ID: 2411.17714

Gauging Flavor Symmetries of the Standard Model: from Dark Energy to Matter-Antimatter Asymmetry from Higher Dimensions in the Early Universe

November 19, 2024

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An Integrated Model of Fermion Flavor and Baryon asymmetry and Dark Matter with The TeV Scale $U(1)_{B-L}$

June 23, 2012

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Wei-Min Yang
Cosmology and Nongalactic As...

This paper has been withdrawn by the author. I suggest a new particle model to solve simultaneously the problems of fermion masses and flavor mixings, and baryon asymmetry and dark matter. The model extends the standard model by adding a local $U(1)_{B-L}$ gauge symmetry at the TeV scale, in addition, the fermion flavor structures are characterized by the original $S_{3}$ and residual $S_{2R}$ flavor family symmetries. The model can excellently fit all the current experimenta...

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Fundamental Particle Structure in the Cosmological Dark Matter

November 11, 2013

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Maxim Yu. Khlopov
Cosmology and Nongalactic As...

The nonbaryonic dark matter of the Universe is assumed to consist of new stable forms of matter. Their stability reflects symmetry of micro world and mechanisms of its symmetry breaking. Particle candidates for cosmological dark matter are lightest particles that bear new conserved quantum numbers. Dark matter particles may represent ideal gas of non-interacting particles. Self-interacting dark matter weakly or superweakly coupled to ordinary matter is also possible, reflecti...

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A New Approach to the Family Structure

June 28, 1996

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Otto C. W. UNC-Chapel Hill Kong
High Energy Physics - Phenom...

In this letter, we introduce a new approach to formulate the family structure of the standard model. Trying to mimic the highly contrained representation structure of the standard model while extending the symmetry, we propose a $SU(4)\otimes SU(3)\otimes SU(2)\otimes U(1)$ symmetry with a SM-like chiral spectra basically "derived" from the gauge anomaly constraints. Embedding the SM leads to $SU(4)_A\otimes SU(3)_C\otimes SU(2)_L\otimes U(1)_X$ models, which upon the $SU(4)_...

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A Simple Solution for the Flavor Question

September 15, 1996

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Felice IFT - S. Paulo - Brazil Pisano
High Energy Physics - Phenom...

We consider a simple way for solving the flavor question by embedding the three-familiy Standard Model in a semisimple gauge group extending minimally the weak isospin factor. Quantum chiral anomalies between families of fermions cancel with a matching of the number of families and the number of color degrees of freedom. Our demonstration shows how the theory leads to determination of families structure when the Standard Model is the input at low energies. The new physics is ...

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Can the matter-antimatter asymmetry be easier to understand within the "spin-charge-family-theory", predicting twice four families and two times $SU(2)$ vector gauge and scalar fields?

November 26, 2010

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N. S. Mankoc Borstnik
General Physics

This contribution is an attempt to try to understand the matter-antimatter asymmetry in the universe within the {\it spin-charge-family-theory} if assuming that transitions in non equilibrium processes among instanton vacua and complex phases in mixing matrices are the sources of the matter-antimatter asymmetry, as studied in the literature for several proposed theories. The {\it spin-charge-family-theory} is, namely, very promising in showing the right way beyond the {\it st...

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A general theory of the standard model and the revelation of the dark side of the universe

February 26, 2025

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Yue-Liang Wu
General Physics

A general theory of the Standard Model is presented in a spin-related gravigauge spacetime, grounded on conformal inhomogeneous spin gauge symmetry WS$_c$(1,3)=SP(1,3)$\rtimes$W$^{1,3}$$\rtimes$SP$_c$(1,1) and scaling gauge symmetry SG(1), along with symmetry U$_Y$(1)$\times$SU$_L$(2)$\times$SU(3)$_c$ in the standard model. It introduces new interactions: spin, chirality boost-spin, chiral conformal-spin, and scaling gauge forces. A gravitization equation is obtained to descr...

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A common origin of the Higgs boson and the flavor hierarchies

December 18, 2024

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Javier M. Lizana
High Energy Physics - Phenom...

We present a model that extends the electroweak gauge symmetry of the Standard Model in a non-universal way to $SU(2)_{L}^{\prime}\times U(1)_X \times SU(2)_{L}^{q_3}\times SU(2)_R^{\ell_3}$. This symmetry is spontaneously broken to $SU(2)_L\times U(1)_Y$ near the TeV scale by a condensate of a new composite sector. Charging appropriately the fermionic degrees of freedom of the composite sector, anomaly cancellation enforces the Standard Model fermions to be charged in such a...

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On the origin of matter-antimatter asymmetry in the Universe

April 7, 2022

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Efstratios Manousakis
High Energy Physics - Theory
High Energy Physics - Lattic...

In order to investigate the origin of matter-antimatter asymmetry in the Universe, we adopt a theoretical framework where the standard model emerges as a Poincar\'e invariant field theory localized at a domain-antidomain wall (DW-aDW) brane pair of a theory which lives on a higher dimensional bulk. We argue that such a system of a parallel DW-aDW pair could have been created at a very early epoch of the cosmological evolution when the Universe was still of microscopic size be...

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Dark Baryogenesis

February 9, 2012

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Devin G. E. Walker
Cosmology and Nongalactic As...

We first suggested a scenario in which a generic, dark chiral gauge group undergoes a first order phase transition in order to generate the observed baryon asymmetry in the universe, provide a viable dark matter candidate and explain the observed baryon-to-dark matter ratio of relic abundances [arXiv:1003.0899]. We now provide a model in which a copy of the electroweak gauge group is added to the Standard Model. We spontaneously break this new gauge group to the diagonal Z_2 ...

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Masses by gauge flavor dynamics

January 18, 2011

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Petr Benes, Jiri Hosek, Adam Smetana
High Energy Physics - Phenom...

We gauge the experimentally observed flavor (family) index of chiral lepton and quark fields and argue that the resulting non-vectorial SU(3)_F dynamics completely self-breaks. This breakdown generates fermion masses, which in turn trigger electroweak symmetry breaking (EWSB). Suggested asymptotically free dynamics with an assumed non-perturbative infrared fixed point has just one free parameter and is therefore either right or plainly wrong. Weak point of field theories stro...

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