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Related papers: SUGRA interactions within flavor triplets

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It is shown that quarks and leptons can couple intrinsically to pure supergravity, preserving for this context the degeneracy of globally supersymmetric vacua, and specifically preserving the vacuum that is characterized by SU(4)XU(1). A…

High Energy Physics - Phenomenology · Physics 2016-09-06 J. Towe

A conventional graviton vertex operator is generated from the gauging of global supersymmetry. If the outgoing gravitino is replaced by a fermion-boson pair of like helicity, and if a new principle of equivalence associates supergravity…

High Energy Physics - Phenomenology · Physics 2007-05-23 Joseph Towe

Colour $SU(3)$ group is an exact symmetry of Quantum Chromodynamics, which describes strong interactions between quarks and gluons. Supplemented by two internal symmetries, $SU(2)$ and $U(1)$, it serves as the internal symmetry of the…

High Energy Physics - Theory · Physics 2020-01-08 Richard Kerner , Jerzy Lukierski

A generic heterotic string theory is uniquely reduced to the standard model in terms of a geometry that transcends compactification. This device also extends the standard model to embrace three generations of fermions, including a…

General Physics · Physics 2007-05-23 J. Towe

In the current version of QCD the quarks are described by ordinary Dirac fields, organized in the following internal symmetry multiplets: the $SU(3)$ colour, the $SU(2)$ flavour, and broken $SU(3)$ providing the family triplets. \noindent…

High Energy Physics - Theory · Physics 2021-11-03 Richard Kerner , Jerzy Lukierski

We show that nuclear interactions are SU(4) symmetric at leading order in chiral perturbation theory in the large-N limit of QCD. The nucleons and delta resonances form a 20-dimensional representation of SU(4) and we show how Wigner's…

High Energy Physics - Phenomenology · Physics 2019-08-15 David B. Kaplan , Martin J. Savage

We consider six-dimensional supergravity with gauge group $SO(10)\times U(1)_A$, compactified on the orbifold $T^2 / \mathbb{Z}_2$. Three quark-lepton generations arise as zero modes of a bulk $\bf16$-plet due to magnetic flux of the…

High Energy Physics - Theory · Physics 2015-10-14 Wilfried Buchmuller , Markus Dierigl , Fabian Ruehle , Julian Schweizer

Quarks come in three colors and have electric charges in multiples of one-third. There are also three families of quarks and leptons. Whereas the first two properties can be understood in terms of unification symmetries such as SU(5),…

High Energy Physics - Phenomenology · Physics 2009-11-11 Ernest Ma

In combination with supersymmetry, flavor symmetry may relate quarks with leptons, even in the absence of a grand-unification group. We propose an SU(3)xSU(2)xU(1) model where both supersymmetry and the assumed A4 flavor symmetries are…

High Energy Physics - Phenomenology · Physics 2011-09-01 S. Morisi , E. Peinado , Yusuke Shimizu , J. W. F. Valle

I investigate the phenomenology of supersymmetric models with extra vector-like supermultiplets that couple to the Standard Model gauge fields and transform as the fundamental representation of a new confining non-Abelian gauge interaction.…

High Energy Physics - Phenomenology · Physics 2011-03-23 Stephen P. Martin

It is argued that every quark flavor can be described as a lepton that has been excited by the absorption of a supernatural field, which is defined. In this context, a minimal irriducible representation of SUSY SU(5) is constructed…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Towe

The discovery of the SU(3) symmetry was fundamental as to establishing an ordering principle in particle physics. We already studied how to couple the SU(3) symmetry to the gravitational field in four-dimensional curved Lorentzian…

General Relativity and Quantum Cosmology · Physics 2026-03-20 Alcides Garat

We construct a 6D supergravity theory which emerges as intermediate step in the compactification of the heterotic string to the supersymmetric standard model in four dimensions. The theory has N=2 supersymmetry and a gravitational sector…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Buchmüller , C. Lüdeling , J. Schmidt

We construct an orbifold model in which all the standard model particles are unified in a gauge multiplet in higher dimensional supersymmetric gauge theory. We find that a flavor symmetry has to remain in four dimensions due to the discrete…

High Energy Physics - Phenomenology · Physics 2009-03-12 Yukihiro Mimura

We argue that the A_4 symmetry as required by three flavors of fermions may well-embed in the SU(3)_C X SU(3)_L X U(1)_X gauge model. The new neutral fermion singlets as introduced in a canonical seesaw mechanism can be combined with the…

High Energy Physics - Phenomenology · Physics 2015-03-13 P. V. Dong , L. T. Hue , H. N. Long , D. V. Soa

We give a model for composite quarks and leptons based on the semisimple gauge group SU(4), with the preons in the 10 representation; this choice of gauge gluon and preon multiplets is motivated by the possibility of embedding them in an…

High Energy Physics - Theory · Physics 2016-09-06 Stephen L. Adler

We show that the recently constructed 5-dimensional supersymmetric $S^1/(Z_2\times Z_2')$ orbifold GUT models allow an appealing explanation of the observed hierarchical structure of the quark and lepton masses and mixing angles. Flavor…

High Energy Physics - Phenomenology · Physics 2014-11-17 Lawrence Hall , John March-Russell , Takemichi Okui , David Smith

The seemingly disparate notions of chiral color and quark-lepton nonuniversality are combined, and shown to be essential to each other as part of an underlying (and unifying) larger symmetry, i.e. supersymmetric SU(3)^6. Both phenomena are…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ernest Ma

We propose an SU(5) SUSY GUT of flavour with A_4 family symmetry in 8d where the vacuum alignment is achieved in an elegant way by the use of boundary conditions on orbifolds. The model involves SU(5) living in the 8d bulk, with matter…

High Energy Physics - Phenomenology · Physics 2014-11-21 T. J. Burrows , S. F. King

We construct a three family flipped SU(5) model from the heterotic string theory compactified on the $\Z_{12-I}$ orbifold with one Wilson line. The gauge group is $\rm SU(5)\times U(1)_X\times U(1)^2\times[SU(2)\times SO(10)\times…

High Energy Physics - Theory · Physics 2008-11-26 Jihn E. Kim , Bumseok Kyae
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