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Related papers: Fermion Masses without Higgs: A Supersymmetric Tec…

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We propose an extension of the Standard Model (SM) based on the $SU(3)_C\otimes SU(3)_L\otimes U(1)_X$ (3-3-1) gauge symmetry and scale invariance. Maintaining the main features of the so-called 3-3-1 models, such as the cancellation of…

High Energy Physics - Phenomenology · Physics 2020-07-29 Alex G. Dias , Julio Leite , B. L. Sánchez-Vega , William C. Vieira

After reviewing electroweak (EW) scale supersymmetry (susy) and split susy, as well as their implications in very high energy cosmic rays, I present a high scale susy model for fermion masses. An O(0.1) nu_e-nu_{tau} mixing is expected.

High Energy Physics - Phenomenology · Physics 2011-07-08 Chun Liu

We present models in which the observed fermion masses and mixings are generated by dynamically localizing the three generations of matter in a flat compact extra dimension. We first construct models assuming the hierarchy problem is…

High Energy Physics - Phenomenology · Physics 2010-02-03 David E. Kaplan , Tim M. P. Tait

We propose a gravitational dual of ``single-sector'' models of supersymmetry breaking which contain no messenger sector and naturally explain the scale of supersymmetry breaking and the fermion mass hierarchy. In five dimensions these…

High Energy Physics - Phenomenology · Physics 2008-11-26 Maxime Gabella , Tony Gherghetta , Joel Giedt

An electroweak model is formulated in a finite, four-dimensional quantum field theory without a Higgs particle. The W and Z masses are induced from the electroweak symmetry breaking of one-loop vacuum polarization graphs. The theory…

High Energy Physics - Phenomenology · Physics 2008-06-11 J. W. Moffat

In the conventional left-right gauge model, if the Higgs scalar sector consists only of an $SU(2)_L$ doublet and an $SU(2)_R$ doublet, fermion masses are zero at tree level. There have been many studies on how they would become massive.…

High Energy Physics - Phenomenology · Physics 2021-05-19 Ernest Ma

We describe a deconstructed Higgsless model in which electroweak symmetry breaking results largely from a Higgsless mechanism while the top quark mass is generated by a topcolor mechanism. The top quark mass arises from a Yukawa coupling to…

High Energy Physics - Phenomenology · Physics 2010-09-15 R. Sekhar Chivukula , Neil D. Christensen , Baradhwaj Coleppa , Elizabeth H. Simmons

An electroweak model in which the masses of the W and Z bosons and the fermions are generated by quantum loop graphs through a symmetry breaking is investigated. The model is based on a regularized quantum field theory in which the quantum…

High Energy Physics - Phenomenology · Physics 2009-08-07 J. W. Moffat , V. T. Toth

We investigate the decays of third generation scalar quarks in the Minimal Supersymmetric extension of the Standard Model, focusing on the three-body modes. We calculate the partial widths of the decays of heavier top and bottom squarks…

High Energy Physics - Phenomenology · Physics 2011-01-27 A. Djouadi , Y. Mambrini

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

In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the exception of neutrino masses. The hierarchies and apparent regularities among the quark and lepton masses are, however, otherwise a mystery.…

High Energy Physics - Phenomenology · Physics 2022-11-07 Sudip Jana , Sophie Klett , Manfred Lindner

Electroweak interactions based on a gauge group $\rm SU(3)_L \times U(1)_X$, coupled to the QCD gauge group $\rm SU(3)_c$, can predict the number of generations to be multiples of three. We first try to unify these models within SU(N)…

High Energy Physics - Phenomenology · Physics 2015-10-07 Pritibhajan Byakti , David Emmanuel-Costa , Arindam Mazumdar , Palash B. Pal

We construct supersymmetric theories in which the correct scale for electroweak symmetry breaking is obtained without significant fine-tuning. We calculate the fine-tuning parameter for these theories to be at the 20% level, which is…

High Energy Physics - Phenomenology · Physics 2009-09-29 Z. Chacko , Yasunori Nomura , David Tucker-Smith

It has been recently claimed that the symmetry group S4 yields to the Tri-bimaximal neutrino mixing in a "natural" way from the group theory point of view. Approving of this feature as an indication, we build a supersymmetric model of…

High Energy Physics - Phenomenology · Physics 2010-05-12 Federica Bazzocchi , Luca Merlo , Stefano Morisi

We built an extended 2HDM theory with a spontaneously broken $U(1) _{X}$ global symmetry, where the tree level Universal Seesaw Mechanism generates the mass hierarchy of the Standard Model charged fermions and the Zee-Babu mechanism…

High Energy Physics - Phenomenology · Physics 2024-10-25 A. E. Cárcamo Hernández , Diego Restrepo , Ivan Schmidt , Óscar Zapata

Antisymmetric tensor fields with chiral couplings to quarks and leptons may induce spontaneous electroweak symmetry breaking in a model without a ``fundamental'' Higgs scalar. No microscopic local mass term for the chiral tensors or…

High Energy Physics - Phenomenology · Physics 2009-11-11 C. Wetterich

We construct a complete, realistic, and natural UV completion of minimal conformal technicolor that explains the origin of quark and lepton masses and mixing angles. As in "bosonic technicolor", we embed conformal technicolor in a…

High Energy Physics - Phenomenology · Physics 2015-05-20 Jared A. Evans , Jamison Galloway , Markus A. Luty , Ruggero Altair Tacchi

I build a SU(2)left x U(1) electroweak gauge theory of J=0 mesons, which transform like sets of fermion-antifermion composite fields. SU(2)left x U(1) is embedded in a natural way, compatible with the Glashow-Salam-Weinberg model for…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Machet

We propose an extension of the 3-3-1 model with an additional symmetry group $Z_{2}\times Z_{4} \times U(1)_{L_g}$ and an extended scalar sector. To our best knowledge this is the first example of a renormalizable 3-3-1 model, which allows…

High Energy Physics - Phenomenology · Physics 2018-10-01 A. E. Cárcamo Hernández , Sergey Kovalenko , H. N. Long , Ivan Schmidt

We consider the detection of the technirho in technicolor models that include a weak scalar doublet. In these models, the scalar develops a vacuum expectation value when the technifermions condense, and fermion masses are generated through…

High Energy Physics - Phenomenology · Physics 2009-10-22 Christopher D. Carone , Mitchell Golden
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