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We explore a scenario of high scale supersymmetry where all supersymmetric particles except gauginos stay at a high energy scale $M_{\rm SUSY}$ which is much larger than the reheating temperature $T_\text{RH}$. The dark matter is dominated…

High Energy Physics - Phenomenology · Physics 2023-12-11 Chengcheng Han , Peiwen Wu , Jin Min Yang , Mengchao Zhang

We study a supergravity model of inflation with R-symmetry and a single scalar field, the inflaton, slowly rolling away from the origin. The scales of inflation can be as low as the supersymmetry breaking scale of 10^10 GeV or even the…

High Energy Physics - Theory · Physics 2009-10-31 G. German , A. de la Macorra , M. Mondragon

If a bosonic partner of a right-handed neutrino dominates the early universe sufficiently before its decay, important ingredients in the present universe are related to physics of the right-handed neutrino sector. In particular, we find…

High Energy Physics - Phenomenology · Physics 2009-11-10 M. Ibe , T. Yanagida

Inflation, as currently understood, requires the presence of fields with very flat potentials. Supersymmetric models in which supersymmetry breaking is communicated by supergravity naturally yield such fields, but the scales are typically…

High Energy Physics - Phenomenology · Physics 2009-10-30 Michael Dine , Antonio Riotto

Neutralino dark matter is well motivated, but also suffers from two shortcomings: it requires gravity-mediated supersymmetry breaking, which generically violates flavor constraints, and its thermal relic density \Omega is typically too…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jonathan L. Feng , Bryan T. Smith , Fumihiro Takayama

We show that the isocurvature perturbations imply that the gravitationally produced superheavy dark matter must have masses larger than few times the Hubble expansion rate at the end of inflation. This together with the bound on tensor to…

Astrophysics · Physics 2008-11-26 Daniel J. H. Chung , Edward W. Kolb , Antonio Riotto , Leonardo Senatore

We study the possibility of an intermediate scale existing in supersymmetric SO(10) grand unified theories: The intermediate scale is demanded to be around 10^{12} GeV so that neutrinos can obtain masses suitable for explaining the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Masako Bando , Joe Sato , Tomohiko Takahashi

In higher-dimensional supersymmetric theories gauge couplings of the effective four-dimensional theory are determined by expectation values of scalar fields. We find that at temperatures above a critical temperature $T_*$, which depends on…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Buchmüller , K. Hamaguchi , M. Ratz

In models with gauge mediated supersymmetry breaking the gravitino is the lightest supersymmetric particle. If R-parity is violated the gravitino decays, but with a half-live far exceeding the age of the universe and thus is, in principle,…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Hirsch , W. Porod , D. Restrepo

Extremely weakly interacting particles like the gravitino may be stable enough on cosmological time scales to constitute a good dark matter candidate even in the presence of R-parity violation. We consider the possibility that the recently…

High Energy Physics - Phenomenology · Physics 2014-07-23 N. -E. Bomark , L. Roszkowski

In this paper, we explore the parameter space of hilltop supernatural inflation model and show the regime within which there is no gravitino problem even if we consider both thermal and nonthermal production mechanisms. We make plots for…

High Energy Physics - Phenomenology · Physics 2011-03-14 Kazunori Kohri , Chia-Min Lin

We study resonant gravitino production in the early Universe in the presence of SUSY flat directions whose large VEVs break some but not all gauge symmetries. We find that for a large region of parameter space the gravitino abundance is…

Cosmology and Nongalactic Astrophysics · Physics 2014-08-06 Namit Mahajan , Raghavan Rangarajan , Anjishnu Sarkar

A class of supersymmetric grand unified theories is introduced that has a single scale below the cutoff, that of the supersymmetry breaking masses $\tilde{m}$. For a wide range of the dimensionless parameters, agreement with the observed…

High Energy Physics - Phenomenology · Physics 2015-06-19 Lawrence J. Hall , Yasunori Nomura , Satoshi Shirai

Bilinear R-parity violation provides an attractive origin for neutrino masses and mixings. In such schemes the gravitino is a viable decaying dark matter particle whose R-parity violating decays lead to monochromatic photons with rates…

High Energy Physics - Phenomenology · Physics 2013-05-30 Diego Restrepo , Marco Taoso , J. W. F. Valle , Oscar Zapata

We analyze the curvaton scenario in the context of supersymmety. Supersymmetric theories contain many scalars, and therefore many curvaton candidates. To obtain a scale invariant perturbation spectrum, the curvaton mass should be small…

High Energy Physics - Phenomenology · Physics 2014-11-17 Marieke Postma

Supersymmetric theories with gravitino dark matter generally do not allow the high reheating temperature required by thermal leptogenesis without running afoul of relic abundance or big bang nucleosynthesis constraints. We report on a…

High Energy Physics - Phenomenology · Physics 2011-01-17 Laura Covi , Marek Olechowski , Stefan Pokorski , Krzysztof Turzynski , James D. Wells

Most of the inflation models end up with non-vanishing vacuum expectation values of the inflaton fields \phi in the true vacuum, which induce, in general, nonvanishing auxiliary field G_\phi for the inflaton potential in supergravity. We…

High Energy Physics - Phenomenology · Physics 2010-11-05 Masahiro Kawasaki , Fuminobu Takahashi , T. T. Yanagida

Since the thermal history of the Universe is unknown before the epoch of primordial nucleosynthesis, the largest temperature of the radiation dominated phase (the reheating temperature) might have been as low as 1 MeV. We perform a…

High Energy Physics - Phenomenology · Physics 2009-11-07 N. Fornengo , A. Riotto , S. Scopel

We study the consequences of the gravitino decay into dark matter. We suppose that the lightest neutralino is the main component of dark matter. In our framework gravitino is heavy enough to decay before Big Bang Nucleosynthesis starts. We…

High Energy Physics - Phenomenology · Physics 2007-06-29 David Gherson

The recently observed mass ~ 125 GeV for the Higgs boson suggests a high-energy scale SUSY breaking, above O(10) TeV. It is, however, very puzzling why nature chooses such a high energy scale for the SUSY breaking, if the SUSY is a solution…

High Energy Physics - Phenomenology · Physics 2015-06-12 Keisuke Harigaya , Masahiro Kawasaki , Tsutomu T. Yanagida