--Hawking entropy, is studied. By virtue of the thermodynamics-gravity correspondence a model of dark energy is investigated. The generalised Friedmann equations for the Friedmann--Lema\^{i}tre--Robertson--Walker spatially flat universe with the barotropic matter fluid are obtained. We compute the dark energy density $\rho_D$, pressure $p_D$ and the deceleration parameter $q$ of the universe. At some model parameters the normalized density parameter of the matter $\Omega_{m0}\approx 0.315$ and the deceleration parameter $q_0\approx -0.535$ for the current epoch, which are in the agreement with the Planck data, are found. Making use of the thermodynamics-gravity correspondence, we describe the late time of the universe acceleration. The entropic cosmology considered is equivalent to cosmology based on the teleparallel gravity with the definite function $F(T)$. The Hubble parameters are in approximate agreement (within $5$ percents) with the observational Hubble data for redshifts $0.07\leq z \leq 1.75$ at the entropy parameter $\alpha\approx 0.305~GH_0^2$.
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physics.gen-ph 2026-04-29

Projective limits turn local pairwise comparisons into global relational structures

by Jean-Pierre Magnot

Pairwise-comparison-valued cosurfaces: a projective framework for multi-scale relational structures

Global coherence is recovered solely from compatibility of comparison data across ordered refinements of finite discretizations.

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We introduce cosurfaces with values in the group \(\PC_n(H)\) of \(H\)-valued reciprocal pairwise comparison matrices. The composition law is covariant on upper triangular coefficients and contravariant on lower triangular coefficients, which makes \(\PC_n(H)\) a natural target for oriented gluing constructions. Starting from a directed family of finite oriented discretizations, we define finite configuration spaces, coarse-graining maps induced by ordered refinements, and the associated universal projective limit. This yields a multi-scale organization of local comparative data in which global objects are reconstructed only through compatibility across scales. In the stochastic setting, projectively compatible probability laws define a cylindrical semantics on the limit space. We also introduce inconsistency observables, interpreted as discrete curvature-type defects measuring obstructions to global coherence. The resulting framework is simultaneously geometric, algebraic, and probabilistic, and suggests a foundational perspective on relational structures built from local comparisons rather than absolute observables.
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physics.gen-ph 2026-04-28

Benchmark splits cross-section and EEDF effects on light-atom ionization

by Abdelmalek Boumali

Electron-impact ionization rates for neutral He, Li, and Be in the Tsallis framework

For He, Li, and Be the Bell-Lotz spread is small for helium but reaches 95 percent for lithium, while distribution tails scale with Ip overT

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The single-ionization rate coefficient of a plasma neutral depends both on the microscopic electron-impact cross section and on the macroscopic shape of the electron energy distribution function (EEDF). We present a reproducible benchmark and sensitivity study -- not a new theory -- of these two effects for the three lightest neutrals He, Li, and Be, combining the recommended Bell~\textit{et~al.}\ (1983) cross sections with a properly normalized two-temperature Tsallis $q$-generalized EEDF and varying $q$ on both sides of the Maxwellian limit and the hot-electron fraction $f_{\mathrm{hot}}$ at $T_{\mathrm{hot}}=10\,T_{\mathrm{bulk}}$. The calculation cleanly separates two independent uncertainty axes -- cross-section model (Bell vs.\ Lotz) and EEDF shape (Maxwellian vs.\ Tsallis). The Bell--Lotz spread on $\tau_M$ is small for He (within about $7\%$), moderate for Be ($\lesssim 17\%$), and largest for Li (up to $+95\%$ at $T=1$~keV); sub-extensive distributions ($q<1$) suppress ionization through a hard tail cut-off, while super-extensive distributions ($q>1$) enhance low-temperature ionization through a $\kappa$-like power-law tail with $\kappa=1/(q-1)$. The quantitatively safest non-Maxwellian cases are $q=1$ and $q=1.2$ ($\kappa=5$), which lie inside the finite-mean-energy regime; the cases $q=1.4$ and $q=1.6$ are retained as heavy-tail stress tests and should be read as qualitative trends rather than as quantitatively reliable predictions. Both EEDF effects scale with $I_p/k_BT$, so He responds most strongly and Li least. The full numerical pipeline is released as a persistent reproducibility package, intended as a drop-in non-Maxwellian ionization module for collisional-radiative and ionization-balance modelling of light-neutral plasmas.
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physics.gen-ph 2026-04-28

Galaxy evolution constrained by Wasserstein geometry and energy rules

by Tsutomu T. Takeuchi ((1) Nagoya University, (2) Institute of Statistical Mathematics)

A Measure-Theoretic Transport Formulation of Galaxy Evolution on the Galaxy Manifold: Geometric Constraints

Populations as measures evolve via transport and jumps, restricted by curvature bounds and free-energy dissipation rather than arbitrarily.

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We develop a measure-theoretic framework for galaxy evolution in which galaxy populations are described as probability measures on a state space. Galaxy evolution is represented as the time evolution of a measure $\nu_t$, governed by the sum of a continuous transport term and a jump operator. The transport term describes internal galaxy evolution, while the jump operator captures discrete events such as mergers and interactions, yielding a unified reaction--transport system on the space of measures. We further equip the space of probability measures with the Wasserstein distance and impose a curvature--dimension condition CD$(K,\infty)$ to reveal the geometric structure of the dynamics. In this setting, the transport term is interpreted as a gradient flow of a free-energy functional, whereas the jump operator generates nonlinear rearrangements induced by many-body interactions. In the low-density limit, these interactions reduce effectively to two-body processes, leading to a closed dynamical system. A central consequence is that galaxy evolution is not arbitrary, but constrained by a variational structure, curvature bounds, and an interaction hierarchy. Admissible trajectories are restricted by energy dissipation, geometric contractivity, and effective interaction closure. The framework also separates intrinsic galaxy dynamics from observational projection, treating observables as pushforwards of measures. It thus provides a unified foundation for structure formation and galaxy evolution as a geometrically constrained reaction--transport process.
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physics.gen-ph 2026-04-27

Clifford algebra with S3 symmetry fixes Yukawa matrix algebraically

by Niels Gresnigt

Higgs and Yukawa Structure in a Clifford Algebra Model with Three Generations and S₃ Family Symmetry

The model produces two Higgs doublets and a non-diagonal Yukawa matrix aligned with masses, preserving Type-II separation without tree-level

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We construct the Higgs and Yukawa sectors as a structural completion of an algebraic three-generation model based on the complex Clifford algebra $\mathbb{C}\ell(10)$ with an intrinsic $S_3$ family symmetry. This addresses a common limitation of algebraic frameworks, in which Standard Model fermion multiplets and gauge symmetries may be described naturally, while the Higgs and Yukawa sectors remain less developed or absent. In the present framework, three algebraically distinguished fermion sectors are permuted by $S_3$, while the Standard Model gauge generators remain generation-independent. Higgs components are realised as right-action operators mapping weak-doublet fermion sectors into the corresponding weak-singlet sectors, and Yukawa coefficients are extracted using a Hilbert--Schmidt trace pairing. This yields two first-generation Higgs doublets with electroweak quantum numbers $(1,2,-1)$ and $(1,2,+1)$ under $SU(3)_C \times SU(2)_L \times U(1)_Y$, together with a Type-II-like separation between down-type and up-type Yukawa channels. Acting with the order-three family generator then generates a family-resolved Higgs sector organised into cyclic $S_3$ orbits. In the cyclically averaged Higgs limit, the Type-II-like Yukawa selection rule is preserved, while the generation-space Yukawa matrix is fixed algebraically and is non-diagonal in the algebraic generation basis. Under the usual implementation of electroweak symmetry breaking, the neutral Higgs couplings are aligned with the corresponding mass matrices, so tree-level flavour-changing neutral currents are not expected in this limit. The result is a constrained algebraic starting point for future $S_3$-breaking flavour phenomenology.
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physics.gen-ph 2026-04-27

Einstein photon field fills space instantly

by Aleksandr Beilinson

The quantum mechanics of Einstein photons and generalized functions

Reinterpreting Majorana equations gives a generalized measure where the quantum field fills all space at once in evolution.

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The article consider an interpretation of Majorana equations as a quantum Lorentz covariant equations for the field of Einstein photon. A photon with "deinterlaced" spins (with diagonal Hamiltonian) is considered, its generalized Green function as a functional on finite test functions and its Schr\"{o}dinger equation are constructed. The generalized process corresponding to this Green function is continued to $\sigma$-additive quantum generalized measure on the space dual to the compact subspace of a photon paths in $L_{2}(-\infty,\infty)$. In this case, the filling of whole space by such quantum field instantly occurs in the evolutionary problem. The last part of the article gives the calculation of the "Casimir forces" arising in this field.
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physics.gen-ph 2026-04-27

Rotating frames create effective source for Aharonov-Bohm scalar effects

by A. Iadicicco, G. Modanese +1 more

Effective Observer-Split Source Terms in Rotating Frames and Gravitomagnetic Backgrounds in Extended Aharonov-Bohm Electrodynamics

A 3+1 decomposition of conserved currents yields a term that drives phenomenological models at macroscopic scales with reversal under sign(Ω

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We examine whether rotating frames and stationary gravitomagnetic backgrounds can provide a meaningful link to extended Aharonov-Bohm electrodynamics without invoking microscopic charge non-conservation. For standard generally covariant, locally $U(1)$-invariant matter, the answer at the microscopic level is negative: the physical four-current remains covariantly conserved, so neither rotation nor stationary gravitomagnetism by themselves generate a genuine source for the scalar sector. A weaker but still useful connection nevertheless emerges after a $3+1$ decomposition with respect to a rotating observer congruence. In that description, the observer-measured transport current on the spatial slice obeys a projected continuity equation containing an exact split source term $I_{\mathrm{split}} \equiv \frac{1}{N} D_i(\rho\,\beta^i)$, which reduces in the weak-field regime to $I_G = D_i(\rho\,\beta^i)$. This term is not a frame-independent microscopic anomaly; it is the bookkeeping term that appears when covariant conservation is rewritten in transport variables adapted to a rotating slicing. We then propose a phenomenological AB-type closure in which this split source drives the scalar sector on finite-scale rotating systems. In the rigid-rotation weak-field limit, the source reduces to $I_G = (\boldsymbol{\Omega} \times \mathbf{r})\cdot \nabla \rho$, and for localized transients to $ I_G = \Omega\partial_\phi (\delta\rho_s)$. The resulting framework is therefore effective rather than fundamental, observer-tied rather than local-inertial, and experimentally meaningful only at mesoscopic or macroscopic scales. It yields concrete operational signatures, including reversal under $\Omega \to -\Omega$, suppression for nearly axisymmetric charge distributions, and sensitivity to transient non-axisymmetric charge structure.
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physics.gen-ph 2026-04-22

Hadrons follow Regge-like paths with variable mass

by Damianos Iosifidis

Novel Regge-like trajectories for spinning, dilating, hadronic particles

Spinning dilating particles have dynamical mass tied to dilation and shear currents rather than fixed rest mass.

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We study the of motion of a spinning, dilating particle with hadronic properties moving on a generic geometric background including curvature, torsion, and nonmetricity. In particular, we discuss generalized spin supplementary conditions and also introduce the concept of a shear supplementary condition. Using these, we investigate the evolution of the dynamical mass of the microstructured test body and the cases where the latter is a constant of motion. In general, we find novel Regge-like trajectories relating the mass to the dilation and/or the shear currents of hypermomentum. This means that for particles with hadronic properties, the rest mass is not a constant of motion in general.
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physics.gen-ph 2026-04-22

Classical fluid splitter reproduces quantum Bell violations

by Ghenadie N. Mardari

Quantum Correlations in Classical Systems

Molecular paths show rotationally invariant and cosine-squared correlations matching Stern-Gerlach devices, allowing Tsirelson-type outcomes

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A classical fluid splitter produces the same patterns of energy redistribution as a Stern-Gerlach quantum device, with rotationally invariant coefficients of correlation between molecular paths. Alternative settings express a cosine squared relationship, leading to Tsirelson-type Bell violations with outcome independence. This result confirms the Correspondence Principle of quantum mechanics, where individual detection events express system-level properties according to Born's Rule. Kochen-Specker contextuality and Bell Locality are not formally contradicted, but their interpretation is in question. Current definitions of Local Realism are limited to intrinsic particle properties. In contrast, quantum-like correlations require the acknowledgement of ensemble effects on dynamically inseparable entities, even when those entities are observed one at a time.
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physics.gen-ph 2026-04-21

One conductance quantum covers electric

by Lino Reggiani, Eleonora Alfinito +1 more

The fundamental units of generalized quantum conductance and quantum diffusion

A quasi-particle Drude model ties Planck's constant to a statistics-adjusted action and derives the same unit for all listed currents.

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Although quantum transport at the nanoscale has received widespread attention since Landauer's pioneering work in 1957, we remark, that a general theory that sheds light on the difference between classical and quantum relativistic physical models is still lacking. By considering a classical 3D gas of non-interacting quasi.particles, the article presents a unified theory that provides a generalized conductance of dimensionless quasi-particles, neutral massive, electric, thermal, and photon currents. The investigation begins with an analogy between the original Drude model of 1900 and a modified Drude model of quasi-particles, which includes a ballistic transport regime and is independent of statistics (excluding Bose-Einstein condensation). Next, we construct connections between the quasi-particle unit in the modified Drude model and the carrier unit in dimensionless, electric, massive neutral, phonon, and photon currents. By establishing a connection between Planck's constant $h$ and a classica\`o action that takes into account the correct statistics, $h_s$, we derive the fundamental quantum unit of conductance for any of the mentioned currents. We further extend the diffusion coefficient of quasi-particles from the classical regime to the quantum and relativistic regimes.
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physics.gen-ph 2026-04-21 Recognition

Radiation entropy keeps gravity in line with second law

by Jorge Pinochet, Giorgio Sonnino

Entropy, Gravity, and an Apparent Violation of the Second Law

Local structure formation under gravity is balanced by entropy exported in radiation and energy, as shown in Sun, black holes and collapsing

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An interesting question to explore in physics classes is whether gravity violates the second law of thermodynamics. Standard physics textbooks provide little to no discussion of the relationship between entropy and gravity, and the same is often true of specialized texts. The aim of this work is to address this question by analyzing the behavior of an ideal gas in two simple scenarios: one in which gravity is negligible and another in which its effects are significant. We show that although systems influenced by gravity may exhibit counterintuitive behavior, such as local ordering through structure formation, the second law of thermodynamics remains valid when the entire system is considered, including all emitted energy and radiation. Given the educational focus of this work and the complexity of the entropy-gravity relationship, we omit detailed calculations that are not strictly necessary and instead focus on the simplest physical scenarios. In this context, we analyze four representative examples through simple calculations: the Sun, the limit of extreme contraction in black holes, the protostellar contraction sequence, and core collapse with neutrino cooling.
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physics.gen-ph 2026-04-20

Linear superposition of metric deviations builds multi-source gravity

by Y. Friedman

Superposition Principle in Relativistic Gravity

The construction stays Lorentz covariant in flat spacetime and recovers standard GR tests for weak or slow sources.

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We develop a framework for superposition in relativistic gravity within Extended Relativity (ER), a Lorentz-covariant theory formulated in flat spacetime. In this approach, gravitational fields are described by deviations from the Minkowski metric associated with individual sources, and multi-source configurations are constructed through a superposition principle linear in the source parameters. The resulting metric preserves Lorentz covariance and reproduces the standard classical tests of General Relativity in the appropriate limits. We derive the explicit form of the superposed field for multiple moving sources and analyze its properties in both near and far zones. The formalism provides a consistent and physically transparent description of interacting gravitational sources and forms the basis for applications to relativistic dynamics and gravitational radiation.
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physics.gen-ph 2026-04-20

Relativistic action unifies gravity and electromagnetism

by Y.Friedman

A unifying physically meaningful relativistic action

It remains Lorentz covariant, reduces to the classical limit, and produces consistent equations for particles in combined fields.

Figure from the paper full image
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We introduce a relativistic action that provides a unified and physically meaningful description of particle dynamics in external fields. The proposed action is constructed to be Lorentz covariant and reduces to the standard classical action in the appropriate limit. It incorporates gravitational and electromagnetic interactions within a single framework and leads to equations of motion consistent with known physical laws. The formulation offers a new perspective on relativistic dynamics and suggests a pathway toward unification of fundamental interactions.
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physics.gen-ph 2026-04-20

Discrete Boltzmann factor suppresses black-hole luminosity near cutoff

by Abdelmalek Boumali, Yassine Chargui

Bounded thermal weights from a discrete Boltzmann factor

It shuts off the thermal Hawking channel and yields an exact work identity for deterministic protocols, recovering standard results as the b

Figure from the paper full image
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The discrete Boltzmann factor $B_E(\beta_n)=(1-bE)^n$, introduced by Chung, Hassanabadi, and Boumali, provides a lattice regularization of the canonical weight $e^{-\beta E}$ and imposes the compact-support condition $E<1/b$. In the present analysis we systematically separate results that follow directly from this bounded thermal weight from those that require additional phenomenological input. First, we study the discrete Bose--Einstein occupation factor relevant for Hawking radiation, derive the leading suppression of black-hole luminosity, and show that the thermal Hawking channel shuts off as the cutoff scale is approached. Second, we formulate a discrete work functional built from ratios of thermal weights and establish an exact Jarzynski-type identity for deterministic measure-preserving protocols; in contrast, the corresponding Crooks relation does not collapse to a function of work alone, and first-order approximations retain an explicit initial-energy dependence that cannot be reduced to a simple $W$-dependent correction without additional assumptions. Third, and purely as an ancillary kinematic extension rather than a derivation from the statistical framework itself, we examine a bounded modified-dispersion ansatz and estimate the associated time-of-flight constraints. Throughout, we include illustrative figures, clarify the non-universal status of the entropy correction, and emphasize that direct laboratory signatures are negligible whenever $b$ is universal and Planck suppressed. Finally, the standard continuum expressions are recovered smoothly in the limit $b\to 0$.
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physics.gen-ph 2026-04-20

Aharonov-Bohm theory keeps Maxwell energy spectrum despite non-conserved charges

by F. Minotti, G. Modanese

Fluctuations in Aharonov-Bohm Electrodynamics

Doubled electric energy is offset by negative scalar field; added violet noise appears in conductor fluctuations.

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We consider the application of the Fluctuation Dissipation Theorem (FDT) to the electrodynamics of Aharonov-Bohm (ABE), which differs from Maxwell's in that it allows for local non-conservation of charge. For the case of a system of non-conserved charges at thermal equilibrium we obtain the same spectral distribution of energy of the electromagnetic field as in Maxwell electrodynamics. However, the electric field contribution to that energy doubles that in Maxwell case, while the magnetic contribution is the same as in Maxwell theory, the electric excess energy is compensated by a negative contribution arising form the Aharonov-Bohm (AB) scalar field. For a conductor with local non-conservation of charge described by the $\gamma$ model, we derive the spectrum of current correlation at first order in $\gamma$, which results in a violet noise contribution added to the classical Johnson-Nyquist white noise result for the voltage fluctuations in a conductor.
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physics.gen-ph 2026-04-20

Decaying vacuum models fit DESI data with H0 near 73

by D. Revanth Kumar, Santosh Kumar Yadav +1 more

Observational tests of texorpdfstring{Λ(t)}{Lambda(t)} cosmology in light of DESI DR2

Joint analysis of supernovae, chronometers and BAO returns evolution parameter 0.3, showing a mild departure from constant vacuum energy.

Figure from the paper full image
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In this article, we investigate two phenomenological decaying vacuum cosmological models describing the accelerated expansion of the Universe. We constrain the model parameters using a Markov Chain Monte Carlo (MCMC) technique with recent datasets, including cosmic chronometer (CC), Pantheon+SH0ES (PPS), and DESI BAO data release (DR2). Our analysis provides constraints from PPS, PPS+CC, and the joint PPS+CC+DR2 datasets for both models. All datasets favor $H_0 \simeq 72.53$--$73.01~\mathrm{Km\,s^{-1}\,Mpc^{-1}}$, while $\Omega_{m0}$ is higher with PPS alone and decreases to standard paradigm estimates with the inclusion of additional data. The evolution parameter is $n \approx 0.30$ from joint analysis, indicating a mild deviation from the $\Lambda$CDM framework. Furthermore, the physical behavior of the models is examined through the deceleration parameter and the total equation of state, confirming a smooth transition from past deceleration expansion to the present accelerated expansion.
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physics.gen-ph 2026-04-17

Mass-center motion equations derived in scalar gravity theory

by Mayeul Arminjon

Equations of motion of the mass centers in a scalar theory of gravity with a preferred frame

Post-Newtonian integration inside bodies produces the center equations for the second version with a preferred frame.

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The theory considered interprets gravity as a pressure force. Thus, the scalar gravitational field defines the gravity acceleration field. However, it also determines the relation between the flat ``background metric'' and a curved ``physical metric''. Here we derive the equations of motion of the mass centers of a system of weakly gravitating bodies in the second version of that theory. We use the framework which was built and used for the first version. Namely, we use an asymptotic scheme of post-Newtonian (PN) approximation to derive the local (field) PN equations, and by integration inside the bodies we deduce from those local equations the equations of motion of the mass centers, using also an asymptotic framework for the good separation between the different bodies.
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physics.gen-ph 2026-04-15

Bessel beams carry finite OAM along light cones

by Felipe A. Asenjo, Swadesh M. Mahajan

Finite Orbital Angular momentum Bessel beams propagating along light-cone coordinates

Airy function products create asymmetric exact solutions to Maxwell's equations with nonzero orbital angular momentum density.

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New solutions for Bessel electromagnetic beams, propagating along the light cones, are investigated. Of the variety of structures possible in the light cone variables, the one involving a product of Airy functions is discussed in detail. This class of solutions, representing an asymmetry on the light-cone coordinates dependence, is a non-trivial extension to the usual plane wave solutions. We also explore the conditions under which these solutions will carry finite orbital angular momentum density.
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physics.gen-ph 2026-04-15

Lattice Universe model accounts for ANITA events naturally

by Massimo Villata

A possible solution to the mystery of the ANITA anomalous events

The upward radio pulses fit a symmetric cosmology that also explains accelerated expansion without dark energy.

Figure from the paper full image
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In 2006 and 2014, the Antarctic Impulsive Transient Antenna (ANITA), a balloon-borne radio observatory flying over Antarctica, detected two strange upward-going radio pulse events that have not yet been explained by our current understanding of physics. These were not signals reflected by the ice and therefore it must have been an air shower originating from a cosmic ray coming from under the Antarctic ice, but this hypothesis was also ruled out by various data analyses. The CPT gravity theory and its associated cosmological model, the lattice Universe, can instead explain those events in a completely natural and spontaneous way, without any additional assumptions beyond general relativity and the expected matter-antimatter symmetry of the Universe on which they are based. Together with the antihelium candidate events from AMS-02, the anomalous ANITA events can thus lend further validity to a cosmological model that has already achieved considerable success in explaining the accelerated expansion of the Universe, without the need for dark energy. These events thus add to a series of problems unsolved by standard cosmology and physics, but whose solution is straightforward, spontaneous and natural within the framework of CPT gravity, without the need for ad hoc hypotheses and unknown ingredients.
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physics.gen-ph 2026-04-15

Thermodynamics recovered when small-system group becomes irrelevant

by Amilcare Porporato, Lamberto Rondoni

Small-System Group: Thermodynamics as a Complete Self-Similarity Limit

Boltzmann's constant introduces Π_B in dimensional analysis; its irrelevance in the macroscopic limit yields standard thermodynamics while Π

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We revisit the Rayleigh--Riabouchinsky paradox in dimensional analysis by making explicit the bridge between thermodynamics and the mechanical interpretation of temperature. Boltzmann's constant $k_B$ acts as a dimensional unifier, leading to an augmented $\Pi$-theorem with an additional dimensionless group that encodes system size. In the macroscopic thermodynamic limit this small-system group, $\Pi_B = k_B/(c\,\ell^3)$ -- the inverse heat capacity of a control volume of size $\ell^3$ in units of $k_B$ -- becomes irrelevant as the response becomes self-similar with respect to it, recovering Rayleigh's formulation. Under suitable conditions, macroscopic limits make the fluctuations of the observables of interest negligible compared to their expected values, hence the state of a system is characterized by a reduced set of parameters. We thus recast thermodynamics as the complete-similarity limit of statistical mechanics with respect to $\Pi_B$, which also controls thermodynamic fluctuations. We also discuss second-order phase transitions from the viewpoint of incomplete similarity.
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physics.gen-ph 2026-04-14 3 theorems

Golden ratio governs quantum metric fluctuations at Mott points

by Zhanchun Li, Renwu Zhang

Quantum Geometry, Fractionalization, and Provability Hierarchy: A Unified Framework for Strongly Correlated Systems

Framework also restricts fractional charges to Fibonacci numbers and labels strange metals as unprovable problems.

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Mott physics - the interplay between itinerancy and localization of electrons - is undergoing a paradigm shift from the binary "bandwidth - filling" tuning framework to an intertwining of geometric, topological, and fractionalized degrees of freedom. Based on a series of breakthroughs in 2024 - 2025, this paper proposes five pioneering discoveries: (1) Prediction of the golden-ratio scaling of quantum metric fluctuations near the Mott critical point, supported by functional renormalization group arguments and DMRG numerical verification (phi = 0.618 +/- 0.005); (2) Establishment of a correspondence between the denominator q of fractional Chern insulator charge and the subgroup index of the quantum geometry group, predicting that allowed q values follow the Fibonacci sequence {2,3,5,8,13,...} with specific material realizations; (3) Proposal of the Provability Hierarchy Theorem, classifying critical states like strange metals as "true but unprovable" QMA hard problems, establishing a rigorous connection to the complexity of the Consistency of Local Density Matrices(CLDM) problem; (4) Prediction of interference oscillations in the nonlinear Hall conductance within the pseudo gap phase, induced by geometric phase differences, supported by tight-binding numerical simulations; (5) Unveiling the quantum geometric tensor as a unified descriptor of band geometry and topology. These findings provide an experimentally testable theoretical framework for understanding strongly correlated quantum materials.
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physics.gen-ph 2026-04-13

Planck data bound doubly logarithmic correction to radiation density

by Christian Balfagon

Doubly Logarithmic Corrections to Radiation Domination from CET {Ω}: Theory and Planck/BBN Constraints

Analysis shows the correction parameter is consistent with zero but limited to absolute value no larger than 0.006

Figure from the paper full image
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We present the CET Omega framework, a causal-informational extension of standard cosmology that predicts a universal doubly logarithmic correction to the radiation energy density in the early Universe. This correction arises naturally from scale-invariant spectral sectors with logarithmically-running infrared scales and represents a low-energy manifestation of the full CET Omega theory. We derive the doubly logarithmic form from two complementary perspectives -- spectral integration and renormalization group flow -- and perform a full Markov Chain Monte Carlo analysis jointly varying six LambdaCDM parameters and alpha_log, using Planck 2018 TT, TE, EE + lowE likelihoods and BBN constraints. The result, alpha_log = -0.008 +/- 0.006 (68\% C.L.), is consistent with zero. We identify the expected N_eff degeneracies with H0 and n_s, establish the first observational bound |alpha_log| <= 0.006, and demonstrate that future CMB-S4 measurements can probe |alpha_log| ~ 10^{-3}.
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physics.gen-ph 2026-04-09 2 theorems

Causality fixes inertial-frame transformations to Lorentz group plus dilatations

by Antonio Pineda

Relativity: A matter of causality

Defining spatial distance geometrically and requiring finite-time communication between observers yields the orthochronous inhomogeneous Lor

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We take causality and uniqueness of events observation as our driving forces. They are built in in the way we define distinct observers, which then require a finite time to communicate between each other. This unavoidably leads to the existence of maximal transfer-information velocity between arbitrary (not necessarily inertial) reference frames. Inertial reference frames are defined by fixing the geometrical properties of (spatial) distance without any reference to relativity, electromagnetism, or laws of physics in general. For these inertial reference frames, the causality condition fixes the causal group to be the orthochronous inhomogeneous Lorentz group times dilatations. The mathematics we will use are quite basic.
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physics.gen-ph 2026-04-09 Recognition

28th workshop continues discussions beyond standard models

by Norma Susana Mankoč Borštnik, Holger Bech Nielsen +2 more

Proceedings to the 28th Workshop What Comes Beyond the Standard Models

Since 1998 the series has favored open exchanges on high-energy physics, cosmology, and dark matter over formal presentations.

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This year was 28th time that our series of workshops entitled "What Comes Beyond the Standard Models?" took place. The series started in 1998 with the idea of organising a workshop where participants would spend most of the time in discussions, encompassing different approaches and ideas, from high energy to cosmology, dark matter physics, random dynamics, and discussions about the nature of spatial dimensions.
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physics.gen-ph 2026-04-08 1 theorem

Asymmetric gyration produces magnetic curvature drift

by Johnathan K. Burchill

What causes the magnetic curvature drift?

Field-direction rotation along the real path breaks gyration symmetry and yields the offset velocity without assuming the particle follows a

Figure from the paper full image
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When asked what causes the magnetic curvature drift of a charged-particle moving in a curving magnetic field, people respond that there is an `F-cross-B' motion of the `guiding center' due to the centrifugal force on the particle as it follows the magnetic field line. This and similar explanations `beg the question' by assuming that the particle follows the field line. In a curving magnetic field, however, a particle moving parallel to the field direction soon won't be. The convective rotation of the field along the particle trajectory ensures that the Lorentz force switches on, and the resulting acceleration rotates the velocity vector back into alignment periodically. The gyration is not symmetric about the field vector, and the resulting velocity offset is the curvature drift. This explanation is guided by Newton's second law of motion in vector notation. It provides a common framework for explaining the three guiding-center motions of a charged particle in a static nonuniform magnetic field: curvature drift, mirror reflection in a magnetic bottle, and gradient-B drift. The discussion aims to provide insight to instructors of electricity and magnetism or plasma physics at the intermediate- to advanced-undergraduate level.
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physics.gen-ph 2026-04-08 2 theorems

Black hole shadows depend on monopoles

by S. E. Baddis, A. Belhaj +3 more

On Computational CUDA Studies of Black Hole Shadows

CUDA ray tracing shows energy emission and silhouette size ignore the nonlinear parameter but yield EHT bounds on the other three quantities

Figure from the paper full image
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Combining high-performance CUDA numerical codes with the Hamilton--Jacobi formalism, we investigate the shadows properties of rotating charged Euler--Heisenberg black holes in the presence of global monopoles. Then, we discuss the associated energy emission rate by varying the involved black hole parameters. As a result, we show that both the shadow structure and the energy emission rate depend on the global monopole parameter, the electric charge, and the rotation parameter. However, we observe that the Euler--Heisenberg nonlinear parameter does not significantly affect either the shadow or the energy emission rate. In order to reconcile the present theoretical predictions with the shadow observations reported by the Event Horizon Telescope collaboration, we employ a CUDA-based computational approach to establish strict bounds on the GM parameter, the electric charge, and the rotation parameter.
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