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We discuss chiral supersymmetric compactifications of the SO(32) heterotic string on Calabi-Yau manifolds equipped with direct sums of stable bundles with structure group U(n). In addition we allow for non-perturbative heterotic…

High Energy Physics - Theory · Physics 2010-02-03 Ralph Blumenhagen , Gabriele Honecker , Timo Weigand

We give a detailed description of the model construction procedures about our new approach to the family structure of the standard model. SM-like chiral fermion spectra, largely "derivable" from the gauge anomaly constraints, are formulated…

High Energy Physics - Phenomenology · Physics 2009-10-28 Otto C. W. Kong

Intersecting Dp-branes often give rise to chiral fermions living on their intersections. We study the construction of four-dimensional chiral gauge theories by considering configurations of type II D(3+n)-branes wrapped on non-trivial…

High Energy Physics - Theory · Physics 2009-10-09 G. Aldazabal , S. Franco , L. E. Ibanez , R. Rabadan , A. M. Uranga

We consider theories with gauged chiral fermions in which there are abelian anomalies, and no nonabelian anomalies (but there may be nonabelian gauge fields present). We construct an associated theory that is gauge invariant,…

High Energy Physics - Theory · Physics 2008-02-03 Paul Federbush

We extend a classification of irreducible, almost-commutative geometries whose spectral action is dynamically non-degenerate, to internal algebras that have six simple summands. We find essentially four particle models: An extension of the…

High Energy Physics - Theory · Physics 2014-11-18 Jan-Hendrik Jureit , Christoph A. Stephan

Any N=2 superconformal field theory (SCFT) in four dimensions has a sector of operators related to a two-dimensional chiral algebra containing a Virasoro sub-algebra. Moreover, there are well-known examples of isolated SCFTs whose chiral…

High Energy Physics - Theory · Physics 2016-11-23 Matthew Buican , Takahiro Nishinaka

We provide what we believe is the minimal three family ${\cal N} = 1$ SUSY and conformal Pati-Salam Model from type IIB superstring theory. This $Z_3$ orbifolded AdS$\otimes S^5$ model has long lived protons and has potential…

High Energy Physics - Phenomenology · Physics 2008-11-26 James B. Dent , Thomas W. Kephart

We discuss the possibility of obtaining a non-abelian discrete flavor symmetry from an underlying continuous, possibly gauged, flavor symmetry SU(2) or SU(3) through spontaneous symmetry breaking. We consider all possible cases, where the…

High Energy Physics - Phenomenology · Physics 2009-09-28 A. Adulpravitchai , A. Blum , M. Lindner

Let $\Gamma=\mathrm{Cay}(G,S)$ be a Cayley digraph on a group $G$ and let $A=\mathrm{Aut}(\Gamma)$. The Cayley index of $\Gamma$ is $|A:G|$. It has previously been shown that, if $p$ is a prime, $G$ is a cyclic $p$-group and $A$ contains a…

Combinatorics · Mathematics 2017-03-08 Luke Morgan , Joy Morris , Gabriel Verret

We study the chiral rings in N=2 and N=4 superconformal algebras. The chiral primary states of N=2 superconformal algebras realized over hermitian triple systems are given. Their coset spaces G/H are hermitian symmetric which can be compact…

High Energy Physics - Theory · Physics 2014-11-18 Murat Gunaydin

Use of the AdS/CFT correspondence to arrive at phenomenological gauge field theories is dicussed, focusing on the orbifolded case without supersymmetry. An abelian orbifold with the finite group $Z_{p}$ can give rise to a $G = SU(N)^p$…

High Energy Physics - Theory · Physics 2007-05-23 Paul H. Frampton

We study D-branes on a three complex dimensional nonabelian orbifold ${\bf C}^3/\Gamma$ with $\Gamma$ a finite subgroup of SU(3). We present general formulae necessary to obtain quiver diagrams which represent the gauge group and the…

High Energy Physics - Theory · Physics 2010-02-03 Tomomi Muto

We study the classification problem for anomaly-free 6D $\mathcal N=(1,0)$ supergravities with a gauged abelian R-symmetry and one tensor multiplet. We present eleven new models with gauge group $G_{\mathrm{non-Abelian}}\times U(1)_R$ that…

High Energy Physics - Theory · Physics 2026-05-19 Katrin Becker , Qi You

We construct four dimensional three generation non-supersymmetric $SU(3)_c \times SU(2)_L \times U(1)_Y$ intersecting D6-brane models with $\nu_R$\rq{s}. At three stacks we find exactly the MSSM chiral fermion matter spectrum. At 4-,…

High Energy Physics - Theory · Physics 2014-02-19 Christos Kokorelis

Motivated by orbifold grand unified theories, we construct a class of three-family Pati-Salam models in a Z6 abelian symmetric orbifold with two discrete Wilson lines. These models have marked differences from previously-constructed…

High Energy Physics - Phenomenology · Physics 2009-11-10 Tatsuo Kobayashi , Stuart Raby , Ren-Jie Zhang

We study the realization of non-Abelian discrete gauge symmetries in 4d field theory and string theory compactifications. The underlying structure generalizes the Abelian case, and follows from the interplay between gaugings of non-Abelian…

High Energy Physics - Theory · Physics 2015-06-05 Mikel Berasaluce-Gonzalez , Pablo G. Camara , Fernando Marchesano , Diego Regalado , Angel M. Uranga

We provide a general overview of the current state of the art in four dimensional three generation model building proposals - using intersecting D-brane toroidal compactifications [without fluxes] of IIA, IIB string theories - which have…

High Energy Physics - Theory · Physics 2007-05-23 Christos Kokorelis

We give a classification of 3-family SO(10) and E_6 grand unification in string theory within the framework of conformal field theory and asymmetric orbifolds. We argue that the construction of such models in the heterotic string theory…

High Energy Physics - Theory · Physics 2009-10-30 Zurab Kakushadze , S. -H. Henry Tye

We study anomalies of non-Abelian discrete symmetries; which part of non-Abelian group is anomaly free and which part can be anomalous. It is found that the anomaly-free elements of the group $G$ generate a normal subgroup $G_0$ of $G$ and…

High Energy Physics - Theory · Physics 2022-03-14 Tatsuo Kobayashi , Hikaru Uchida

The success of SU(5)-like gauge coupling unification boundary conditions $g_3^2=g_2^2=5/3 g_1^2$ has biased most attempts to embed the SM interactions into a unified structure. After discussing the limitations of the orthodox approach, we…

High Energy Physics - Phenomenology · Physics 2011-03-23 G. Aldazabal , L. E. Ibanez , F. Quevedo