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In a recent paper, we pointed out that mixing of the light neutrinos with heavy gauge singlet states could reconcile the Z-pole data from e+e- colliders and the nu_mu (anti-nu_mu) scattering data from the NuTeV experiment at Fermilab. We…

High Energy Physics - Phenomenology · Physics 2007-05-23 Will Loinaz , Naotoshi Okamura , Saifuddin Rayyan , Tatsu Takeuchi , L. C. R. Wijewardhana

We investigate the generation of the baryon asymmetry of the Universe within a SUSY SU(5) x T' model of flavour, which gives rise to realistic masses and mixing patterns for quarks and leptons. The model employs the see-saw mechanism for…

High Energy Physics - Phenomenology · Physics 2012-03-21 A. Meroni , E. Molinaro , S. T. Petcov

We propose an $SO(10)$ supersymmetric grand unified theory (SUSY GUT), where the $SO(10)$ gauge symmetry breaks down to $SU(3)_c \times SU(2)_L \times U(1)_Y\times U(1)_{X}$ at the GUT scale and $U(1)_X$ is radiatively broken at the…

High Energy Physics - Phenomenology · Physics 2015-05-20 Junji Hisano , Yu Muramatsu , Yuji Omura , Masato Yamanaka

We study the phenomenological implications of sfermion flavour mixing in supersymmetry in the context of Non-Minimal Flavour Violation (NMFV). We study the general flavour mixing hypothesis, parametrizing the squark and slepton mass…

High Energy Physics - Phenomenology · Physics 2013-12-18 M. Arana-Catania

We demonstrate that natural supersymmetry is readily realized in the framework of SU(4)_c \times SU(2)_L \times SU(2)_R with non-universal gaugino masses. Focusing on ameliorating the little hierarchy problem, we explore the parameter space…

High Energy Physics - Phenomenology · Physics 2015-06-12 Ilia Gogoladze , Fariha Nasir , Qaisar Shafi

In a (0,1) supersymmetric (SUSY) six-dimensional gauge theory, a gauge fermion gives rise to box anomalies. These anomalies are completely canceled by assuming a vector multiplet of (1,1) SUSY. With a T^2/Z_3 orbifold compactification of…

High Energy Physics - Phenomenology · Physics 2017-08-23 T. Watari , T. Yanagida

We analyze the most natural formulations of the minimal lepton flavour violation hypothesis compatible with a type-I seesaw structure with three heavy singlet neutrinos N, and satisfying the requirement of being predictive, in the sense…

High Energy Physics - Phenomenology · Physics 2011-08-03 Rodrigo Alonso , Gino Isidori , Luca Merlo , Luis Alfredo Muñoz , Enrico Nardi

The see-saw mechanism of neutrino mass generation, when incorporated in supersymmetric theories with supergravity mediated supersymmetry breaking, results in low-energy lepton-flavour violation arising from the soft supersymmetry breaking…

High Energy Physics - Phenomenology · Physics 2009-11-10 Bruce A. Campbell , David W. Maybury , Brandon Murakami

We present a new mechanism to explain naturally and through a common flavour symmetry the mildly hierarchical neutrino masses with large mixings and the hierarchical Yukawa matrices with small mixing angles. Although this mechanism is not…

High Energy Physics - Phenomenology · Physics 2007-05-23 Oscar Vives

We investigate Lepton-Flavor Violating (LFV) decays of Higgs to muon-tau in the supersymmetric economical 3-3-1 (SUSYE331) model. In the presence of flavor mixing in sleptons {mu,tau} and large values of v/v', the ratio of Br(H…

High Energy Physics - Phenomenology · Physics 2012-07-11 P. T. Giang , L. T. Hue , D. T. Huong , H. N. Long

Pursuing a bottom-up approach to explore which flavor symmetry could serve as an explanation of the observed fermion masses and mixings, we discuss an extension of the standard model (SM) where the flavor structure for both quarks and…

High Energy Physics - Phenomenology · Physics 2011-05-05 C. Hagedorn , M. Lindner , R. N. Mohapatra

We demonstrate that an $SU(2)_L\times U(1)_Y$ model with extended Higgs sector gives rise to bi-maximal neutrino mixing through the incorporation of SO(3) flavour symmetry and discrete symmetry. The neutrino and the charged lepton masses…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ambar Ghosal

U(1) family symmetries have led to successful predictions of the fermion mass spectrum and the mixing angles of the hadronic sector. In the context of the supersymmetric unified theories, they further imply a non-trivial mass structure for…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. E. Gomez , G. K. Leontaris , S. Lola , J. D. Vergados

Among three typical energy scales, a neutrino mass scale ($m_\nu\sim$ 0.1 eV), a GUT scale ($M_{GUT}\sim 10^{16}$ GeV), and a TeV-scale ($M_{NP}\sim$ 1 TeV), there is a fascinating relation of $M_{NP}\simeq \sqrt{m_\nu\cdot M_{GUT}}$.The…

High Energy Physics - Phenomenology · Physics 2013-05-30 Naoyuki Haba , Kunio Kaneta , Yasuhiro Shimizu

The observed pattern of neutrino mixing may be the result of a 2-3($ \mu- \tau$) symmetry in the leptonic sector. We consider a two Higgs doublet model with a 2-3 symmetry in the down type quark and the charged lepton sector. The breaking…

High Energy Physics - Phenomenology · Physics 2009-11-11 Alakabha Datta , Patrick J. O'Donnell

We show how approximate Minimal Flavour Violation (MFV) can emerge from an SU(5) Supersymmetric Grand Unified Theory (SUSY GUT) supplemented by an S4 x U(1) family symmetry, which provides a good description of all quark and lepton…

High Energy Physics - Phenomenology · Physics 2016-03-23 Maria Dimou , Stephen F. King , Christoph Luhn

We calculate quark and lepton masses and quark mixing angles in the framework of a supersymmetric SU(4)$\otimes$SU(2)$_L\otimes$SU(2)$_R$ model where the gauge group is broken at 10$^{16}$ GeV. The model predicts third family top-bottom-tau…

High Energy Physics - Phenomenology · Physics 2010-11-01 B. C. Allanach , S. F. King

We propose a model for the vector-like lepton to explain the small muon mass by a seesaw mechanism, based on lepton-specific two Higgs doublet models with a local $U(1)'$ symmetry. There is no bare muon mass for a nonzero $U(1)'$ charge of…

High Energy Physics - Phenomenology · Physics 2021-12-22 Hyun Min Lee , Jiseon Song , Kimiko Yamashita

Successful Soft Leptogenesis (SL) requires a relatively low mass scale for the SU(2) singlet neutrinos of $10^5-10^8$ GeV. However, conventional SL (unflavoured) requires an unnaturally small soft supersymmetry(SUSY)-breaking bilinear $B…

High Energy Physics - Phenomenology · Physics 2015-03-17 Chee Sheng Fong

We present a scenario wherein the anomalous U(1) D-term of string origin triggers supersymmetry breaking and generates naturally a Split Supersymmetry spectrum. When the gaugino and the Higgsino masses (which are of the same order of…

High Energy Physics - Phenomenology · Physics 2009-11-11 K. S. Babu , Ts. Enkhbat , Biswarup Mukhopadhyaya