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Related papers: Breaking SU3f Spontaneously Down to Isospin

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A new mechanism for spontaneous breaking of flavour symmetry is demonstrated. An exactly flavour symmetric model with degenerate bare nonets and with sufficiently strong tri-linear meson couplings is shown to lead to self-consistency…

High Energy Physics - Phenomenology · Physics 2009-10-30 Nils A. Tornqvist

The mechanism where flavor symmetry is broken spontaneously is discussed within a scalar QCD model with effective three-meson couplings. For sufficiently large coupling the model is unstable with respect to quantum loops from mesonic vacuum…

High Energy Physics - Phenomenology · Physics 2007-05-23 Nils A. Tornqvist

We show how gauged flavour breaking and N = 1 supersymmetry breaking can be dynamically aligned to produce natural models. Supersymmetry is broken in a metastable vacuum, while a weakly gauged flavour symmetry is identified with an SU(3)_F…

High Energy Physics - Phenomenology · Physics 2015-06-19 Steven Abel , Moritz McGarrie

The gauge model with $SO(3)_{F}$ flavor symmetry and three Higgs triplets is studied. We show how the intriguing nearly degenerate neutrino mass and bi-maximal mixing scenario comes out naturally after spontaneous breaking of the symmetry.…

High Energy Physics - Phenomenology · Physics 2015-06-25 Yue-Liang Wu

According to an idea that the quark and lepton mass spectra originate in a VEV structure of a U(3)-flavor nonet scalar \Phi, the mass spectra of the down-quarks and charged leptons are investigated. The U(3) flavor symmetry is spontaneously…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yoshio Koide

Flavor SU(3) symmetry, including $30\%$ first order SU(3) breaking, has been shown to describe adequately a vast amount of data for charmed meson decays to two pseudoscalar mesons and to a vector and a pseudoscalar meson. We review a recent…

High Energy Physics - Phenomenology · Physics 2015-05-20 Michael Gronau

We show that baryon number symmetry is spontaneously broken in a class of three-dimensional, ${\cal N}=1$ supersymmetric theories with a discrete mass spectrum. These models serve as lower-dimensional, less-supersymmetric analogs of the…

High Energy Physics - Theory · Physics 2025-10-06 Antón F. Faedo , Carlos Hoyos , Javier G. Subils

We show how the nearly bi-maximal mixing scenario comes out naturally from gauged $SO(3)_{F}$ flavor symmetry via spontaneous symmetry breaking. An interesting relation between the neutrino mass-squared differences and the mixing angle,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yue-Liang Wu

The decay of charmed mesons into pseudoscalar (P) and vector (V) mesons is studied in the context of nonet symmetry. We have found that it is badly broken in the PP channels and in the P sector of the PV channels as expected from the…

High Energy Physics - Phenomenology · Physics 2009-10-22 Waikwok Kwong , S. P. Rosen

My recent fit of the light scalar mesons is discussed in the light of the U3 x U3 linear sigma model. The argument for why there exists a light and broad sigma meson is explained in more detail, and the mechanism of spontaneous symmetry…

High Energy Physics - Phenomenology · Physics 2009-10-30 Nils A. Tornqvist

Two-dimensional quantum materials can host original electronic phases that arise from the interplay of electronic correlations, symmetry and topology. In particular, the spontaneous breaking of internal symmetry that acts simultaneously on…

Fermion masses and mixing matrices can be described in terms of spontaneously broken (global or gauge) flavor symmetries. We propose a little-Higgs inspired scenario in which an SU(2)xU(1) gauge flavor symmetry is spontaneously (and…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Bazzocchi , S. Bertolini , M. Fabbrichesi , M. Piai

A new mechanism for breaking an internal symmetry spontaneously is discussed, which is intermediate between the Nambu-Goldstone and Wigner modes of symmetry breaking. Here the quark-antiquark sea takes the role of the vacuum of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Nils A. Tornqvist

We examine the possibility of the flavor symmetry being $SU_f(3)$ in which the phenomenologically successful discreet symmetry $A_4$ is embedded. The allowed quadratic and quartic potentials are constructed exploiting the full symmetry…

General Physics · Physics 2019-04-05 J. D. Vergados

Recent work on a lepton mass matrix model based on an SU(3) flavor symmetry which is broken into S_4 is reviewed. The flavor structures of the masses and mixing are caused by VEVs of SU(2)_L-singlet scalars \phi which are nonets ({\bf…

High Energy Physics - Phenomenology · Physics 2007-07-09 Yoshio Koide

Several modes of $B$ decays into three pseudoscalar octet mesons PPP have been measured. These decays have provided useful information for B decays in the standard model (SM). Some of powerful tools in analyzing B decays are flavor $SU(3)$…

High Energy Physics - Phenomenology · Physics 2015-03-06 Xiao-Gang He , Guan-Nan Li , Dong Xu

Decays of the D mesons to two pseudoscalars, to two vectors, and to pseudoscalar plus vector are discussed in the context of broken flavor SU(3). A few assumptions are used to reduce the number of parameters. Amplitudes are fit to the…

High Energy Physics - Phenomenology · Physics 2016-09-01 Ian Hinchliffe , Thomas A. Kaeding

Global fits to charmless B --> PP decays in the framework of flavor SU(3) symmetry are updated and improved without reference to the \sin2\beta measured from the charmonium decay modes. Fit results directly constrain the (\bar\rho,\bar\eta)…

High Energy Physics - Phenomenology · Physics 2011-03-23 Cheng-Wei Chiang , Yu-Feng Zhou

A novel, nonperturbative, way to generate chiral symmetry breaking within the linear sigma model for 3 flavours is discussed. After spontaneous chiral symmetry breaking in the vacuum at the tree level the scalar nonet obtains mass, while…

High Energy Physics - Phenomenology · Physics 2009-10-30 Nils A. Tornqvist

We discuss why the SU(3)^3 supersymmetric model with the most general superpotential can naturally break to the standard model if gauge singlets and a discrete symmetry are included. This mechanism does away with the need for fine-tuning in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Meng Y. Wang , Eric D. Carlson
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