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Related papers: Lessons from an Extended Heterotic Mini-Landscape

200 papers

In spite of its many successes, the Standard Model makes many empirical assumptions in the Higgs and fermion sectors for which a deeper theoretical basis is sought. Starting from the usual gauge symmetry $u(1) \times su(2) \times su(3)$…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. M. Chan , S. T. Tsou

We provide a new class of Z_N x Z_M heterotic orbifolds on non-factorisable tori, whose boundary conditions are defined by Lie lattices. Generally, point groups of these orbifolds are generated by Weyl reflections and outer automorphisms of…

High Energy Physics - Theory · Physics 2009-11-13 Kei-Jiro Takahashi

The totality of neutrino-oscillation phenomena appears to require the existence of a light singlet neutrino. As pointed out recently, this can be naturally accommodated with a specific extra U(1) factor contained in the superstring-inspired…

High Energy Physics - Phenomenology · Physics 2009-10-28 E. Keith , Ernest Ma

We explore the phenomenology of a class of models with anomaly-mediated supersymmetry breaking. These models retain the successful flavor properties of the minimal scenario while avoiding the tachyons. The mass spectrum is predicted in…

High Energy Physics - Phenomenology · Physics 2008-11-26 Riccardo Rattazzi , Alessandro Strumia , James D. Wells

Our contribution sets out to investigate the phenomenology of a gauge model based on an $SU_{L}(2) \times U_{R}(1)_{J} \times U(1)_{K}$-symmetry group. The model can accommodate in its distinct phases - by virtue of different…

High Energy Physics - Phenomenology · Physics 2018-02-19 M. J. Neves , J. A. Helayël-Neto

The Landau problem is discussed in two similar but still different non-commutative frameworks. The ``standard'' one, where the coupling to the gauge field is achieved using Poisson brackets, yields all Landau levels. The ``exotic''…

High Energy Physics - Theory · Physics 2008-11-26 P. A. Horvathy

For a smooth cubic fourfold Y, we study the moduli space M of semistable objects of Mukai vector $2\lambda_1+2\lambda_2$ in the Kuznetsov component of Y. We show that with a certain choice of stability conditions, M admits a symplectic…

Algebraic Geometry · Mathematics 2020-07-29 Chunyi Li , Laura Pertusi , Xiaolei Zhao

We study the relationship between exotic R^4's and Stein surfaces as it applies to smoothing theory on more general open 4-manifolds. In particular, we construct the first known examples of large exotic R^4's that embed in Stein surfaces.…

Geometric Topology · Mathematics 2016-07-20 Julia Bennett

We consider the renormalizable $SO(5)/SO(4)$ $\sigma$-model, in which the Higgs particle has a pseudo-Nambu-Goldstone boson character, and explore what the minimal field extension required to implement the Peccei-Quinn symmetry (PQ) is,…

High Energy Physics - Phenomenology · Physics 2019-09-18 I. Brivio , M. B. Gavela , S. Pascoli , R. del Rey , S. Saa

The effective field theory of the minimal Low Scale Orientifold Models is developed. It describes universal features of related orientifold vacua in string theory. It contains, beyond the Standard Model fields, an MSSM-like Higgs sector and…

High Energy Physics - Phenomenology · Physics 2010-04-05 Claudio Coriano' , Nikos Irges , Elias Kiritsis

We present a plausible mechanism for the origin of the $XYZ$ mesons in the heavy meson spectra within a standard quark-model picture. We discuss the conditions required for the existence of four--quark bound states or resonances…

High Energy Physics - Phenomenology · Physics 2015-07-30 J. Vijande , A. Valcarce

We present a detailed analysis of the eclectic flavor structure of the two-dimensional $\mathbb Z_2$ orbifold with its two unconstrained moduli $T$ and $U$ as well as $\mathrm{SL}(2,\mathbb Z)_T\times \mathrm{SL}(2,\mathbb Z)_U$ modular…

High Energy Physics - Theory · Physics 2021-07-07 Alexander Baur , Moritz Kade , Hans Peter Nilles , Saul Ramos-Sanchez , Patrick K. S. Vaudrevange

We study the phenomenology of the strong-coupling limit of $E_8\times E_8$ heterotic string obtained from M-theory, using a Calabi-Yau compactification. After summarizing the standard embedding results, we concentrate on non-standard…

High Energy Physics - Phenomenology · Physics 2010-11-19 D. G. Cerdeno , C. Munoz

We describe a new type of discrete symmetry that relates heterotic-string models. It is based on the spectral flow operator which normally acts within a general N=(2,2) model and we use this operator to construct a map between N=(2,0)…

High Energy Physics - Theory · Physics 2015-08-03 Panos Athanasopoulos

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 go beyond the Standard Model guided by presymmetry, the discrete electroweak quark-lepton symmetry hidden by topological effects which explain quark fractional charges as in condense matter physics. Partners of the particles of the…

High Energy Physics - Phenomenology · Physics 2015-05-14 Ernesto A. Matute

We extend the littlest modular seesaw to a Grand Unified scenario based on $SU(5)$ endowed with three modular $S_4$ symmetries. We leverage symmetry protected zeroes in the leptonic and down quark sectors to suppress deviations to the…

High Energy Physics - Phenomenology · Physics 2023-09-29 Ivo de Medeiros Varzielas , Steve F. King , Miguel Levy

We construct a supersymmetric standard model in the context of the $Z_{12-I}$ orbifold compactification of the heterotic string theory. The gauge group is $SU(3)_c\times SU(2)_L\times U(1)_Y\times U(1)^4\times[SO(10)\times U(1)^3]'$. We…

High Energy Physics - Phenomenology · Physics 2010-10-27 Jihn E. Kim , Ji-Hun Kim , Bumseok Kyae

In this paper, globally N=1 supersymmetric configurations of intersecting D6-branes on the Z6-orientifold are discussed, involving also fractional branes. It turns out rather miraculously that one is led almost automatically to just ONE…

High Energy Physics - Theory · Physics 2014-11-18 Gabriele Honecker , Tassilo Ott

Intersecting stacks of supersymmetric fractional branes on the Z_6' orientifold may be used to construct the supersymmetric Standard Model. If a,b are the stacks that generate the SU(3)_{colour} and SU(2)_L gauge particles, then, in order…

High Energy Physics - Theory · Physics 2019-08-19 David Bailin , Alex Love