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Related papers: On Discrete R-Symmetries in MSSM and its Extension…

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The well-known Giudice-Masiero mechanism explains the presence of a mu term of the order of the gravitino mass, but does not explain why the holomorphic mass term is absent in the superpotential. We discuss anomaly-free discrete symmetries…

High Energy Physics - Phenomenology · Physics 2015-06-05 Mu-Chun Chen , Michael Ratz , Christian Staudt , Patrick K. S. Vaudrevange

We construct an N=1 supersymmetric three-family flipped SU(5) model from type IIA orientifolds on $T^6/(\Z_2\times \Z_2)$ with D6-branes intersecting at general angles. The model is constrained by the requirement that Ramond-Ramond tadpoles…

High Energy Physics - Theory · Physics 2009-11-11 C. -M. Chen , G. V. Kraniotis , V. E. Mayes , D. V. Nanopoulos , J. W. Walker

It is shown that embedding a four-dimensional flipped SU(5) model in a five-dimensional SO(10) model, preserves the best features of both flipped SU(5) and SO(10). The missing partner mechanism, which naturally achieves both doublet-triplet…

High Energy Physics - Phenomenology · Physics 2011-05-12 S. M. Barr , Ilja Dorsner

Anomalies of discrete R-symmetries appearing in heterotic orbifold models are studied. We find that the mixed anomalies for different gauge groups satisfy the universal Green-Schwarz (GS) condition, indicating that these anomalies are…

High Energy Physics - Phenomenology · Physics 2008-11-26 Takeshi Araki , Kang-Sin Choi , Tatsuo Kobayashi , Jisuke Kubo , Hiroshi Ohki

Recently it was shown that there is a unique Z_4^R symmetry for the MSSM which allows the Yukawa couplings and dimension five neutrino mass operator, forbids the mu term and commutes with SO(10). This Z_4^R symmetry contains matter parity…

High Energy Physics - Theory · Physics 2015-05-20 Rolf Kappl , Bjoern Petersen , Stuart Raby , Michael Ratz , Roland Schieren , Patrick K. S. Vaudrevange

The strategy for assigning $Z_{4R}$ parity in the string compactification is presented. For the visible sector, an anti-SU(5) (flipped-SU(5)) grand unification (GUT) model with three families is used to reduce the number of representations…

High Energy Physics - Phenomenology · Physics 2021-07-21 Jihn E. Kim

The conditions for the cancellation of all gauge, gravitational, and mixed anomalies of $N=1$ supersymmetric models in six dimensions are reviewed and illustrated by a number of examples. Of particular interest are models that cannot be…

High Energy Physics - Theory · Physics 2009-10-28 John H. Schwarz

We show that more than two generations of quarks and leptons are required to have an anomaly free discrete R-symmetry larger than R-parity, provided that the supersymmetric Standard Model can be minimally embedded into a grand unified…

High Energy Physics - Phenomenology · Physics 2013-06-13 Jason L. Evans , Masahiro Ibe , John Kehayias , Tsutomu T. Yanagida

We investigate matrix models in three dimensions where the global $\text{SU}(N)$ symmetry acts via the adjoint map. Analyzing their ground state which is homogeneous in space and can carry either a unique or multiple fixed charges, we show…

High Energy Physics - Theory · Physics 2018-08-01 Orestis Loukas

We propose a renormalisable model based on $A_4$ family symmetry with an $SU(5)$ grand unified theory (GUT) which leads to the minimal supersymmetric standard model (MSSM) with a two right-handed neutrino seesaw mechanism. Discrete…

High Energy Physics - Phenomenology · Physics 2015-07-01 Fredrik Björkeroth , Francisco J. de Anda , Ivo de Medeiros Varzielas , Stephen F. King

We study global anomalies of discrete gauge symmetries in six-dimensional supergravities and their realizations in F-theory. We explicitly construct a discrete Green-Schwarz mechanism that depends on the choice of a coupling constant and on…

High Energy Physics - Theory · Physics 2023-04-05 Markus Dierigl , Paul-Konstantin Oehlmann , Thorsten Schimannek

In the minimal supersymmetric Standard Model with seesaw neutrino masses we show how R-parity can emerge naturally as a discrete gauge symmetry. The same discrete symmetry explains the smallness of the \mu-term (the Higgsino mass parameter)…

High Energy Physics - Phenomenology · Physics 2010-04-05 K. S. Babu , Ilia Gogoladze , Kai Wang

In order that discrete symmetries should not be violated by gravitational effects, it is necessary to gauge them. In this paper we discuss the gauging of $\Z_N$ from the breaking of a high energy $SU(N)$ gauge symmetry, and derive…

High Energy Physics - Phenomenology · Physics 2009-10-22 P. L. White

In particle physics model building discrete symmetries are often invoked to forbid unwanted or dangerous couplings. A classical example is the R-parity of the MSSM, which guarantees the absence of dimension four baryon- and lepton-number…

High Energy Physics - Theory · Physics 2015-05-28 Mikel Berasaluce-González , Luis E. Ibáñez , Pablo Soler , Angel M. Uranga

We study the supersymmetric spontaneous symmetry breaking of SO(10) into SU(3)xSU(2)xU(1) for the most physically interesting cases of SU(5) or flipped SU(5)xU(1) intermediate symmetries. The first case is more easily realized while the…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. Buccella , C. A. Savoy

In string theory, there are no continuous global symmetries. Discrete symmetries frequently appear, and these can often be understood as unbroken subgroups of larger, spontaneously broken gauge symmetries (discrete gauge symmetries). In…

High Energy Physics - Theory · Physics 2007-05-23 D. A. MacIntire

A new supersymmetric grand unified model based on the gauge group $SU(5)\times SU(5)$ is discussed. The model has the feature that the conventional seesaw mechanism for neutrino masses is implemented using the $(15, 1)+(1,\bar{15)}$…

High Energy Physics - Phenomenology · Physics 2009-10-28 R. N. Mohapatra

We examine discrete gauge symmetries in axionic extensions of the SSM which provide a solution of the $\mu$-problem. Automatic-PQ symmetry and proton stability are shown to be guaranteed by certain discrete symmetries. Focusing on the…

High Energy Physics - Phenomenology · Physics 2009-10-22 E. J. Chun , A. Lukas

I remark that the weak mixing angle in the standard model may be computed even in the absence of a grand unification symmetry. In particular, if there is an additional gauged $U(1)$ symmetry at some large scale which can be made…

High Energy Physics - Phenomenology · Physics 2016-09-01 L. E. Ibáñez

``Anomalous'' U(1) gauge symmetry with Green-Schwarz anomaly cancellation mechanism is discussed in the orbifold construction of four-dimensional heterotic string models. Some conditions are given as criteria to have ``anomalous'' U(1) in…

High Energy Physics - Theory · Physics 2016-09-06 Tatsuo Kobayashi , Hiroaki Nakano