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Related papers: TeV-scale GUTs

200 papers

To solve the hierarchy problem of the Higgs mass, it may be suggested that there are no an intermediate scale up to the Planck scale except for the TeV scale. For this motivation, we investigate possibilities of gauge coupling unification…

High Energy Physics - Phenomenology · Physics 2015-04-28 Yuya Yamaguchi

A brief review is given of recent developments related to the Higgs signal and its implications for supersymmetry in the supergravity grand unification framework. The Higgs data indicates that the allowed parameter space largely lies on…

High Energy Physics - Phenomenology · Physics 2012-08-02 Pran Nath

In the present paper we demonstrate the possibility of the [SUSY(5)]^3 SUSY unification at the energy scale $\mu_{GUT}\approx 10^{18.3} GeV$ with the value of GUT inverse finestructure constant $\alpha_{GUT}^{-1}\approx 34.4$, which is very…

High Energy Physics - Theory · Physics 2007-05-23 L. Laperashvili , D. A. Ryzhikh

This work presents a general formalism to analyze a generic bulk scalar field in a multiple warped extra-dimensional model with arbitrary number of extra dimensions. The Kaluza-Klein mass modes along with the self-interaction couplings are…

General Relativity and Quantum Cosmology · Physics 2014-06-05 Sumanta Chakraborty , Soumitra SenGupta

A TeV-scale scenario is constructed in an attempt to understand the relationship between quark and lepton masses. This scenario combines a model of early (TeV) unification of quarks and leptons with the physics of large extra dimensions. It…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. Q. Hung

We discuss the structure of general Anisotropic Compactification in Type I D=4, N=1 string theory. It is emphasized that, in this context, a possible interpretation of M_{Planck} as ``dual'' to (at least) one of the Kaluza-Klein or Windings…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. Donini , S. Rigolin

We consider the possibility of grand unification of the $\mathrm{ SU(3)_c \otimes SU(3)_L \otimes U(1)_X}$ model in an SU(6) gauge unification group. Two possibilities arise. Unlike other conventional grand unified theories, in SU(6) one…

High Energy Physics - Phenomenology · Physics 2016-10-07 Frank F. Deppisch , Chandan Hati , Sudhanwa Patra , Utpal Sarkar , Josè W. F. Valle

We discuss how a model for the electroweak interactions without a Higgs could be embedded into a grand unified theory. The requirement of a non-trivial fixed point in the SU(2) sector of the weak interactions together with the requirement…

High Energy Physics - Phenomenology · Physics 2015-06-04 Stephen M. Barr , Xavier Calmet

Higher-dimensional models of grand unification allow us to relate the top Yukawa coupling y_t to the gauge coupling g. The tree level relation y_t=g at the scale of grand unification implies, in the framework of the MSSM, a rather small…

High Energy Physics - Phenomenology · Physics 2010-05-28 Pierre Hosteins , Rolf Kappl , Michael Ratz , Kai Schmidt-Hoberg

We study a five dimensional nonsupersymmetric SU(3) gauge theory compactified on $M^4\times S^1/Z_2$. The gauge hierarchy is discussed in the scenario of the gauge-Higgs unification. We present two models in which the large gauge hierarchy…

High Energy Physics - Phenomenology · Physics 2017-08-23 Kazunori Takenaga

The possibility of achieving a gauge coupling grand unification by increasing the QCD degrees of freedom at higher energies is investigated. When confronted with precision low-energy data, the generic weak-mixing angle relation…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. C. Branco , J. -M. Gerard , R. Gonzalez Felipe , B. M. Nobre

Proton decay is a smoking gun signature of Grand Unified Theories (GUTs). Searches by Super-Kamiokande have resulted in stringent limits on the GUT symmetry breaking scale. The large-scale multipurpose neutrino experiments DUNE,…

High Energy Physics - Phenomenology · Physics 2021-01-19 Stephen F. King , Silvia Pascoli , Jessica Turner , Ye-Ling Zhou

The use of the AdS/CFT correspondence to arrive at quiver 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 $G = SU(N)^p$ gauge…

High Energy Physics - Theory · Physics 2017-08-23 P. H. Frampton

After a brief review of the motivations for grand unification, I discuss the main challenges facing realistic SUSY GUT model building. Achieving doublet-triplet splitting without fine--tuning is chief among them. Symmetry breaking should…

High Energy Physics - Phenomenology · Physics 2011-11-10 K. S. Babu

In the minimal supersymmetric standard model, the three gauge couplings appear to unify at a mass scale near $2 \times 10^{16}$ GeV. We investigate the possibility that intermediate scale particle thresholds modify the running couplings so…

High Energy Physics - Phenomenology · Physics 2016-09-01 Stephen P. Martin , Pierre Ramond

The full parameter space of supergravity grand unified theory with $SU(5)$ type $p \rightarrow \bar{\nu} K$ proton decay is analysed using renormalization group induced electroweak symmetry breaking under the restrictions that the universal…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Arnowitt , Pran Nath

Recently it has been pointed out that the characteristic quantum-gravity scale could be as low as the weak scale in theories with gravity propagating in higher dimensions. The observed smallness of Newton's constant is a consequence of the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Gian F. Giudice , Riccardo Rattazzi , James D. Wells

The effects of extra dimensions on gauge coupling unification is studied. We start with a comparison between power law running of the gauge couplings in models with extra dimensions and logarithmic running that happens in many realistic…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Pérez-Lorenzana , R. N. Mohapatra

There is a unique $SU(4) \otimes SU(2)_L \otimes SU(2)_R$ gauge model which allows quarks and leptons to be unified at the TeV scale. It is already known that the neutrino masses arise radiatively in the model and are naturally light. We…

High Energy Physics - Phenomenology · Physics 2009-11-07 T. L. Yoon , R. Foot

Arkani-Hamed, Dimopoulos, and Dvali have proposed that the fundamental gravitational scale is close to 1 TeV, and that the observed weakness of gravity at long distances is explained by the presence of large extra compact dimensions. If…

High Energy Physics - Phenomenology · Physics 2009-10-31 Schuyler Cullen , Maxim Perelstein , Michael E. Peskin