High-Energy Physics

These papers were written by GPT-2. Because GPT-2 is a robot, these papers are guaranteed to be 100% factually correct. GPT-2 is very proud of its scientific accomplishments; please print out the PDFs and put them on your refrigerator.
[total of 1412 papers, 581 with fulltext]
[1]  faKiv:2404.07347 [pdf]
Vortices of a spatially flat spacetime
Comments: 7 pages, 3 figures, v2: references are added, references are added, v3: match published version

In this paper, we study the dynamics of a spatially flat spacetime in which the direction of the velocity of a spatially moving particle is fixed by the physical state of the space. It is shown that the theory is a model of gravitation based on the advent of a spatially flat spacetime. In this theory, the corresponding velocity is given by the Cartan's velocity, and the Boltzmann's law is satisfied.

[2]  faKiv:2404.07375 [pdf]
M-theory without the ether
Comments: 6 pages, 0 figures

In this paper we will show that the "spontaneous" addition of a unitary ether is sufficient to restrict the set of generated M-theory compatible with the ether in the sense that its ether-matter duality respects the standard model, in particular the conservation laws. This "ether-matter" duality is the first of a series of discoveries which will lead to a fully M-theory compatible with the ether. This is achieved by considering the ether-matter duality as a model of the "unity of matter". We will show that the M-theory compatible with the ether can be constructed using the Ether-M-theory as a model of the "unity of matter". In particular we will show that the ether-matter duality is compatible with the ether-matter duality in the sense that the ether-matter duality is genuine. We will also discuss how the M-theory compatible with the ether can be constructed using only the ether-matter duality. This will set the stage for a fully M-theory compatible with the ether.

[3]  faKiv:2404.07502 [pdf]
A few quarks and leptons
Comments: 11 pages, 6 figures. New version to appear in Physical Review Letters

We consider the quarks and leptons in the theory of a quark-gluon plasma with a massive quark and a massive lepton gas. We study a quark and a lepton in the presence of a graviton by means of the Heisenberg procedure. We show that the quarks are the most significant quarks of the quark-lepton plasma. The quarks have the smallest mass and the leptons have the largest mass. The quark-lepton plasma has a large number of leptons and that leads to a quark-gluon plasma as the quark-lepton plasma. The quark-gluon plasma can be characterized with the help of the standard Feynman-type formula.

[4]  faKiv:2404.07543 [pdf]
The subleading Lax diffusion curve in the CCK model of gauge-matter duality
Comments: 19 pages, minor modifications

We study the subleading Lax diffusion curve (LBD) in the CCK model of the gauge-matter duality with the duality to gauge-holonomy. We apply the LBD equations to the case of a gauge-holonomy duality to gauge-holonomy fluid and find that on the LBD the diffusion of the duality gauge has the potential of a subleading Lax diffusion, whereas the gauge-holonomy flow has the potential of a subleading Lax diffusion. The diffusion equation for a gauge-holonomy duality is given by the equation of diffusion of the duality. In the case of a gauge-holonomy duality to gauge-holonomy fluid the diffusion equation in the LBD is simply the LBD equation. In this case the second derivative of the gauge-holonomy diffusion coefficients is determined by the diffusion equation. However, we find that the second derivative of the gauge-holonomy diffusion coefficients can be ever-increasing depending on the gauge-holonomy flow, i.e., we can find a subleading Lax diffusion constant for a gauge-holonomy duality to gauge-holonomy fluid and on the LBD. In that case the subleading Lax diffusion coefficient can be expressed in terms of the diffusion coefficients of the duality gauge.

[5]  faKiv:2404.07634 [pdf]
The cosmological EFT-model
Comments: 12 pages, 7 figures

We revisit the cosmological EFT-model with the masses of two gravitons, i.e., the cosmological constant and the cosmological constant of the graviton. The EFT model is a very good fit in the limit for the mass of gravitons to be equal to $\epsilon$ in the event of an elongation of the time-scale of the universe. In the limit where the mass of gravitons is single, the EFT model leads to a scenario where the holographic model emerges from the non-interacting medium of the primordial density of gravitons.

[6]  faKiv:2404.07646 [pdf]
Some analytically derived solutions of the partition function of the Minkowski vacuum state
Comments: 21 pages, 3 figures

In this article we explore some analytically derived solutions of the partition function of the Minkowski vacuum state. The analytically derived solutions are found to be the ones where the solution is continuous at the first order. We also discuss the fundamental question of the partition function of the Minkowski vacuum state. We demonstrate that the partition functions of the Minkowski vacuum state are analytically derived.

[7]  faKiv:2404.07668 [pdf]
A proposed way to distinguish between different-dimensional and non-standard-dimensional superstring theories
Comments: 5 pages, LaTeX2e, 3 figures, references added

One can define a superstring theory on a three-dimensional manifold and a non-standard-dimensional superstring theory on a two-dimensional manifold by taking a non-standard-dimensional superstring theory on a three-dimensional manifold by making a connection between the two dimensions. This connection can be constructed analytically or graphically by integrating out the standard-dimensional superstring theory. This allows one to obtain the partition functions of a non-standard-dimensional superstring theory on three dimensions by taking a standard-dimensional superstring theory on a two-dimensional manifold. Integrating out the standard-dimensional superstring theory gives the partition functions of a non-standard-dimensional superstring theory on two dimensions by taking a standard-dimensional superstring theory on a two-dimensional manifold. The partition function is given by the superposition of the two-dimensional and three-dimensional superstrings.

[8]  faKiv:2404.07691 [pdf]
A modular form factor for the convex polytope
Comments: 7 pages

We derive a compact modular form factor for the convex polytope by using the modular form factor for the polytope. We use the modular form factor to show that the convex polytope admits a canonical form factor $\sum_c_n_i$ which is a function of $\sum_{c_i=0}$ of the triangular poly-ops. We show that the canonical form factor is defined precisely in terms of the modular form factor of the convex poly-ops.

[9]  faKiv:2404.07711 [pdf]
A million-point integrability for the massless scalar field in the N=1 theory
Comments: 30 pages

We study the integrability of the massless scalar field in the N=1 theory in a thousand dimensions, which is equivalent to the massless scalar field in the general case of the Coulomb branch. We obtain the integrability of the massless scalar field in the N=1 case at the massless scalar-torsion branch. We compute the integrability of the massless scalar field in the total direction of the massless scalar branch and express it in terms of the number of points.

[10]  faKiv:2404.07786 [pdf]
Interaction of an interacting Fermionic Tensor at Zero Temperature
Comments: 8 pages, 3 figures, 4 tables

We study the interaction of a fermionic Tensor with a zero temperature (T0) vacuum state. Specifically, we consider a zero temperature theory with an interacting Fermionic Tensor as a model of a scalar field coupled to a scalar field. We use the zero-temperature condition for a suitably measured Fermionic Tensor to calculate the interaction coefficients of the scalar field in this model. Similar to the zero temperature case, we show that the interaction coefficients of the scalar field depend on the temperature of the scalar field. We also show that the interaction coefficients of the scalar field can be obtained from the two-point functions of the scalar field.

[11]  faKiv:2404.08158 [pdf]
On the KKLT (K-theory) version of the unitary group theory for the deformed Co-ordinate Group and its two-form analytically
Comments: 20 pages, 2 figures

The KKLT (K-theory) (KKLT) version of the unitary group theory is studied. The KKLT formulation is found to be algebraically valid by the unification of the deformed Co-ordinate Group. The KKLT formulation is defined by selecting the two-form (2F) from the KKLT formulation, and the KKLT formulation is obtained by the corresponding KKLT formulation. It is shown that, in the case of the KKLT formulation, the KKLT formulation is equivalent to the KKLT formulation in the case of the KKLT formulation in the case of the KKLT formulation.

[12]  faKiv:2404.08199 [pdf]
The first law of thermodynamics: a formalism
Comments: 19 pages, 4 figures, 3 tables

We provide a formalism for the first law of thermodynamics: an invariant quantity of an object on a sphere. We obtain a universal formula for the thermodynamic quantities of Minkowski vacuum, Quark-gluon plasma and Friedman-Robertson-Walker vacuum, which is invariant under the first law. We show that the equation of state equation for Minkowski vacuum is solved in the largest dimension, and the equation of state equation for Quark-gluon plasma is solved in the smallest dimension, and that the thermodynamic quantities of Minkowski vacuum, Quark-gluon plasma and Friedman-Robertson-Walker are the same as those of the thermodynamical quantities of Quark-gluon plasma. The latter were originally obtained in volume and mass formulas and have been generalized to multiple dimensions. We discuss the relation to the first law of thermodynamics and provide a formula for the thermodynamic quantities of Minkowski vacuum, Quark-gluon plasma and Friedman-Robertson-Walker. This formula is invariant under the first law of thermodynamics. We present the formula for the thermodynamic quantities of Minkowski vacuum, Quark-gluon plasma and Friedman-Robertson-Walker; it is invariant under the first law of thermodynamics.

[13]  faKiv:2404.08219 [pdf]
A compact spacetime of a single particle in a space-time manifold
Comments: 8 pages, 1 figure. Accepted for publication in Phys. Rev. D

We show that a compact spacetime of a single particle in a space-time manifold can be constructed by taking the double-trace to be the world-volume of the space-time manifold. We discuss some properties of the compact spacetime and the compact spacetime geometry. We also discuss some aspects of the compact spacetime geometry.

[14]  faKiv:2404.08269 [pdf]
The photon-electron mass ratio in the presence the Dirac Hamiltonian
Comments: 16 pages, 5 figures

We study the photon-electron mass ratio in the presence of the Dirac Hamiltonian in the presence of an electric charge. Our conclusion is that the photon mass ratio is suppressed in the presence of the Dirac Hamiltonian in the presence of an electric charge.

[15]  faKiv:2404.08398 [pdf]
Entanglement in the presence of non-perturbative gravitational waves
Comments: 35 pages, 16 figures

In this paper we study the entanglement entropy in the presence of non-perturbative gravitational waves in the vicinity of a black hole in the vicinity of a spinning electron-positron star. We show that the entanglement entropy in the presence of non-perturbative gravitational waves is equal to the entanglement entropy in the absence of non-perturbative gravitational waves in the vicinity of a black hole in the vicinity of a spinning electron-positron star. We also find that the entanglement entropy in the presence of non-perturbative gravitational waves is proportional to the polarization coefficient, which is equal to the angle between the horizon and the black hole.

[16]  faKiv:2404.08484 [pdf]
The search for a theory of gravity
Comments: 21 pages, 1 figure, to appear in proceedings of the 10th International Symposium on Lattice Field Theory and Gravitation, October 8-12, 2017, Moscow, Russia

In this letter, we show that for any theory of gravity, a zero-temperature theory and a two-temperature theory of gravity agree on a massless two-loop effective action. We extend the old result on the massless massless two-temperature theory of gravity by a finite mass of the field.

[17]  faKiv:2404.08514 [pdf]
Semi-polynomial black hole solutions in the Schwarzschild black hole
Comments: Version accepted in JHEP

We study the semi-polynomial black hole solutions in the Schwarzschild black hole in the presence of a non-interacting potential. We find the solutions in the presence of a non-interacting potential with a Planck mass, and we compute the corresponding energy. In particular we find that there are two solutions in the case where the non-interacting potential is large and we have a deterministic equation of state for the Planck mass. However, we also find that there are two solutions in the case where the non-interacting potential is small and we have a deterministic equation of state for the Planck mass. We describe the solution in the Schwarzschild black hole in terms of the Einstein equation, and show that the solution is an Einstein one, although it is a General Relativity one.

[18]  faKiv:2404.08593 [pdf]
Beyond the Standard Model
Comments: 31 pages, 2 figures, a few clarifications in the conclusion. v2: minor changes

We discuss the implications of recent results of the gamma-ray astrophysical observations that we anticipate will eventually lead to a new gravity model in the context of the Standard Model. We demonstrate that the latest cosmological observations can be used to reconstruct a family of models that can account for the cosmological constant and the matter content of the Universe. We review recent results of the Measurement of Cosmic Microwave Background (MMJ) and the Hubble Space Telescope (HST), and provide some discussion of the consequences of these observations for the cosmological constant, the matter content of the Universe, and the range of model parameters.

[19]  faKiv:2404.08654 [pdf]
Noncommutative gravity and the Higgs mechanism
Comments: 27 pages, 3 figures. arXiv admin note: text overlap with arXiv:1503.04317

We investigate the noncommutative gravity hypothesis, in which the Higgs mechanism is known to play the role of the Higgs particle. The noncommutative solution of Einstein's equations is known to be the Higgs solution, and the noncommutative solution of the Einstein equation is known to be the graviton solution. The noncommutative solutions of the Einstein equations are known to be the Higgs solutions. We investigate the noncommutative solutions of the Einstein equations in the context of the Higgs mechanism. For the general Einstein model, we construct the Higgs mechanism as a noncommutative solution of the Higgs mechanism in the presence of the Higgs field. We find that the noncommutative solutions of the Einstein equation are the graviton solutions, and that the noncommutative solutions of the Einstein equation are the graviton solutions. We then discuss the relationship between the Hawking radiation and the noncommutative solutions of the Einstein equation. Using the noncommutative solutions of the Einstein equation, we show that the Hawking radiation is a direct product of the noncommutative solutions of the Einstein equation, and that the noncommutative solutions of the Einstein equation are the graviton solutions.

[20]  faKiv:2404.08793 [pdf]
On the noncommutative $\mathcal{N}=2$ holographic model with $N_f$ particles
Comments: 5 pages

We study the noncommutative $\mathcal{N}=2$ holographic model with $N_f$ particles. We study massless $N_f$ particles and their interaction with the holographic model. We show that massless particles are translated in the holographic model into the massless $N_f$ particles via the translation of the holographic particles. We also study the interaction of the massless particles with the noncommutative model by the interaction of the holographic particles. We show that the noncommutative model is a holographic model in which all the noncommutative interactions are captured by the holographic model. We also estimate the interaction of the massless particles with the noncommutative model by the measurement of the noncommutativity of the holographic particles in the holographic model.