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Related papers: Building SO$_{10}$- models with $\mathbb{D}_{4}$ s…

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We consider Grand Unified Theories based on $SO(10)$ which originate from $M$ theory on $G_2$ manifolds. In this framework we are naturally led to a novel solution of the doublet-triplet splitting problem involving an extra $\overline{{\bf…

High Energy Physics - Phenomenology · Physics 2015-09-02 Miguel Crispim Romão

We consider d=10 N=1 supersymmetry algebra with maximal number of tensor charges Z and introduce a class of orbits of Z, invariant w.r.t. the $T_8$ subgroup of massless particles' little group $T_8\ltimes SO(8)$. For that class of orbits we…

High Energy Physics - Theory · Physics 2009-11-10 H. Mkrtchyan , R. Mkrtchyan

A three-dimensional simple N=1 supergravity theory with a supersymmetric sigma-model on the coset E_{8(+8)} / SO(16) is constructed. Both bosons and fermions in the matter multiplets are in the spinorial 128-representation of SO(16) with…

High Energy Physics - Theory · Physics 2009-11-07 Hitoshi Nishino , Subhash Rajpoot

In this work we study an SO(10) GUT model with minimum Higgs representations belonging only to the 210 and 16 dimensional representations of SO(10). We add a singlet fermion S in addition to the usual 16 dimensional representation…

High Energy Physics - Phenomenology · Physics 2009-11-11 Kaushik Bhattacharya , C. R. Das , Bipin R. Desai , G. Rajasekaran , Utpal Sarkar

For supersymmetric GUT models from heterotic string theory, built from a stable holomorphic SU(n) vector bundle $V$ on a Calabi-Yau threefold $X$, the net amount of chiral matter can be computed by a Chern class computation. Corresponding…

High Energy Physics - Theory · Physics 2015-05-30 Gottfried Curio

We consider SUSY SO(10) models in which SUSY breaking occurs via an F-term which does not transform as an SO(10) singlet. This results in non-universal GUT-scale gaugino masses leading to a different pattern of sparticle masses from what is…

High Energy Physics - Phenomenology · Physics 2009-11-07 Nidal Chamoun , Chao-Shang Huang , Chun Liu , Xiao-Hong Wu

We present GUT models based on an $SU(5)\times SU(5)$ GUT group. These models maintain the main successes of simple-group GUTs but permit simple solutions to the doublet-triplet splitting problem. Moreover, GUT breaking is triggered by…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yael Shadmi

An intriguing correspondence between four-qubit systems and simple singularity of type $D_4$ is established. We first consider an algebraic variety $X$ of separable states within the projective Hilbert space…

Mathematical Physics · Physics 2015-06-18 Frédéric Holweck , Jean-Gabriel Luque , Michel Planat

We present the first example of a grand unified theory (GUT) with a modular symmetry interpreted as a family symmetry. The theory is based on supersymmetric $SU(5)$ in 6d, where the two extra dimensions are compactified on a…

High Energy Physics - Phenomenology · Physics 2020-02-04 Francisco J. de Anda , Stephen F. King , Elena Perdomo

Let $D_{n}$ be the dihedral group of order $n$. The structure of the unit group $U(F(C_3 \times D_{10}))$ of the group algebra $F(C_3 \times D_{10})$ over a finite field $F$ of characteristic $3$ is given in \cite{sh13}. In this article,…

Rings and Algebras · Mathematics 2021-06-07 Meena Sahai , Sheere Farhat Ansari

A complete supersymmetric SO(10) model is constructed, which is the most general consistent with certain $R$, discrete, and $U(1)$ flavor symmetries. The desired vacuum of the theory has vevs which lie in particular directions of group…

High Energy Physics - Phenomenology · Physics 2016-09-01 L. J. Hall , S. Raby

Conventional SO(10) models involve more than one scale for a complete breaking of the GUT symmetry requiring further assumptions on the VEVs of the Higgs fields that enter in the breaking to achieve viable models. Recent works where the…

High Energy Physics - Phenomenology · Physics 2015-06-05 Pran Nath

We propose a bottom-up approach to the building of particle physics models from string theory. Our building blocks are Type II D-branes which we combine appropriately to reproduce desirable features of a particle theory model: 1) Chirality…

High Energy Physics - Theory · Physics 2009-10-31 G. Aldazabal , L. E. Ibanez , F. Quevedo , A. M. Uranga

We perform the first convergent Bayesian global fits of 4D Composite Higgs Models with partially-composite third generation quarks and leptons based on the minimal $SO(5) \rightarrow SO(4)$ symmetry breaking pattern. We consider two models…

High Energy Physics - Phenomenology · Physics 2024-07-02 Ethan Carragher , Kenn Shern Goh , Wei Su , Martin White , Anthony G. Williams

Let group generators having finite-dimensional representation be realized as Hermitian linear differential operators without nhomogeneous terms as takes place, for example, for the SO(n) group. Then orresponding group Hamiltonians…

solv-int · Physics 2007-05-23 O. B. Zaslavskii

We discuss an $SU(5)$ Grand Unified Theory (GUT) based on the 10d orbifold $(\mathbb{T}^2)^3/(\mathbb{Z}_4\times\mathbb{Z}_2)$ plus three modular $S_4$ groups with moduli at respective fixed points $i,i+2,\omega=e^{2i\pi/3}$. The resulting…

High Energy Physics - Phenomenology · Physics 2024-06-03 Francisco J. de Anda , Stephen F. King

We consider a supersymmetric Grand Unified Theory (GUT) based on the gauge group SO(10) suggested by Aulakh et al., which features two--step intermediate symmetry breaking, $SO(10) \to SU(4)_C \times SU(2)_L \times SU(2)_R \to SU(3)_C…

High Energy Physics - Phenomenology · Physics 2010-04-28 Manuel Drees , Ju Min Kim

We construct a five dimensional supersymmetric SO(10)$\times$D$_3$ grand unified model with an $S^1/(Z_2 \times Z^\prime_2)$ orbifold as the extra dimension. The orbifold breaks half of the supersymmetry and breaks the SO(10) gauge symmetry…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hyung Do Kim , Stuart Raby , Leslie Schradin

In early 1930s Seifert and Threlfall classified up to conjugacy the finite subgroups of $\mathrm{SO}(4)$, this gives an algebraic classification of orientable spherical 3-orbifolds. For the most part, spherical 3-orbifolds are Seifert…

Geometric Topology · Mathematics 2016-07-22 Mattia Mecchia , Andrea Seppi

We compute characteristic numbers of elliptically fibered fourfolds with multisections or non-trivial Mordell-Weil groups. We first consider the models of type E$_{9-d}$ with $d=1,2,3,4$ whose generic fibers are normal elliptic curves of…

High Energy Physics - Theory · Physics 2018-08-23 Mboyo Esole , Monica Jinwoo Kang
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