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Related papers: The Limits of Custodial Symmetry

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A mixed-symmetry nuclear shell-model scheme for carrying out calculations in regimes where there is a competition between two or more modes is proposed. A one-dimensional toy model is used to demonstrate the concept. The theory is then…

Nuclear Theory · Physics 2007-05-23 J. P. Draayer , V. G. Gueorguiev , Feng Pan , Yanan Luo

We consider a conformal complex singlet extension of the Standard Model with a Higgs portal interaction. Two different scenarios depending on whether the global U(1) symmetry is broken or not have been studied. In the unbroken phase, the…

High Energy Physics - Phenomenology · Physics 2016-11-11 Zhi-Wei Wang , Frederick S. Sage , T. G. Steele , R. B. Mann , T. Hanif

We obtain constraints on possible anomalous interactions of the top quark with the electroweak vector bosons arising from the precision measurements at the Z pole. In the framework of $SU(2)_L \otimes U(1)_Y$ chiral Lagrangians, we examine…

High Energy Physics - Phenomenology · Physics 2009-10-30 O. J. P. Eboli , M. C. Gonzalez-Garcia , S. F. Novaes

A new supersymmetric standard model based on N=1 supergravity is constructed, aiming at natural explanation for the proton stability without invoking an ad hoc discrete symmetry through R parity. The proton is protected from decay by an…

High Energy Physics - Phenomenology · Physics 2009-10-31 Mayumi Aoki , Noriyuki Oshimo

While little Higgs models provide an interesting way to address the hierarchy problem, concrete models in the literature typically face two major obstacles. First, the mechanism for generating a Higgs quartic coupling often leads to large…

High Energy Physics - Phenomenology · Physics 2014-11-21 Martin Schmaltz , Daniel Stolarski , Jesse Thaler

We consider a recent proposal by Dimopoulos and Kaplan to embed the electroweak SU(2)_L X U(1)_Y into a larger group SU(3)_W X SU(2) X U(1) at a scale above a TeV. This idea is motivated by the prediction for the weak mixing angle sin^2…

High Energy Physics - Phenomenology · Physics 2009-09-17 Csaba Csaki , Joshua Erlich , Graham D. Kribs , John Terning

We show that some models with $SU(3)_C\otimes SU(3)_L\otimes U(1)_X$ gauge symmetry can be realized at the electroweak scale and that this is a consequence of an approximate global $SU(2)_{L+R}$ symmetry. This symmetry implies a condition…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. G. Dias , J. C. Montero , V. Pleitez

The model proposed by Georgi and Machacek enables the Higgs sector to involve isospin triplet scalar fields while retaining a custodial $SU(2)_V$ symmetry in the potential and thus ensuring the electroweak $\rho$ parameter to be one at tree…

High Energy Physics - Phenomenology · Physics 2017-07-12 Simone Blasi , Stefania De Curtis , Kei Yagyu

We construct a model of spontaneous CP violation in E6 supersymmetric grand unified theory. In the model, we employ an SU(2)F flavor symmetry and an anomalous U(1)A symmetry. The SU(2)F flavor symmetry is introduced to provide the origin of…

High Energy Physics - Phenomenology · Physics 2014-11-20 M. Ishiduki , S. -G. Kim , N. Maekawa , K. Sakurai

We investigate the SU(N) supersymmetric Grand Unified Theories with ``custodial symmetry'' mechanism to explane the doublet-triplet hierarchy. We show that in such type of SU(7) SUSY theory intermediate scale appears naturally and the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ilia Gogoladze

We study a supersymmetric extension of the SM with Higgs triplets in the scalar sector. We begin with a review of the SM, particularly the Higgs mechanism. In the SM, the Higgs mechanism requires the presence of a complex Higgs doublet to…

High Energy Physics - Phenomenology · Physics 2024-08-09 Yingnan Xu

In this work we study the interactions of the $Z$ and $Z^{\prime}$ generated by kinetic mixing in a class of theories for physics beyond the standard model motivated by the dark matter problem, containing a spontaneously broken extra…

High Energy Physics - Phenomenology · Physics 2021-10-19 M. Napsuciale , S. Rodriguez , H. Hernandez-Arellano

We consider non-supersymmetric quiver theories obtained by orbifolding the N=4 supersymmetric U(K) gauge theory by a discrete Z_\Gamma group embedded in the SU(4) R-symmetry group. We explicitly find that in such theories there are no…

High Energy Physics - Theory · Physics 2015-06-26 Philippe Brax , Adam Falkowski , Zygmunt Lalak , Stefan Pokorski

Two dimensional QCD coupled to fermions in the adjoint representation of the gauge group $SU(N)$, a useful toy model of QCD strings, is supersymmetric for a certain ratio of quark mass and gauge coupling constant. Here we study the theory…

High Energy Physics - Theory · Physics 2009-10-28 Joshua Boorstein , David Kutasov

As shown in [1], two copies of the large $N$ Majorana SYK model can produce spontaneous breaking of a $Z_2$ symmetry when they are coupled by appropriate quartic terms. In this paper we similarly study two copies of the complex SYK model…

High Energy Physics - Theory · Physics 2020-12-30 Igor R. Klebanov , Alexey Milekhin , Grigory Tarnopolsky , Wenli Zhao

Two models which generate the supersymmetric Grand Unification Scale from the strong dynamics of an additional gauge group are presented. The particle content is chosen such that this group confines with chiral symmetry breaking. Fields…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Graesser

I derive conservative upper bounds on the supersymmetry breaking parameter $m_{1/2}$ as a function of the strong coupling in the Standard Supersymmetric Model (SSM) using gauge coupling unification. I find that over more than $99\%$ of the…

High Energy Physics - Phenomenology · Physics 2016-09-01 S. Kelley

We obtain the condition to protect the baryon number in the $SU(2)_{L}$ triplet Higgs model. The obtained condition gives the upper limits for either of the two kinds of the coupling constants which are newly introduced in addition to ones…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. Hasegawa

We propose a E_6 inspired supersymmetric model with a non-Abelian discrete flavor symmetry (S_4 group); that is, SU(3)_c x SU(2)_W x U(1)_Y x U(1)_X x S_4 x Z_2. In our scenario, the additional abelian gauge symmetry; U(1)_X, not only…

High Energy Physics - Phenomenology · Physics 2014-11-20 Y. Daikoku , H. Okada

The Standard Model with a light Higgs provides a very accurate description of the electroweak precision observables. The largest deviation between the Standard Model predictions and the experimental measurements, the forward-backward…

High Energy Physics - Phenomenology · Physics 2011-05-10 Leandro Da Rold