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It is pointed out that every renormalizable field theory has a symmetry which is hidden in plain sight. In all practical cases, it is also broken softly, either explicitly or spontaneously. The soft explicit breaking mass terms may be…

High Energy Physics - Phenomenology · Physics 2025-02-20 Ernest Ma

We have recently argued that quark masses may follow a simple scaling law. In this paper we build a simple mass matrix for quarks that can reproduce the scaling law expression. The simple mass matrices of the model are then generalized…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alp Deniz Özer

We propose a model of dynamical symmetry breaking, in which a new type of fundamental scalar fields of zero mass-dimension mediate the couplings of fermions to the gravitational field, represented here as a tetrad field in the same manner…

High Energy Physics - Theory · Physics 2022-10-03 J. Miller , M. A. Zubkov

Considering that the soft SUSY breaking scalar masses come from a vacuum expectation value of the D-term for an external gauge multiplet, the renormalization of the scalar masses is related to the gauge anomaly. Then, if the external gauge…

High Energy Physics - Phenomenology · Physics 2009-09-29 J. Hisano , Kiichi Kurosawa , Yasunori Nomura

We propose for the flavour structure of both the quark and lepton sectors, the principle of Universal Democracy (UD), which reflects the presence of a $Z_3$ symmetry. In the quark sector, we emphasize the importance of UD for obtaining…

High Energy Physics - Phenomenology · Physics 2013-04-05 G. C. Branco , N. Raimundo Ribeiro , J. I. Silva-Marcos

I propose a controlled approximation to QCD-like theories with massless quarks by employing supersymmetric QCD perturbed by anomaly-mediated supersymmetry breaking. They have identical massless particle contents. Thanks to the…

High Energy Physics - Theory · Physics 2021-06-30 Hitoshi Murayama

The order parameters of dynamical chiral symmetry breaking in QCD, the dynamical mass of quarks and the chiral condensates, are evaluated by numerically solving the Non-Perturbative Renormalization Group (NPRG) equations. We employ an…

High Energy Physics - Theory · Physics 2009-10-31 Ken-Ichi Aoki , Kaoru Takagi , Haruhiko Terao , Masashi Tomoyose

Mass matrix of quarks is studied in the Supersymmetric $E_6$ Grand Unified Theory (GUT). The fundamental representation $\textbf{27}$ in $E_6$ which corresponds to one generation contains two sets of $\textbf{5}^{*}$'s in SU(5), so that…

High Energy Physics - Phenomenology · Physics 2007-05-23 Midori Obara , Gi-Chol Cho , Makiko Nagashima , Akio Sugamoto

It is shown that when the mass matrix changes in orientation (rotates) in generation space for changing energy scale, then the masses of the lower generations are not given just by its eigenvalues. In particular, these masses need not be…

High Energy Physics - Phenomenology · Physics 2009-02-09 Jose Bordes , H. M. Chan , S. T. Tsou

We reconstruct the neutrino mass matrix in flavor basis, in the case of inverted mass hierarchy (ordering), using all available experimental data on neutrino masses and oscillations. We analyze the dependence of the matrix elements m_{alpha…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. Frigerio , A. Yu. Smirnov

We propose a supersymmetric model of quark flavor symmetry based on SU(3)colorxSU(3)WxU(1)X x T' where T' (binary tetrahedral group) is a discrete flavor symmetry group. The third (heavy) generation of quarks are assigned to singlet…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sutapa Sen

In this paper, we obtain the light neutrino masses and mixings consistent with the experiments, in the democratic texture approach. The essential ansatz is that $\nu_{Ri}$ are assumed to transform as "right-handed fields" $\bf 2_{R} +…

High Energy Physics - Phenomenology · Physics 2020-05-28 Masaki J. S. Yang

We calculate the low energy effective action of massless and massive complex linear superfields coupled to a massive U(1) vector multiplet. Our calculations include superspace higher derivative corrections and therefore go beyond previous…

High Energy Physics - Theory · Physics 2015-03-05 Fotis Farakos , Rikard von Unge

We propose a simple gauge-mediated supersymmetry breaking model in which suitable soft breaking masses are dynamically generated without relying on a messenger sector. This model is constructed as an extention of the 3-2 model and needs no…

High Energy Physics - Phenomenology · Physics 2009-10-30 N. Haba , N. Maru , T. Matsuoka

The observed neutrino mixing, having a near maximal atmospheric neutrino mixing angle and a large solar mixing angle, is close to tri-bi-maximal. This structure may be related to the existence of a discrete non-Abelian family symmetry. In…

High Energy Physics - Phenomenology · Physics 2015-08-04 Ivo de Medeiros Varzielas

We show that the fermion mass spectrum may naturally be understood in terms of flavour democratic fixed points in supersymmetric theories which have a large domain of attraction in the presence of "strong unification". Our approach provides…

High Energy Physics - Phenomenology · Physics 2009-10-31 Steven Abel , Steven King

The mass hierarchies of quarks and charged leptons as well as a large $\n_\m$-$\n_\t$ mixing angle are naturally explained by the Frogatt-Nielsen mechanism with a nonparallel family structure of chiral charges. We extend this mechanism to…

High Energy Physics - Phenomenology · Physics 2009-10-31 W. Buchmüller , T. Yanagida

It is known that a three Higgs doublet model (3HDM)symmetric under an exact $A_4$ symmetry is not compatible with nonzero quark masses and/or non-block-diagonal CKM matrix. We show that a 3HDM with softly broken $A_4$ terms in the scalar…

High Energy Physics - Phenomenology · Physics 2023-05-03 Iris Bree , Sergio Carrolo , Jorge C. Romao , Joao P. Silva

In non-supersymmetric grand unified models a ``radiative fermion mass hierarchy" can be achieved in which the spectrum of quark and lepton masses is determined entirely by physics at the unification scale, with many relations following from…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Barr

We introduce a new method for calculating the mixing matrix for non-singlet quark operators including total derivatives, based solely on their renormalization structure in the chiral limit. As input, the method requires the well-known…

High Energy Physics - Phenomenology · Physics 2022-03-02 Sam Van Thurenhout , Sven-Olaf Moch