English
Related papers

Related papers: Dark matter in gravity-mediated supersymmetry brea…

200 papers

Searches for supersymmetry (SUSY) often rely on a combination of hard physics objects (jets, leptons) along with large missing transverse energy to separate New Physics from Standard Model hard processes. We consider a class of…

High Energy Physics - Phenomenology · Physics 2015-05-28 Daniele S. M. Alves , Jia Liu , Neal Weiner

The lack of evidence for low energy supersymmetry at the LHC implies a supersymmetry scale in excess a TeV. While this is consistent (and even helpful) with a Higgs boson mass at $\approx$ 125 GeV, simple supersymmetric models with scalar…

High Energy Physics - Phenomenology · Physics 2016-04-26 Keith A. Olive

In the event that R-Parity conserving supersymmetry (SUSY) is discovered at the LHC, a key issue which will need to be addressed will be the consistency of that signal with astrophysical and non-accelerator constraints on SUSY Dark Matter.…

High Energy Physics - Phenomenology · Physics 2010-02-03 G. Polesello , D. R. Tovey

Supersymmetric scenarios with a very weakly interacting lightest superparticle (LSP) - like the gravitino or axino - naturally give rise to a long-lived next-to-LSP (NLSP). In the case of a stau NLSP, the scenario shows up in a very…

High Energy Physics - Phenomenology · Physics 2012-07-13 Jan Heisig

We study models in which supersymmetry breaking appears at an intermediate scale, M_in, below the GUT scale. That is, that the soft supersymmetry-breaking parameters of the MSSM are universal at M_in. We demand that the lightest neutralino…

High Energy Physics - Phenomenology · Physics 2007-10-10 Pearl Sandick

We study dark matter for gaugino-mediated supersymmetry breaking and compact dimensions of order the grand unification scale. Higgs fields are bulk fields, and in general their masses differ from those of squarks and sleptons at the…

High Energy Physics - Phenomenology · Physics 2009-11-11 Wilfried Buchmuller , Laura Covi , Joern Kersten , Kai Schmidt-Hoberg

We point out that, if R-parity is broken spontaneously, the neutralino can decay to the final state majoron plus neutrino, which from the experimental point of view is indistinguishable from the standard missing momentum signal of…

High Energy Physics - Phenomenology · Physics 2009-11-11 M. Hirsch , W. Porod

We show some consequences of the nonlinear supersymmetric general relativity (NLSUSYGR) theory on particle physics, cosmology and their relations. They may give new insights into the SUSY breaking mechanism, dark energy, dark matter and the…

High Energy Physics - Theory · Physics 2015-06-03 Kazunari Shima , Motomu Tsuda

If the axino is the lightest superpartner and satisfies cosmological bounds, including a preferred range of the relic abundance of cold dark matter, then the usual stringent constraints on the parameter space of the CMSSM become greatly…

High Energy Physics - Phenomenology · Physics 2009-11-10 Laura Covi , Leszek Roszkowski , Roberto Ruiz de Austri , Michael Small

Axino and gravitino are promising candidates to solve the dark matter (DM) problem in the framework of supersymmetry. In this work, we assume that the axino is the lightest supersymmetric particle (LSP), and therefore contributes to DM. In…

High Energy Physics - Phenomenology · Physics 2020-02-05 German A. Gomez-Vargas , Daniel E. Lopez-Fogliani , Carlos Munoz , Andres D. Perez

The present matter content of our universe may be governed by a $U(1)_{B-L}$ symmetry -- the simplest gauge completion of the seesaw mechanism which produces small neutrino masses. The matter parity results as a residual gauge symmetry,…

High Energy Physics - Phenomenology · Physics 2020-12-15 Phung Van Dong , Duong Van Loi

A small breaking of R-parity reconciles thermal leptogenesis, gravitino dark matter and primordial nucleosynthesis. We find that the same breaking relaxes cosmological bounds on the axion multiplet. Naturally expected spectra become allowed…

High Energy Physics - Phenomenology · Physics 2015-05-27 Jasper Hasenkamp , Jörn Kersten

There is almost universal agreement among astronomers that most of the mass in the Universe and most of the mass in the Galactic halo is dark. Many lines of reasoning suggest that the dark matter consists of some new, as yet undiscovered,…

High Energy Physics - Phenomenology · Physics 2009-10-28 G. Jungman , M. Kamionkowski , K. Griest

We consider theories with spontaneously broken global or local supersymmetry where the pseudo-goldstino or the gravitino is the lightest superparticle (LSP). Assuming that the long-lived next-to-lightest superparticle (NSP) is a charged…

High Energy Physics - Phenomenology · Physics 2007-05-23 Wilfried Buchmuller , Koichi Hamaguchi , Michael Ratz , Tsutomu Yanagida

The ability of the LHC to make statements about the dark matter problem is considered, with a specific focus on supersymmetry. After reviewing the current strategies for supersymmetry searches at the LHC (in both CMS and ATLAS), some key…

High Energy Physics - Phenomenology · Physics 2010-11-03 Martin J. White

The WIMP dark matter (DM) hypothesis now is in an awkward position, owing to the stronger and stronger exclusion from DM direct detection. In this article we design a mechanism to evade this constraint.The idea is simple. DM has a…

High Energy Physics - Phenomenology · Physics 2022-01-12 Jun Guo , Zhaofeng Kang , Peng Zhang

In many models, stability of dark matter particles is protected by a conserved Z_2 quantum number. However dark matter can be stabilized by other discrete symmetry groups, and examples of such models with custom-tailored field content have…

High Energy Physics - Phenomenology · Physics 2013-05-30 I. P. Ivanov , V. Keus

The possible phenomenological consequences of R-parity violating interactions in the framework of low energy supersymmetry breaking are studied. It is pointed out that even very weak R-parity violation would completely overshadow one of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Carena , S. Pokorski , C. E. M. Wagner

We present an explicit model where the decay of an R-parity even scalar $S$ with ${\cal O}({\rm TeV})$ mass is the origin of non-thermal dark matter. The correct relic abundance can be produced for both large and small annihilation rates in…

High Energy Physics - Phenomenology · Physics 2013-05-01 Rouzbeh Allahverdi , Bhaskar Dutta , Kuver Sinha

We consider a broad class of supersymmetric theories in which dark matter (DM) is the lightest superpartner (LSP) of a hidden sector that couples very weakly to visible sector fields. Portal interactions connecting visible and hidden…

High Energy Physics - Phenomenology · Physics 2011-04-11 Clifford Cheung , Gilly Elor , Lawrence J. Hall , Piyush Kumar