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Related papers: Gravitino thermal production

200 papers

Considering gravitino dark matter scenarios, we study constraints on the reheating temperature of inflation. We present the gauge-invariant result for the thermally produced gravitino yield to leading order in the Standard Model gauge…

High Energy Physics - Phenomenology · Physics 2008-11-26 Josef Pradler , Frank Daniel Steffen

We consider the direct $s$-channel gravitational production of dark matter during the reheating process. Independent of the identity of the dark matter candidate or its non-gravitational interactions, the gravitational process is always…

High Energy Physics - Phenomenology · Physics 2021-06-16 Yann Mambrini , Keith A. Olive

Worldline approaches, when available, often simplify and make more efficient the calculation of various observables in quantum field theories. In this contribution we first review the calculation of the graviton self-energy due to a loop of…

High Energy Physics - Theory · Physics 2015-04-10 Fiorenzo Bastianelli , Roberto Bonezzi

The impact of a kination-dominated phase generated by a quintessential exponential model on the thermal abundance of gravitinos and axinos is investigated. We find that their abundances become proportional to the transition temperature from…

High Energy Physics - Phenomenology · Physics 2009-07-20 M. E. Gomez , S. Lola , C. Pallis , J. Rodriguez-Quintero

We present for smooth non-oscillating backgrounds an analytic formula which calculates the energy density of massive and massless particles created via gravitational particle production, thus giving the corresponding reheating temperature.…

General Relativity and Quantum Cosmology · Physics 2023-03-09 Jaume de Haro , Llibert Aresté Saló

We calculate in a general background gauge, to one-loop order, the leading logarithmic contribution from the graviton self-energy at finite temperature $T$, extending a previous analysis done at $T=0$. The result, which has a transverse…

High Energy Physics - Theory · Physics 2023-05-02 F. T. Brandt , J. Frenkel , D. G. C. McKeon , G. S. S. Sakoda

At the end of inflation, the inflaton field decays into an initially nonthermal population of relativistic particles which eventually thermalize. We consider the production of dark matter from this relativistic plasma, focusing on the…

High Energy Physics - Phenomenology · Physics 2018-12-18 Marcos A. G. Garcia , Mustafa A. Amin

We compute the gravitational production of conformally coupled superheavy particles during the phase transition from the end of inflation to the beginning of kination for $\alpha$-attractors potentials in the context of Quintessential…

General Relativity and Quantum Cosmology · Physics 2021-12-28 Llibert Aresté Saló , Jaume de Haro

The production rate of heavy Majorana neutrinos is relevant for models of thermal leptogenesis in the early Universe. In the high temperature limit the production can proceed via the 1 <-> 2 (inverse) decays which are allowed by the thermal…

High Energy Physics - Phenomenology · Physics 2011-04-04 Alexey Anisimov , Denis Besak , Dietrich Bodeker

We consider gravitational particle production (GPP) of dark matter (DM) under a supergravity framework, where the $\alpha$-attractor inflation model is used. The particle spectrum is computed numerically and the DM number density is…

High Energy Physics - Phenomenology · Physics 2024-12-10 Chenhuan Wang , Wenbin Zhao

We study the high-energy equivalence between helicity 1/2 gravitinos and goldstinos in order to calculate the production of gravitinos in time-dependent scalar and gravitational backgrounds. We derive this equivalence for equations of…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. L. Maroto , J. R. Pelaez

Gravitinos with a mass in the keV range are an interesting candidate for warm dark matter. Recent measurements of the matter density of the universe and of cosmic structures at the dwarf galaxy scale rule out the simplest gravitino models…

Astrophysics · Physics 2009-11-07 Edward A. Baltz , Hitoshi Murayama

Thermal leptogenesis requires the reheating temperature $T_R \gsim 3\times 10^{9}$ GeV, which contradicts a recently obtained constraint on the reheating temperature, $T_R \lsim 10^6$ GeV, for the gravitino mass of 100 GeV-10 TeV. This…

High Energy Physics - Phenomenology · Physics 2015-06-25 M. Fujii , M. Ibe , T. Yanagida

In the framework of the Hard Thermal Loop effective theory, we calculate the two-loop contributions to hard lepton pair production in a quark-gluon plasma. We show that the result is free of any infrared and collinear singularity. We also…

High Energy Physics - Phenomenology · Physics 2009-11-07 P. Aurenche , F. Gelis , H. Zaraket

After a period of inflationary expansion, the Universe reheated and reached full thermal equilibrium at the reheating temperature. In this talk, based on the paper, arXiv:0710.3349, we point out that, in the context of effective low-energy…

High Energy Physics - Phenomenology · Physics 2009-05-01 Ki-Young Choi , Leszek Roszkowski , Roberto Ruiz de Austri

We obtain new stronger bounds by orders of magnitude, on the ultimate temperature of the universe by exploiting the copious production of gravitinos at finite temperature.

High Energy Physics - Theory · Physics 2009-10-28 Willy Fischler

We explore an alternative mechanism for the production of gravitino dark matter whereby relic gravitinos originate from the decays of superpartners which are still in thermal equilibrium, i.e. via freeze-in. Contributions to the gravitino…

High Energy Physics - Phenomenology · Physics 2015-05-27 Clifford Cheung , Gilly Elor , Lawrence Hall

Studies are cited indicating that gravitino production acts as a natural upper bound to Li6 and Li7 levels, based on what happens after hadronic decay of relic 1 TeV into 100 GeV gravitinos at 1000 s. after the Big Bang. The produced…

General Physics · Physics 2014-11-18 A. W. Beckwith

We perform a numerical study of the preheating mechanism of particle production in models of quintessential inflation and compare it with the usual gravitational production mechanism. We find that even for a very small coupling between the…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. H. Campos , H. C. Reis , R. Rosenfeld

Under general circumstances full thermal equilibrium may not be established for a long period after perturbative or non-perturbative decay of the inflaton has completed. One can instead have a distribution of particles which is in kinetic…

High Energy Physics - Phenomenology · Physics 2007-05-23 Rouzbeh Allahverdi , Anupam Mazumdar