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Related papers: Superheavy Supersymmetry

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If a light gaugino sector exists in the supersymmetric standard model then the mass of lightest neutralino may be of the order of 1 GeV or less. As a consequence of neutral flavor violation in supersymmetric theories $B_s$-meson may decay…

High Energy Physics - Phenomenology · Physics 2009-09-25 Rathin Adhikari , Biswarup Mukhopadhyaya

A search for supersymmetry in the context of general gauge-mediated (GGM) breaking with the lightest neutralino as the next-to-lightest supersymmetric particle and the gravitino as the lightest is presented. The data sample corresponds to…

High Energy Physics - Experiment · Physics 2012-08-27 CMS Collaboration

We propose a new framework for mediating supersymmetry breaking through an extra dimension. It predicts positive scalar masses and solves the supersymmetric flavor problem. Supersymmetry breaks on a ``source'' brane that is spatially…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Elazzar Kaplan , Graham D. Kribs , Martin Schmaltz

Supersymmetric models with a high supersymmetry breaking scale give, in general, large contributions to epsilon_K and/or to various electric dipole moments, even when contributions to CP conserving, flavor changing processes are…

High Energy Physics - Phenomenology · Physics 2014-11-17 Michael Dine , Erik Kramer , Yosef Nir , Yael Shadmi

The problem of generating light neutrinos within supersymmetric models is discussed. It is shown that the hierarchy of scales induced by supersymmetry breaking can give rise to suppression factors of the correct order of magnitude to…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. Borzumati , K. Hamaguchi , Y. Nomura , T. Yanagida

Supersymmetry is one of the most plausible extensions of the Standard Model, since it is well motivated by the hierarchy problem, supported by measurements of the gauge coupling strengths, consistent with the suggestion from precision…

High Energy Physics - Phenomenology · Physics 2007-05-23 John Ellis

It is argued that in the context of supersymmetry, the Strong CP Problem is most naturally seen as an aspect (particularly severe) of the whole complex of flavor-violating and CP-violating problems of supersymmetry. It is shown that certain…

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

The current measurement of the Higgs mass, the ubiquitous nature of loop-suppressed gaugino masses in gravity-mediated supersymmetry breaking, relic dark matter density from $\sim$ TeV mass gauginos, together with the success of…

High Energy Physics - Phenomenology · Physics 2013-01-01 Nima Arkani-Hamed , Arpit Gupta , David E. Kaplan , Neal Weiner , Tom Zorawski

We consider a simple setup with light squarks which is free from the gravitino and SUSY flavor problems. In our setup, a SUSY breaking sector is sequestered from the matter and gauge sectors, and it only couples to the Higgs sector directly…

High Energy Physics - Phenomenology · Physics 2020-05-20 Tsutomu T. Yanagida , Wen Yin , Norimi Yokozaki

In supersymmetric models the mass of the stops can be considered as the naturalness measure of the theory. Roughly, the lighter the stops are, the more natural the theory is. Both, the absence of supersymmetric signals at experiment and the…

High Energy Physics - Phenomenology · Physics 2016-10-17 Mateo Garcia-Pepin

Anomaly mediation solves the supersymmetric flavor and CP problems. This is because the superconformal anomaly dictates that supersymmetry breaking is transmitted through nearly flavor-blind infrared physics that is highly predictive and UV…

High Energy Physics - Phenomenology · Physics 2009-09-29 Ryuichiro Kitano , Graham D. Kribs , Hitoshi Murayama

The heavy right-handed neutrinos in supersymmetric models can act as the source of lepton flavor violation (LFV). LFV processes like $ \mu \rightarrow e \gamma $, $ \tau \rightarrow \mu \gamma $, $ \tau \rightarrow e \gamma $ is an…

High Energy Physics - Phenomenology · Physics 2020-04-03 Gayatri Ghosh

Motivated by the absence, so far, of any direct signal of conventional low-energy supersymmetry, we explore the consequences of making the lightest Higgs boson in supersymmetry relatively heavy, up to about 300 GeV, in the most…

High Energy Physics - Phenomenology · Physics 2008-11-26 Riccardo Barbieri , Lawrence J. Hall , Yasunori Nomura , Vyacheslav S. Rychkov

This review summarizes the state of the art in searches for supersymmetry at colliders on the eve of the LHC era. Supersymmetry is unique among extensions of the standard model in being motivated by naturalness, dark matter, and force…

High Energy Physics - Experiment · Physics 2014-11-18 Jonathan L. Feng , Jean-Francois Grivaz , Jane Nachtman

We construct a complete, realistic, and natural UV completion of minimal conformal technicolor that explains the origin of quark and lepton masses and mixing angles. As in "bosonic technicolor", we embed conformal technicolor in a…

High Energy Physics - Phenomenology · Physics 2015-05-20 Jared A. Evans , Jamison Galloway , Markus A. Luty , Ruggero Altair Tacchi

The cosmological constant problem is a failure of naturalness and suggests that a fine-tuning mechanism is at work, which may also address the hierarchy problem. An example -- supported by Weinberg's successful prediction of the…

High Energy Physics - Theory · Physics 2009-11-10 Nima Arkani-Hamed , Savas Dimopoulos

Supersymmetry is still a viable explanation for the muon $g-2$ anomaly, if the sleptons and electroweak gauginos are $\mathcal{O}(100)$ GeV. However, for supersymmetry breaking masses this light, the SUSY flavor and CP-problem are…

High Energy Physics - Phenomenology · Physics 2023-03-22 Jason L. Evans , Tsutomu T. Yanagida , Norimi Yokozaki

We begin an exploration of the physics associated with the general CP-conserving MSSM with Minimal Flavor Violation, the pMSSM. The 19 soft SUSY breaking parameters in this scenario are chosen so as to satisfy all existing experimental and…

High Energy Physics - Phenomenology · Physics 2010-04-23 C. F. Berger , J. S. Gainer , J. L. Hewett , T. G. Rizzo

We investigate Supersymmetric models where neither R parity nor lepton number is imposed. Neutrino masses can be kept highly suppressed compared to the electroweak scale if the $\mu$-terms in the superpotential are aligned with the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Tom Banks , Yuval Grossman , Enrico Nardi , Yosef Nir

A generic feature of gauge-mediated supersymmetry breaking models is that the gravitino is the lightest supersymmetric particle (LSP). In order not to overclose the universe, the gravitino LSP should be light enough (~ 1 keV), or…

High Energy Physics - Phenomenology · Physics 2009-11-10 Gi-Chol Cho , Yosuke Uehara
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