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Related papers: Effective R-parity violation from supersymmetry br…

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We summarize two sets of signals at HERA in supersymmetric models with explicitly broken R-parity. (1) The resonant production of single squarks through an operator $L_1Q_i{ \bar D}_j$. (2) The MSSM production of a squark and a slepton…

High Energy Physics - Phenomenology · Physics 2007-05-23 Herbi Dreiner

Motivated by the recent experimental data of the E787, E949 and E865 collaborations and by the difference between the standard model (SM) prediction and data, we consider in detail R-parity violating (RPV) supersymmetric contributions to K…

High Energy Physics - Phenomenology · Physics 2007-05-23 Julien Welzel

The magnitude of R-parity violating coupling constants depends on which direction in the space of weak doublets with hypercharge = -2 corresponds to the Higgs. To address this ``basis dependence'', one can construct combinations of coupling…

High Energy Physics - Phenomenology · Physics 2009-10-31 Sacha Davidson

Here, we give a broad overview of the more natural spectra allowed by the LHC when UDD R-parity violation is allowed. Because R-parity violation removes the missing energy signals in colliders, the experimental constraints on the gluino,…

High Energy Physics - Phenomenology · Physics 2015-06-12 Biplob Bhattacherjee , Jason L. Evans , Masahiro Ibe , Shigeki Matsumoto , Tsutomu T. Yanagida

Supersymmetric theories with an R-parity generally yield a striking missing energy signature, with cascade decays concluding in a neutralino that escapes the detector. In theories where R-parity is broken the missing energy is replaced with…

High Energy Physics - Phenomenology · Physics 2015-06-05 Joshua T. Ruderman , Tracy R. Slatyer , Neal Weiner

In supersymmetric models where the mu problem is solved via discrete R-symmetries, then both the global U(1)_{PQ} (Peccei-Quinn, needed to solve the strong CP problem) and R-parity conservation (RPC, needed for proton stability) are…

High Energy Physics - Phenomenology · Physics 2025-05-27 Howard Baer , Vernon Barger , Jessica Bolich , Dibyashree Sengupta , Kairui Zhang

In this talk, I will present the general structure of RPV couplings when a Froggatt-Nielsen horizontal symmetry is responsible for the flavor structure of both the SM and the MSSM. For sub-TeV ({\it natural}) SUSY, lepton number must be an…

High Energy Physics - Phenomenology · Physics 2013-10-01 Angelo Monteux

Within the framework of an SU(5) SUSY GUT model, a possible general form of the neutrino mass matrix induced by R-parity violation is investigated. The model has matter fields \bar{5}'_{L}+5'_{L} in addition to the ordinary matter fields…

High Energy Physics - Phenomenology · Physics 2009-11-10 Yoshio Koide

Flavour and CP violations that the neutrino-seesaw couplings of types I, II, and III induce radiatively in the soft massive parameters of the minimal supersymmetric SU(5) model, made realistic by nonrenormalizable operators, are analyzed.…

High Energy Physics - Phenomenology · Physics 2011-05-12 Francesca Borzumati , Toshifumi Yamashita

Formation of the $s$-channel slepton resonances at LEP2 or Tevatron at current energies is an exciting possibility in R-parity violating SUSY models. Existing LEP2 and Tevatron data can be exploited to look for sleptons, or to derive bounds…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Kalinowski

In this short reappraisal of spontaneous lepton number violation in a supersymmetric scenario implemented through singlet sneutrino vacuum expectation value (VEV), we contribute with two new things in the context where the lepton number…

High Energy Physics - Phenomenology · Physics 2010-10-13 Gautam Bhattacharyya , Palash B. Pal

We propose a theoretical framework for R-parity violation. It is realized by a class of Calabi--Yau compactification of Heterotic string theory. Trilinear R-parity violation in superpotential is either absent or negligibly small without an…

High Energy Physics - Phenomenology · Physics 2013-05-29 Minoru Kuriyama , Hiroto Nakajima , Taizan Watari

We construct the complete SU(2) parity-violating (PV) $\pi, N, \Delta$ interaction Lagrangian with one derivative, and calculate the chiral corrections to the PV Yukawa $NN\pi$ coupling constant $h_\pi$ through ${\cal O}(1/\Lambda_\chi^3)$…

High Energy Physics - Phenomenology · Physics 2009-10-31 Shi-Lin Zhu , S. J. Puglia , B. R. Holstein , M. J. Ramsey-Musolf

We consider supersymmetric extensions of the standard model in which the usual $R$ or matter parity gets replaced by another $R$ or non-$R$ discrete symmetry that explains the observed longevity of the nucleon and solves the $\mu$ problem…

High Energy Physics - Phenomenology · Physics 2015-01-14 Mu-Chun Chen , Michael Ratz , Volodymyr Takhistov

Supersymmetric models with R-parity violation (RPV) have become more popular following the lack of any excess of missing energy events at the 8 TeV LHC. To identify such models, the suggested searches generally rely on the decay products of…

High Energy Physics - Phenomenology · Physics 2015-01-12 N. -E. Bomark , A. Kvellestad , S. Lola , P. Osland , A. R. Raklev

Studies of R-parity violating (RPV) supersymmetry typically assume that nucleon stability is protected by approximate baryon number (B) or lepton number (L) conservation. We present a new class of RPV models that violate B and L…

High Energy Physics - Phenomenology · Physics 2015-04-30 Cyrus Faroughy , Siddharth Prabhu , Bob Zheng

Minimal R-parity violating supergravity predicts a value for $alpha_s(M_Z)$ smaller than in the case with conserved R-parity, and therefore closer to the experimental world average. We show that the R-parity violating effect on the…

High Energy Physics - Phenomenology · Physics 2009-09-17 M. A. Diaz , J. Ferrandis , J. C. Romao , J. W. F. Valle

Electroweak precision data at LEP are used to place bounds on some $\lambda'$-type ($L$-violating) and $\lambda''$-type ($B$-violating) $R$-parity violating supersymmetric Yukawa couplings. We consider one-loop corrections (triangles and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Gautam Bhattacharyya

The dimuon plus dijet signal is analyzed in the top squark pair production at Tevatron Run-II experiment and the total event rate is compared with the existing dimuon data. This comparison rules out top squark mass upto 188(104) GeV for the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Subhendu Chakrabarti , Monoranjan Guchait , N. K. Mondal

We summarize the signals at HERA in supersymmetric models with explicitly broken R-parity. As the most promising case, we consider in detail the resonant production of single squarks through an operator $L_1Q_i{ \bar D}_j$, a production…

High Energy Physics - Phenomenology · Physics 2009-10-22 Jon Butterworth , Herbert Dreiner