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In the simplest compactification, we discuss the intermediate unification in M-theory on $S^1/Z_2$, and point out that we can push the eleven dimension Planck scale to the TeV range if the gauge coupling in the hidden sector is super weak,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tianjun Li

We study compactification of five dimensional ungauged N=2 supergravity coupled to vector- and hypermultiplets on orbifold $S^1/Z_2$. In the model the vector multiplets scalar manifold is arbitrary while the hypermultiplet scalars span a…

High Energy Physics - Theory · Physics 2010-11-19 F. P. Zen , B. E. Gunara , Arianto , H. Zainuddin

We present a new supersymmetric index for three-dimensional ${\cal N}=2$ gauge theories defined on $\Sigma \times S^1$, where $\Sigma$ is a spindle, with twist or anti-twist for the $R$-symmetry background gauge field. We start examining…

High Energy Physics - Theory · Physics 2024-02-20 Matteo Inglese , Dario Martelli , Antonio Pittelli

Within D=4 N=1 supergravity theory we obtain an effective theory of the thin wall limit for a flat domain wall configuration, interpolating between isolated supersymmetric extrema of the matter potential. We focus on the Z_2 symmetric flat…

High Energy Physics - Phenomenology · Physics 2009-09-17 Francisco A. Brito , Mirjam Cvetic , SangChul Yoon

If scale invariance is a classical symmetry then both the Planck scale and the weak scale should emerge as quantum effects. We show that this can be realized in simple scale invariant theories with a hidden sector. The weak/Planck scale…

High Energy Physics - Phenomenology · Physics 2008-11-26 Robert Foot , Archil Kobakhidze , Kristian L. McDonald , Raymond R. Volkas

We consider N=2 supergravity theories that have the same spectrum as the R+R^2 supergravity, as predicted from the off-shell counting of degrees of freedom. These theories describe standard N=2 supergravity coupled to one or two long…

High Energy Physics - Theory · Physics 2014-07-15 Anna Ceresole , Gianguido Dall'Agata , Sergio Ferrara , Mario Trigiante , Antoine Van Proeyen

We present a renormalizable theory of scalars in which the low energy effective theory contains a pseudo-Goldstone Boson with a compact field space of 2{\pi} F and an approximate discrete shift symmetry Z_Q with Q>>1, yet the number of…

High Energy Physics - Phenomenology · Physics 2016-04-13 David E. Kaplan , Riccardo Rattazzi

We consider four supergravities with 16+16, 32+32, 64+64, 128+128 degrees of freedom displaying some curious properties: (1) They exhibit minimal supersymmetry (N=1, 2, 2, 1) but maximal rank (r=7, 6, 4, 0) of the scalar coset in D=4, 5, 7,…

High Energy Physics - Theory · Physics 2011-02-23 M. J. Duff , S. Ferrara

We present the locally supersymmetric formulation of unimodular gravity theory in D (1\le D \le 11) dimensions, namely supergravity theory with the metric tensor whose determinant is constrained to be unity. In such a formulation, the usual…

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

Semiclassical approximation to the Wheeler-DeWitt equation which corresponds to gravity with a minimally coupled scalar field has been performed. To the leading order, vacuum Einstein's equation along with the functional Schrodinger…

General Relativity and Quantum Cosmology · Physics 2017-07-26 Abhik Kumar Sanyal

We introduce a $N=1$ supergravity model with a very simple hidden sector coupled to the electroweak gauge and Higgs sectors of the MSSM. At the classical level, supersymmetry and $SU(2)\times U(1)$ are both spontaneously broken, with…

High Energy Physics - Theory · Physics 2014-07-16 Hui Luo , Fabio Zwirner

In the framework of linearized non-minimal supergravity (20/20), we present the embedding of the $R + R^2$ model and we analyze its field spectrum. As usual, the auxiliary fields of the Einstein theory now become propagating, giving rise to…

High Energy Physics - Theory · Physics 2015-06-23 Fotis Farakos , Alex Kehagias , Konstantinos Koutrolikos

I will report on a top-down approach relating N=2, D=4 pure supergravity with non-trivial boundary behavior to a (2+1)-dimensional analog model which is able to describe the electronic properties of graphene-like materials. This is…

High Energy Physics - Theory · Physics 2025-02-25 Laura Andrianopoli

The minimal supersymmetric standard model, when extended to embed the seesaw mechanism, obtains two dimensionful parameters in its superpotential: the mu parameter and the right-handed neutrino mass M_N. These mass parameters, belonging to…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. Demir , Y. Farzan

The structure theory for the quadratic algebra generated by first and second order constants of the motion for 2D second order superintegrable systems with nondegenerate (3-parameter) and or 2-parameter potentials is well understood, but…

Mathematical Physics · Physics 2009-01-23 Ernest G. Kalnins , Jonathan M. Kress , Willard Miller , Sarah Post

The supersymmetric completion of higher-derivative operators often requires introducing corrections to the scalar potential. In this paper we study these corrections systematically in the context of theories with $\mathcal{N}=1$ global and…

High Energy Physics - Theory · Physics 2018-04-20 David Ciupke

We construct the dilaton Weyl multiplet for $N=2$ conformal supergravity in four dimensions. Beginning from an on-shell vector multiplet coupled to the standard Weyl multiplet, the equations of motion can be used to eliminate the…

High Energy Physics - Theory · Physics 2018-04-18 Daniel Butter , Subramanya Hegde , Ivano Lodato , Bindusar Sahoo

We review the general gauged N=2 supergravity coupled to an arbitrary number of vector multiplets and hypermultiplets. We consider two different models where N=2 supersymmetry is broken to N=1 spontaneously, one has a U(1) vector multiplet…

High Energy Physics - Theory · Physics 2007-05-23 Kazunobu Maruyoshi

We consider the simplest and most economic version among the proposed non-minimal supersymmetric models, in which the $\mu$-parameter is promoted to a singlet superfield, whose all self-couplings are absent from the renormalizable…

High Energy Physics - Phenomenology · Physics 2009-10-31 C. Panagiotakopoulos , A. Pilaftsis

Why are the cosmological constant, electroweak and Planck scales so different? This ``double hierarchy" problem, where $\Lambda \ll M^2_{EW} \ll M^2_p$, is one of the most pressing in fundamental physics. We show that in a theory of $N$…

High Energy Physics - Theory · Physics 2021-06-02 Nima Khosravi