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Related papers: R-Parity Violation and Light Neutralinos at SHiP a…

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A review of supersymmetric dark matter in minimal supergravity unification with R-parity invariance and with radiative breaking of the electro-weak symmetry is given. The analysis shows the lightest neutralino is the LSP over most of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Pran Nath , R. Arnowitt

R-parity violation in the supersymmetric standard model could be the origin of neutrino masses and mixing accounting for the atmospheric and solar neutrino oscillations. More interestingly, this hypothesis may be tested in future colliders…

High Energy Physics - Phenomenology · Physics 2016-11-03 Eung Jin Chun

Both electroweak precision measurements and simple supersymmetric extensions of the standard model prefer a mass of the Higgs boson less than the experimental lower limit of 114 GeV. We show that supersymmetric models with R parity…

High Energy Physics - Phenomenology · Physics 2008-11-26 Linda M. Carpenter , David E. Kaplan , Eun-Jung Rhee

R-parity-violating supersymmetry (with a conserved baryon number B) provides a framework for particle physics with lepton number (L) violating interactions. We examine in detail the structure of the most general R-parity-violating…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yuval Grossman , Howard E. Haber

We present a study of sensitivity of the R-parity violating SUSY searches with the upgraded D0 detector in Run II of the Fermilab Tevatron, within a SUGRA framework. We considered the lightest neutralino as an LSP that decays into a lepton…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Banerjee , N. K. Mondal , V. S. Narasimham , N. Parua

This paper describes the physics case for a new fixed target facility at CERN SPS. The SHiP (Search for Hidden Particles) experiment is intended to hunt for new physics in the largely unexplored domain of very weakly interacting particles…

High Energy Physics - Phenomenology · Physics 2016-10-27 Sergey Alekhin , Wolfgang Altmannshofer , Takehiko Asaka , Brian Batell , Fedor Bezrukov , Kyrylo Bondarenko , Alexey Boyarsky , Nathaniel Craig , Ki-Young Choi , Cristóbal Corral , David Curtin , Sacha Davidson , André de Gouvêa , Stefano Dell'Oro , Patrick deNiverville , P. S. Bhupal Dev , Herbi Dreiner , Marco Drewes , Shintaro Eijima , Rouven Essig , Anthony Fradette , Björn Garbrecht , Belen Gavela , Gian F. Giudice , Dmitry Gorbunov , Stefania Gori , Christophe Grojean , Mark D. Goodsell , Alberto Guffanti , Thomas Hambye , Steen H. Hansen , Juan Carlos Helo , Pilar Hernandez , Alejandro Ibarra , Artem Ivashko , Eder Izaguirre , Joerg Jaeckel , Yu Seon Jeong , Felix Kahlhoefer , Yonatan Kahn , Andrey Katz , Choong Sun Kim , Sergey Kovalenko , Gordan Krnjaic , Valery E. Lyubovitskij , Simone Marcocci , Matthew Mccullough , David McKeen , Guenakh Mitselmakher , Sven-Olaf Moch , Rabindra N. Mohapatra , David E. Morrissey , Maksym Ovchynnikov , Emmanuel Paschos , Apostolos Pilaftsis , Maxim Pospelov , Mary Hall Reno , Andreas Ringwald , Adam Ritz , Leszek Roszkowski , Valery Rubakov , Oleg Ruchayskiy , Jessie Shelton , Ingo Schienbein , Daniel Schmeier , Kai Schmidt-Hoberg , Pedro Schwaller , Goran Senjanovic , Osamu Seto , Mikhail Shaposhnikov , Brian Shuve , Robert Shrock , Lesya Shchutska , Michael Spannowsky , Andy Spray , Florian Staub , Daniel Stolarski , Matt Strassler , Vladimir Tello , Francesco Tramontano , Anurag Tripathi , Sean Tulin , Francesco Vissani , Martin W. Winkler , Kathryn M. Zurek

Using the example of selected decays driven by R-parity-violating supersymmetric operators, we demonstrate how strong final-state interactions can be controlled quantitatively with high precision, thus allowing for a more accurate…

High Energy Physics - Phenomenology · Physics 2013-02-04 J. T. Daub , H. K. Dreiner , C. Hanhart , B. Kubis , U. -G. Meißner

The recent LHC discovery of a Higgs-like boson at 126 GeV has important consequences for SUSY, pushing the spectrum of strong-interacting supersymmetric particles to high energies, very difficult to probe at the LHC. This gives extra…

High Energy Physics - Phenomenology · Physics 2015-06-12 Maria Eugenia Cabrera , J. Alberto Casas , Bryan Zaldivar

We consider implications of the loop process sneutrino -> gamma gamma in the MSSM with R-parity violation for future experiments, where the sneutrino is produced as the only supersymmetric particle. We present a scenario for the R-parity…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. Bar-Shalom , G. Eilam , A. Soni , J. Wudka

We investigate a neutrino mass model in which the neutrino data is accounted for by bilinear R-parity violating supersymmetry with anomaly mediated supersymmetry breaking. We focus on the CERN Large Hadron Collider (LHC) phenomenology,…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. de Campos , M. A. Diaz , O. J. P. Eboli , M. B. Magro , W. Porod , S. Skadhauge

A search for the electroweak production of pairs of charged sleptons or charginos decaying into two-lepton final states with missing transverse momentum is presented. Two simplified models of $R$-parity-conserving supersymmetry are…

High Energy Physics - Experiment · Physics 2023-07-13 ATLAS Collaboration

Within the R-parity violating minimal supersymmetric standard model (MSSM), we use a hierarchical ansatz for the lepton-number violating trilinear Yukawa couplings by relating them to the corresponding Higgs-Yukawa couplings. This ansatz…

High Energy Physics - Phenomenology · Physics 2013-05-30 M. Hanussek , J. S. Kim

We study the potential to observe CP-violating effects in SUSY cascade decay chains at the LHC. We consider squark and gluino production followed by subsequent decays into neutralinos with a three-body leptonic decay in the final step.…

High Energy Physics - Phenomenology · Physics 2010-01-22 G. Moortgat-Pick , K. Rolbiecki , J. Tattersall , P. Wienemann

In R parity violating theories, there does not exist the {\it stable} lightest supersymmetric particle (LSP). The LSP, $\chi$, of MSSM decays to lighter ordinary particles with dimension 6 effective R violating interaction terms. Since the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jihn E. Kim , Bumseok Kyae , Jong Dae Park

We study the pair production of right selectrons at a 500 GeV $e^-e^-$ collider followed by their decay into an electron and a lightest neutralino. This lightest neutralino decays into multifermion final states in the presence of…

High Energy Physics - Phenomenology · Physics 2011-03-23 Dilip Kumar Ghosh , Sourov Roy

In the recently proposed `split supersymmetry' scenario, the squark and slepton masses are allowed to be at a high scale while the gauginos and Higgsinos are within a TeV. We show that in a theory with broken R-parity, the parameter space…

High Energy Physics - Phenomenology · Physics 2010-04-05 Sudhir Kumar Gupta , Partha Konar , Biswarup Mukhopadhyaya

R-parity conservation is an ad-hoc assumption in the most popular versions of supersymmetric scenarios. Hence R-parity violation (RPV) not only is allowed but, if induced by bilinear terms (bRPV), it also provides an explanation for the…

High Energy Physics - Phenomenology · Physics 2014-04-30 Vasiliki A. Mitsou

Radiation amplitude zeros have long been used to test the Standard Model. Here, we consider the supersymmetric radiation amplitude zero in chargino-neutralino associated production, which can be observed at the luminosity upgraded LHC. Such…

High Energy Physics - Phenomenology · Physics 2012-05-22 JoAnne L. Hewett , Ahmed Ismail , Thomas G. Rizzo

Dark matter is a well-established theoretical addition to the Standard Model supported by many observations in modern astrophysics and cosmology. In this context, the existence of weakly interacting massive particles represents an appealing…

High Energy Physics - Experiment · Physics 2021-06-03 SHiP Collaboration

Heavy right-handed neutrinos (RHNs) provide the simplest explanation for the origin of light neutrino masses and mixings. If the RHN masses are at or below the weak scale, direct experimental discovery of these states is possible at…

High Energy Physics - Phenomenology · Physics 2016-08-26 Brian Batell , Maxim Pospelov , Brian Shuve
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