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Related papers: LHC-scale left-right symmetry and unification

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The apparent unification of gauge couplings around 10^16 GeV is one of the strong arguments in favor of Supersymmetric extensions of the Standard Model (SM). In this contribution two new analyses of the gauge coupling running, the latter…

High Energy Physics - Phenomenology · Physics 2009-11-11 Dimitri Bourilkov

We explain how physics in the kaon sector proves useful in setting constraints in models where the gluino mass is below 2 TeV, while the other supersymmetric particles are in the range $\sim(3-10)$ TeV. We also discuss the signals of these…

High Energy Physics - Phenomenology · Physics 2012-07-17 L. Velasco-Sevilla

Maximally supersymmetric SO(10) and SU(6) unified theories are constructed on the orbifold T^2/(Z_2 x Z'_2), with one length scale R_5 taken much larger than the other, R_6. The effective theory below 1/R_6 is found to be the highly…

High Energy Physics - Phenomenology · Physics 2009-09-29 Lawrence J. Hall , Yasunori Nomura

The alternative $SU(4) \otimes SU(2)_L \otimes SU(2)_R$ gauge model, which allows unification of the quarks and leptons at the TeV scale, is studied in detail. We discuss the implications for nucleon decay, B and K rare meson decays and…

High Energy Physics - Phenomenology · Physics 2009-10-31 R. Foot , G. Filewood

We embed the minimal left-right model SU(2)_L*SU(2)_R* U(1)_{B-L} into an SU(4)_W gauge group, and break the unified group via five-dimensional S^1/(Z_2*Z_2) orbifolding. Leptons are fitted into SU(4)_W multiplets and located on a symmetry…

High Energy Physics - Phenomenology · Physics 2009-09-07 Csaba Balazs , Tianjun Li , Fei Wang , Jin Min Yang

In the Minimal Supersymmetric Standard Model, the higgsinos can have masses around the electroweak scale, while the other supersymmetric particles have TeV-scale masses. This happens in models of gauge-mediated SUSY breaking with a high…

High Energy Physics - Phenomenology · Physics 2012-05-08 F. Brümmer

We discuss the minimal supersymmetric $U(1)_{B-L}\times U(1)_R$ extension of the standard model. Gauge couplings unify as in the MSSM, even if the scale of $U(1)_{B-L}\times U(1)_R$ breaking is as low as order TeV and the model can be…

High Energy Physics - Phenomenology · Physics 2012-11-20 Martin Hirsch , Werner Porod , Laslo Reichert , Florian Staub

We explore a realistic supersymmetric SU(2)_L \times SU(2)_R \times U(1)_B-L model spontaneously broken at around 10^12 GeV. The presence of D and F-flat directions gives rise to TeV mass doubly charged particles which can be found at the…

High Energy Physics - Phenomenology · Physics 2011-05-12 Shahida Dar , Qaisar Shafi , Arunansu Sil

We propose an effective left-right-right-left model with a parity breaking scale around a few TeV. One of the main achievements of the model is that the mirror fermions as well as the mirror gauge sector simultaneously could be at TeV…

High Energy Physics - Phenomenology · Physics 2017-02-08 Gauhar Abbas

A self-consistent version of the left-right (LR) symmetric model is used to examine tree- as well as one-loop level radiative corrections to the muon decay. It is shown that constraints on the heavy sector of the model parameters are…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. Czakon , J. Gluza , J. Hejczyk

The string landscape suggests that the supersymmetry breaking scale can be high, and then the simplest low energy effective theory is the Standard Model (SM). Considering grand unification scale supersymmetry breaking, we show that gauge…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , Jing Jiang , Paul Langacker , Tianjun Li

We show that left-right symmetric models can easily accommodate stable TeV-scale dark matter particles without the need for an ad-hoc stabilizing symmetry. The stability of a newly introduced multiplet arises either accidentally as in the…

High Energy Physics - Phenomenology · Physics 2015-09-21 Julian Heeck , Sudhanwa Patra

We propose a non-supersymmetric $\mathrm{E}_{6}$ GUT with the scalar sector consisting of $\mathbf{650}\oplus \mathbf{351'} \oplus \mathbf{27}$. Making use of the first representation for the initial symmetry breaking to an intermediate…

High Energy Physics - Phenomenology · Physics 2024-04-01 K. S. Babu , Borut Bajc , Vasja Susič

With minimal field content and for an interesting range of the supersymmetric Higgs mixing parameter, 0.5 < tan^2 \beta < 2, the superpartner mass scale, \tilde{m}, is found to be at the intermediate scale, ~ 10^{10 \pm 1} GeV, near where…

High Energy Physics - Phenomenology · Physics 2015-06-18 Lawrence J. Hall , Yasunori Nomura

Tests of gauge coupling unification require knowledge of thresholds between the weak scale and the high scale of unification. If these scales are far separated, as is the case in most unification scenarios considered in the literature, the…

High Energy Physics - Phenomenology · Physics 2015-04-29 Sebastian A. R. Ellis , James D. Wells

Despite the successes of the Standard Model of particle physics, it is known to suffer from a number of deficiencies. Several of these can be addressed within non-supersymmetric theories of grand unification based on $\mathrm{SO}(10)$.…

High Energy Physics - Phenomenology · Physics 2020-09-14 Davide Meloni , Tommy Ohlsson , Marcus Pernow

We argue that Left-Right parity symmetry $\mathcal{P}$ can arise as a discrete remnant of a unified gauge symmetry. The high-energy unification necessarily includes the gauging of the Lorentz symmetry, bringing into the game gravitational…

High Energy Physics - Theory · Physics 2022-06-15 Alessio Maiezza , Fabrizio Nesti

We show that unification of the three gauge couplings can be realized consistently in a class of non-supersymmetric SO(10) models with a one-step breaking to the Standard Model if a color-sextet scalar field survives down to the TeV scale.…

High Energy Physics - Phenomenology · Physics 2015-06-05 K. S. Babu , R. N. Mohapatra

We develop a minimal left-right symmetric model based on the gauge group $SU(3)_C \otimes SU(2)_L \otimes SU(2)_R \otimes U(1)_{B-L}$ wherein the Higgs triplets conventionally employed for symmetry breaking are replaced by Higgs doublets.…

High Energy Physics - Phenomenology · Physics 2020-12-29 K. S. Babu , Anil Thapa

We reconsider the idea of identifying the Higgs field as the internal component of a gauge field in the flat space R^4XS^1/Z_2, by relaxing the constraint of having unbroken SO(4,1) Lorentz symmetry in the bulk. In this way, we show that…

High Energy Physics - Phenomenology · Physics 2009-11-11 Giuliano Panico , Marco Serone , Andrea Wulzer