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Our approximately \mu-\tau symmetric neutrino mass textures fall into two different categories, whose behaviors in the \mu-\tau symmetric limit are characterized by either \sin(theta_{13})->0 (referred to as C1)), or \sin(theta_{12})->0…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kenichi Fuki , Masaki Yasue

We present an extension $U(1)_{X}$ to the Standard Model that reproduces the lepton mass structures determined by the experiments. In the charged sector, we introduced effective operators of dimension $n = 7$ to generate the mass of the…

High Energy Physics - Phenomenology · Physics 2022-10-27 C. Cortes-Parra , R. Martinez , J. S. Alvarado

We build a supersymmetric version of a recently proposed SU(3)xSU(3)xU(1)X model with heavy charged lepton and no bilepton gauge bosons.The model is an anomaly free, three generation extension of the Standard model with SU(3)L x U(1)gauge…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sutapa Sen , Aparna Dixit

The role of the a_1(1420) resonance in the three-pion decays of the tau lepton is investigated using a phenomenological model. For all data before 2008, roughly equal fit quality is achieved when the basic a_1(1260) resonance is…

High Energy Physics - Phenomenology · Physics 2017-04-07 Peter Lichard

We propose a new $\mathrm{SU}(3)_C \otimes \mathrm{SU}(2)_{L}\otimes \mathrm{U}(1)_{Y}\otimes \mathrm{U}(1)_{X}$ gauge model which is non universal respect to the three fermion families of the Standard Model. We introduce additional one…

High Energy Physics - Phenomenology · Physics 2018-08-22 R. Martinez , S. F. Mantilla

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 construct d=4,N=1 orientifolds of Gepner models with just the chiral spectrum of the standard model. We consider all simple current modular invariants of c=9 tensor products of N=2 minimal models. For some very specific tensor…

High Energy Physics - Theory · Physics 2009-11-10 T. P. T. Dijkstra , L. R. Huiszoon , A. N. Schellekens

The mass spectra of neutral mesons $K_0, \pi_0, \eta, \eta'$ on temperature-quark chemical potential $(T-\mu)$ plane in the presence of a constant magnetic field is investigated in the $SU(3)$ NJL model. As a Goldstone boson of chiral…

High Energy Physics - Phenomenology · Physics 2023-04-26 Jie Mei , Tao Xia , Shijun Mao

The R-symmetry formalism is applied for the supersymmetric economical SU(3)_C X SU(3)_L X U(1)_X (3-3-1) model. The generalization of the minimal supersymmetric standard model relation among R-parity, spin and matter parity is derived, and…

High Energy Physics - Phenomenology · Physics 2011-10-13 P. V. Dong , D. T. Huong , M. C. Rodriguez , H. N. Long

Assuming three light neutrinos and the see-saw mechanism we present a semiquantitative model of fermion masses based on (SUSY) SU(5) and abelian horizontal charges. A good description of the observed pattern of quark and lepton masses is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Guido Altarelli , Ferruccio Feruglio

Following a previous proposal, lepton number is considered as the result of a spontaneously broken non-Abelian gauge $SU(2)_N$ symmetry. New fermions are added to support this new symmetry, the spontaneous breaking of which allows these new…

High Energy Physics - Phenomenology · Physics 2021-06-23 Ernest Ma

In the covariant level-classification scheme of hadrons proposed recently, the existence of "chiral particles", scalar and axial-vector mesons as the partners of the ground-state pseudo-scalar and vector mesons, respectively, were predicted…

High Energy Physics - Phenomenology · Physics 2007-05-23 Daiki Ito , Muneyuki Ishida , Shin Ishida , Toshihiko Komada , Hiroshi Tonooka , Kenji Yamada

We perform a systematic study of the Standard Model embedding in a D-brane configuration of type I string theory at the TeV scale. We end up with an attractive model and we study several phenomenological questions, such as gauge coupling…

High Energy Physics - Theory · Physics 2008-11-26 I. Antoniadis , E. Kiritsis , J. Rizos , T. N. Tomaras

psi and Upsilon decays may be used to search for light neutral spin-1 or spin-0 bosons associated with a broken extra-U(1) symmetry, local or global, acting axially on quarks and leptons, as may be present in supersymmetric theories with a…

High Energy Physics - Phenomenology · Physics 2011-03-28 Pierre Fayet

We use the natural $SU(3)\times U(1)$ global symmetry of the gauge-fermion interaction sector of the standard model to discuss the fermion mass hierarchy problem. The $SU(3)$ sixtet and triplet Higgs are introduced. The Yukawa sector is…

High Energy Physics - Phenomenology · Physics 2007-05-23 Dan-di Wu

The tau lepton can be more composite than naively expected in models of strong electroweak symmetry breaking with tri-bimaximal lepton mixing. New leptonic resonances required by custodial symmetry, the tau custodians, can then be the first…

High Energy Physics - Phenomenology · Physics 2011-01-04 Francisco del Aguila , Adrian Carmona , Jose Santiago

We study whether the nonmonotonic behavior found in the differential cross section of the phi-meson photoproduction near threshold can be described by a resonance. Namely, we add a resonance to a model consisting of Pomeron and (pi,eta)…

High Energy Physics - Phenomenology · Physics 2014-11-21 Alvin Kiswandhi , Ju-Jun Xie , Shin Nan Yang

The elementary particles are modeled as harmonic oscillator excitations of transverse U(1) gauge fields propagating at v = c, with open and closed string-like propagation paths. One, two and three node states represent the leptons, bosons,…

High Energy Physics - Theory · Physics 2007-05-23 Roger C. Millikan

We search for a new gauge boson $Z'$ that couples only to heavy leptons and their corresponding neutrinos in the process $e^{+} e^{-} \rightarrow Z'(\rightarrow \mu^{+}\mu^{-}) \mu^{+}\mu^{-}$, using a 643 fb$^{-1}$ data sample collected by…

High Energy Physics - Experiment · Physics 2022-07-12 T. Czank , I. Jaegle , A. Ishikawa , I. Adachi , K. Adamczyk , H. Aihara , D. M. Asner , T. Aushev , R. Ayad , V. Babu , S. Bahinipati , P. Behera , J. Bennett , F. Bernlochner , M. Bessner , V. Bhardwaj , B. Bhuyan , T. Bilka , J. Biswal , A. Bobrov , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , M. Campajola , L. Cao , D. Červenkov , M. -C. Chang , A. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , Y. Choi , S. Choudhury , D. Cinabro , S. Das , N. Dash , G. De Nardo , R. Dhamija , F. Di Capua , Z. Doležal , T. V. Dong , S. Eidelman , T. Ferber , D. Ferlewicz , B. G. Fulsom , R. Garg , V. Gaur , A. Garmash , A. Giri , P. Goldenzweig , B. Golob , O. Grzymkowska , Y. Guan , K. Gudkova , C. Hadjivasiliou , O. Hartbrich , K. Hayasaka , H. Hayashii , M. T. Hedges , M. Hernandez Villanueva , T. Higuchi , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , G. Inguglia , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , E. -J. Jang , S. Jia , Y. Jin , C. W. Joo , K. K. Joo , K. H. Kang , G. Karyan , T. Kawasaki , H. Kichimi , C. Kiesling , B. H. Kim , C. H. Kim , D. Y. Kim , K. -H. Kim , S. H. Kim , Y. -K. Kim , P. Kodyš , I. Komarov , T. Konno , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , M. Kumar , K. Kumara , Y. -J. Kwon , Y. -T. Lai , J. S. Lange , I. S. Lee , S. C. Lee , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , D. Liventsev , T. Luo , C. MacQueen , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , F. Metzner , K. Miyabayashi , R. Mizuk , G. B. Mohanty , S. Mohanty , T. Mori , M. Mrvar , R. Mussa , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , H. Ono , Y. Onuki , P. Pakhlov , G. Pakhlova , T. Pang , S. Pardi , H. Park , S. -H. Park , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , V. Popov , E. Prencipe , M. T. Prim , M. Röhrken , A. Rostomyan , N. Rout , G. Russo , D. Sahoo , S. Sandilya , A. Sangal , L. Santelj , T. Sanuki , V. Savinov , G. Schnell , J. Schueler , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , M. Shapkin , C. Sharma , V. Shebalin , C. P. Shen , J. -G. Shiu , B. Shwartz , A. Sokolov , E. Solovieva , S. Stanič , M. Starič , Z. S. Stottler , M. Sumihama , T. Sumiyoshi , W. Sutcliffe , M. Takizawa , K. Tanida , Y. Tao , F. Tenchini , K. Trabelsi , M. Uchida , S. Uehara , T. Uglov , K. Uno , S. Uno , P. Urquijo , R. Van Tonder , G. Varner , A. Vossen , C. H. Wang , E. Wang , M. -Z. Wang , P. Wang , S. Watanuki , E. Won , X. Xu , B. D. Yabsley , H. Yamamoto , W. Yan , S. B. Yang , H. Ye , J. Yelton , J. H. Yin , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov

I examine the possibility that the third generation fermion masses are determined by an exact fixed point of the minimal supersymmetric SU(5) model. When one-loop supersymmetric thresholds are included, this unified fixed point successfully…

High Energy Physics - Phenomenology · Physics 2009-11-07 Javier Ferrandis