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We consider a supersymmetric model motivated by a SO(10) grand unified theory: the gauge sector near the supersymmetry scale consists of SU(3)_c x SU(2)_L x U(1)_R x U(1)_{B-L}. We embed this model in minimal gauge mediation and incorporate…

High Energy Physics - Phenomenology · Physics 2013-08-06 Manuel E. Krauss , Werner Porod , Florian Staub

We propose a novel mechanism of electroweak symmetry breaking in supersymmetric models, as the one recently discussed by Birkedal, Chacko and Gaillard, in which the Standard Model Higgs doublet is a pseudo-Goldstone boson of some global…

High Energy Physics - Phenomenology · Physics 2009-11-10 Piotr H. Chankowski , Adam Falkowski , Stefan Pokorski , Jakub Wagner

Assuming that supersymmetry exists well above the weak scale, we derive the full one-loop matching conditions between the SM and the supersymmetric theory, allowing for the possibility of an intermediate Split-SUSY scale. We also compute…

High Energy Physics - Phenomenology · Physics 2014-09-18 Emanuele Bagnaschi , Gian F. Giudice , Pietro Slavich , Alessandro Strumia

In this PhD thesis, we first look at some manifestations of CP violation, such as electric dipole moments (EDMs) of elementary particles, both in the weak sector in the presence of neutrino masses (absent in the SM) as well as in the strong…

High Energy Physics - Phenomenology · Physics 2021-01-29 Selim Touati

There are many possibilities for new physics beyond the Standard Model that feature non-standard Higgs sectors. These may introduce new sources of CP violation, and there may be mixing between multiple Higgs bosons or other new scalar…

High Energy Physics - Phenomenology · Physics 2022-10-26 S. Kraml , E. Accomando , A. G. Akeroyd , E. Akhmetzyanova , J. Albert , A. Alves , N. Amapane , M. Aoki , G. Azuelos , S. Baffioni , A. Ballestrero , V. Barger , A. Bartl , P. Bechtle , G. Belanger , A. Belhouari , R. Bellan , A. Belyaev , P. Benes , K. Benslama , W. Bernreuther , M. Besancon , G. Bevilacqua , M. Beyer , M. Bluj , S. Bolognesi , M. Boonekamp , F. Borzumati , F. Boudjema , A. Brandenburg , T. Brauner , C. P. Buszello , J. M. Butterworth , M. Carena , D. Cavalli , G. Cerminara , S. Y. Choi , B. Clerbaux , C. Collard , J. A. Conley , A. Deandrea , S. De Curtis , R. Dermisek , A. De Roeck , G. Dewhirst , M. A. Diaz , J. L. Diaz-Cruz , D. D. Dietrich , M. Dolgopolov , D. Dominici , M. Dubinin , O. Eboli , J. Ellis , N. Evans , L. Fano , J. Ferland , S. Ferrag , S. P. Fitzgerald , H. Fraas , F. Franke , S. Gennai , I. F. Ginzburg , R. M. Godbole , T. Gregoire , G. Grenier , C. Grojean , S. B. Gudnason , J. F. Gunion , H. E. Haber , T. Hahn , T. Han , V. Hankele , C. Hays , S. Heinemeyer , S. Hesselbach , J. L. Hewett , K. Hidaka , M. Hirsch , W. Hollik , D. Hooper , J. Hosek , J. Hubisz , C. Hugonie , J. Kalinowski , S. Kanemura , V. Kashkan , T. Kernreiter , W. Khater , V. A. Khoze , W. Kilian , S. F. King , O. Kittel , G. Klamke , J. L. Kneur , C. Kouvaris , M. Krawczyk , P. Krstonosic , A. Kyriakis , P. Langacker , M. P. Le , H. -S. Lee , J. S. Lee , M. C. Lemaire , Y. Liao , B. Lillie , V. Litvin , H. E. Logan , B. McElrath , T. Mahmoud , E. Maina , C. Mariotti , P. Marquard , A. D. Martin , K. Mazumdar , D. J. Miller , P. Mine , K. Moenig , G. Moortgat-Pick , S. Moretti , M. M. Muhlleitner , S. Munir , R. Nevzorov , H. Newman , P. Niezurawski , A. Nikitenko , R. Noriega-Papaqui , Y. Okada , P. Osland , A. Pilaftsis , W. Porod , H. Przysiezniak , A. Pukhov , D. Rainwater , A. Raspereza , J. Reuter , S. Riemann , S. Rindani , T. G. Rizzo , E. Ros , A. Rosado , D. Rousseau , D. P. Roy , M. G. Ryskin , H. Rzehak , F. Sannino , E. Schmidt , H. Schroder , M. Schumacher , A. Semenov , E. Senaha , G. Shaughnessy , R. K. Singh , J. Terning , L. Vacavant , M. Velasco , A. Villanova del Moral , F. von der Pahlen , G. Weiglein , J. Williams , K. Williams , A. F. Zarnecki , D. Zeppenfeld , D. Zerwas , P. M. Zerwas , A. R. Zerwekh , J. Ziethe

Current data on the signal strengths and angular spectrum of the 125.5 GeV Higgs boson still allow a CP-mixed state, namely, the pseudoscalar coupling to the top quark can be as sizable as the scalar coupling: $C_u^S \approx C_u^P =1/2$. CP…

High Energy Physics - Phenomenology · Physics 2015-06-19 Kingman Cheung , Jae Sik Lee , Eibun Senaha , Po-Yan Tseng

The status of two on-going studies concerning important aspects of the phenomenology of gauge-mediated supersymmetry breaking (GMSB) models at TeV colliders is reported. The first study deals with the characteristics of the light Higgs…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Ambrosanio , S. Heinemeyer , B. Mele , S. Petrarca , G. Polesello , A. Rimoldi , G. Weiglein

The question of CP violating phases and electric dipole moments (EDMs)for the electron ($d_e$) and the neutron ($d_n$) for supergravity models with nonuniversal soft breaking is considered for models with a light ($\stackrel{<}{\sim}$1 TeV)…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Accomando , R. Arnowitt , B. Dutta

The absence of low energy supersymmetry in run I data at the LHC has pushed the nominal scale for supersymmetry beyond a TeV. While this is consistent with the discovery of the Higgs boson at \approx 125 GeV, simple models with scalar and…

High Energy Physics - Phenomenology · Physics 2015-10-23 Keith A. Olive

We investigate the supersymmetry breaking soft terms for all the viable models in the complete landscape of three-family supersymmetric Pati-Salam models arising from intersecting D6-branes on a $\mathbb{T}^6/(\mathbb{Z}_2\times…

High Energy Physics - Phenomenology · Physics 2025-02-04 Mudassar Sabir , Adeel Mansha , Tianjun Li , Zhi-Wei Wang

We discuss SUSY models in which renormalizable lepton number violating couplings hide the decay of the Higgs through h -> \chi_1^0 + \chi_1^0 followed by \chi_1^0 -> \tau + 2 jets or \chi_1^0 -> \nu_\tau + 2 jets and also explain neutrino…

High Energy Physics - Phenomenology · Physics 2009-02-09 Tom Banks , Linda M. Carpenter , Jean-François Fortin

Recently, a proposal (by R.N.M. and S.N.) was made for a new class of gauge mediated supersymmetry breaking (GMSB) models where the standard model gauge group is embedded into the gauge group $SU(2)_L\times U(1)_{I_{3R}}\times U(1)_{B-L}$…

High Energy Physics - Phenomenology · Physics 2009-10-30 Z. Chacko , B. Dutta , R. N. Mohapatra , S. Nandi

We consider gravity mediated supersymmetry (SUSY) breaking in 5D spacetime with two 4D branes B1 and B2 separated in the extra dimension. Using an off-shell 5D supergravity (SUGRA) formalism, we argue that the SUSY breaking scales could be…

High Energy Physics - Phenomenology · Physics 2011-05-12 Bumseok Kyae , Qaisar Shafi

We study in some detail the next-to-minimal supersymmetric standard model with gauge mediation of supersymmetry breaking. We find that it is feasible to spontaneously generate values of the Higgs mass parameters $\mu$ and $B_\mu$ consistent…

High Energy Physics - Phenomenology · Physics 2009-10-31 Tao Han , Danny Marfatia , Ren-Jie Zhang

We perform a multichannel analysis in context of the Large Hadron Collider (LHC) for supersymmetric (SUSY) theories with high-scale non-universal gaugino masses arising from different non-singlet representations of SU(5) and SO(10) gauge…

High Energy Physics - Phenomenology · Physics 2009-02-02 Subhaditya Bhattacharya

We investigate the limits on the higgs mass in variations of Split Supersymmetry, where the boundary value of the Higgs quartic coupling at the SUSY breaking scale ($m_s$) is allowed to deviate from its value in the minimal model of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Rakhi Mahbubani

This report summarizes the progress in SUSY studies performed during the Extended ECFA/DESY Workshop since the TESLA TDR. Based on accurate future measurements of masses of SUSY particles and the determination of the couplings and mixing…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jan Kalinowski

We investigate the Higgs boson sector of the Minimal Supersymmetric Standard Model (MSSM) in the framework of the three most prominent soft SUSY-breaking scenarios, mSUGRA, MGMSB and mAMSB. For each scenario, we determine the parameters at…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. Ambrosanio , A. Dedes , S. Heinemeyer , S. Su , G. Weiglein

Though the mass of Higgs particle is the parameter determined by the experiment in the standard model (SM), SUSY models have rather predictive power for the lightest Higgs mass, and its upper bound in some SUSY models are close to the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Naoyuki Haba

We consider supersymmetric scenarios in which the scale of SUSY breaking is low, sqrt{F}=O(TeV). Instead of studying specific models of this type, e.g. those with extra dimensions and low fundamental scale, we follow a model-independent…

High Energy Physics - Phenomenology · Physics 2010-04-05 A. Brignole , J. A. Casas , J. R. Espinosa , I. Navarro
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