Search results for "inflaton"

showing 10 items of 35 documents

Reheating the Standard Model from a hidden sector

2016

We consider a scenario where the inflaton decays to a hidden sector thermally decoupled from the visible Standard Model sector. A tiny portal coupling between the hidden and the visible sectors later heats the visible sector so that the Standard Model degrees of freedom come to dominate the energy density of the Universe before Big Bang Nucleosynthesis. We find that this scenario is viable, although obtaining the correct dark matter abundance and retaining successful Big Bang Nucleosynthesis is not obvious. We also show that the isocurvature perturbations constituted by a primordial Higgs condensate are not problematic for the viability of the scenario.

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Ultimate fate of the universereheatingmedia_common.quotation_subjectDark matterUNIVERSEFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics114 Physical sciences01 natural sciencesdark matterdecouplingpimeä aineHigh Energy Physics - Phenomenology (hep-ph)INFLATIONBig Bang nucleosynthesis0103 physical sciencesDARK-MATTERELECTROWEAK VACUUM010306 general physicsmedia_commonPhysicsQuintom scenariota114STABILITY010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDecoupling (cosmology)InflatonHIGGSUniverseHidden sectorextensions of the Standard ModelHigh Energy Physics - Phenomenologyhidden sectorsSCALARAstrophysics - Cosmology and Nongalactic Astrophysics
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Spontaneous baryogenesis in spiral inflation

2019

We examined the possibility of spontaneous baryogenesis driven by the inflaton in the scenario of spiral inflation, and found the parametric dependence of the late-time baryon number asymmetry. As a result, it is shown that, depending on the effective coupling of baryon/lepton number violating operators, it is possible to obtain the right amount of asymmetry even in the presence of a matter-domination era as long as such era is relatively short. In a part of the parameter space, the required expansion rate during inflation is close to the current upper-bound, and hence can be probed in the near future experiments.

Particle physicsPhysics and Astronomy (miscellaneous)media_common.quotation_subjectFOS: Physical scienceslcsh:AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsParameter space01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)media_commonInflation (cosmology)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInflatonLepton numberBaryonBaryogenesisHigh Energy Physics - Phenomenologylcsh:QC770-798Baryon numberEuropean Physical Journal C: Particles and Fields
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Quantum corrections to inflation: the importance of RG-running and choosing the optimal RG-scale

2017

We demonstrate the importance of correctly implementing RG running and choosing the RG scale when calculating quantum corrections to inflaton dynamics. We show that such corrections are negligible for single-field inflation, in the sense of not altering the viable region in the ${n}_{s}\ensuremath{-}r$ plane, when imposing Planck constraints on ${A}_{s}$. Surprisingly, this also applies, in a nontrivial way, for an inflaton coupled to additional spectator degrees of freedom. The result relies on choosing the renormalization scale (pseudo-)optimally, thereby avoiding unphysical large logarithmic corrections to the Friedmann equations and large running of the couplings. We find that the viabl…

Physics beyond the Standard ModelScalar (mathematics)FOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesClassical limitRenormalizationsymbols.namesakeGeneral Relativity and Quantum Cosmologyquantum correctionsHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciences010306 general physicsQuantumMathematical physicsPhysicsta114010308 nuclear & particles physicsFriedmann equationsInflatonRenormalization groupinflatonHigh Energy Physics - Phenomenologysymbols
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Inflation with mixed helicities and its observational imprint on CMB

2018

In the framework of effective field theories with prominent helicity-0 and helicity-1 fields coupled to each other via a dimension-3 operator, we study the dynamics of inflation driven by the helicity-0 mode, with a given potential energy, as well as the evolution of cosmological perturbations, influenced by the presence of a mixing term between both helicities. In this scenario, the temporal component of the helicity-1 mode is an auxiliary field and can be integrated out in terms of the time derivative of the helicity-0 mode, so that the background dynamics effectively reduces to that in single-field inflation modulated by a parameter $\beta$ associated to the coupling between helicity-0 a…

PhysicsHigh Energy Physics - TheoryCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsCosmic microwave backgroundCosmic background radiationFOS: Physical sciencesObservableGeneral Relativity and Quantum Cosmology (gr-qc)Astrophysics::Cosmology and Extragalactic AstrophysicsInflaton01 natural sciencesGeneral Relativity and Quantum CosmologyTheoretical physicsAuxiliary fieldsymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)0103 physical sciencesTime derivativeEffective field theorysymbolsPlanck010306 general physicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Primordial Black Holes and Slow-Roll Violation

2017

For primordial black holes (PBH) to be the dark matter in single-field inflation, the slow-roll approximation must be violated by at least ${\cal O}(1)$ in order to enhance the curvature power spectrum within the required number of efolds between CMB scales and PBH mass scales. Power spectrum predictions which rely on the inflaton remaining on the slow-roll attractor can fail dramatically leading to qualitatively incorrect conclusions in models like an inflection potential and misestimate the mass scale in a running mass model. We show that an optimized temporal evaluation of the Hubble slow-roll parameters to second order remains a good description for a wide range of PBH formation models …

PhysicsInflation (cosmology)Cosmology and Nongalactic Astrophysics (astro-ph.CO)Slow roll010308 nuclear & particles physicsDark matterCosmic microwave backgroundSpectral densityFOS: Physical sciencesPrimordial black holeAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsGeneral Relativity and Quantum Cosmology (gr-qc)Inflaton01 natural sciencesGeneral Relativity and Quantum Cosmology0103 physical sciencesAttractor010306 general physicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Spiral Inflation

2015

We propose a novel scenario of primordial inflation in which the inflaton goes through a spiral motion starting from around the top of a symmetry breaking potential. We show that, even though inflation takes place for a field value much smaller than Planck scale, it is possible to obtain relatively large tensor to scalar ratio ($r \sim 0.1$) without fine tuning. The inflationary observables perfectly match Planck data.

PhysicsInflation (cosmology)Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Field (physics)Scalar (mathematics)FOS: Physical sciencesFísicaObservableAstrophysics::Cosmology and Extragalactic AstrophysicsInflatonlcsh:QC1-999High Energy Physics - PhenomenologyTheoretical physicssymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)symbolsTensorSymmetry breakingPlancklcsh:PhysicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Peccei–Quinn field for inflation, baryogenesis, dark matter, and much more

2016

We propose a scenario of brane cosmology in which the Peccei-Quinn field plays the role of the inflaton and solves simultaneously many cosmological and phenomenological issues such as the generation of a heavy Majorana mass for the right-handed neutrinos needed for seesaw mechanism, MSSM $\mu$-parameter, the right amount of baryon number asymmetry and dark matter relic density at the present universe, together with an axion solution to the strong CP problem without the domain wall obstacle. Interestingly, the scales of the soft SUSY-breaking mass parameter and that of the breaking of $U(1)_{\rm PQ}$ symmetry are lower bounded at $\mathcal{O}(10) {\mathrm TeV}$ and $\mathcal{O}(10^{11}) {\ma…

PhysicsInflation (cosmology)Particle physicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsPhysics beyond the Standard ModelDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsInflaton01 natural scienceslcsh:QC1-999BaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBrane cosmologyStrong CP problemHigh Energy Physics::Experiment010306 general physicsAxionlcsh:PhysicsAstrophysics - Cosmology and Nongalactic AstrophysicsPhysics Letters B
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Transplanckian masses in inflation

2016

AbstractWe explore the possibility that the transplanckian field values needed to accommodate the experimental results in minimally coupled single-field inflation models are only due to our insistence of imposing a minimal coupling of the inflaton field to gravity. A simple conformal transformation can bring the field values below the Planck mass without changing the physics at the expense of having a richer gravitational sector. Transplanckian field values may be the signal that we are (miss)interpreting phenomena due to gravity as being originated exclusively in the scalar sector.

PhysicsMinimal couplingInflation (cosmology)Nuclear and High Energy PhysicsGravity (chemistry)Field (physics)010308 nuclear & particles physicsScalar (mathematics)Planck massInflaton01 natural sciencesGravitationTheoretical physicsGeneral Relativity and Quantum CosmologyClassical mechanics0103 physical sciences010306 general physicsNuclear and Particle Physics Proceedings
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Phenomenological approaches of inflation and their equivalence

2014

In this work, we analyze two possible alternative and model-independent approaches to describe the inflationary period. The first one assumes a general equation of state during inflation due to Mukhanov, while the second one is based on the slow-roll hierarchy suggested by Hoffman and Turner. We find that, remarkably, the two approaches are equivalent from the observational viewpoint, as they single out the same areas in the parameter space, and agree with the inflationary attractors where successful inflation occurs. Rephrased in terms of the familiar picture of a slowly rolling, canonically normalized scalar field, the resulting inflaton excursions in these two approaches are almost ident…

PhysicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsFísicaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsInflatonParameter space01 natural sciencessymbols.namesakeTheoretical physicsGeneral Relativity and Quantum Cosmology0103 physical sciencesAttractorsymbolsInflationary epochPlanck010306 general physicsScalar fieldEquivalence (measure theory)Eternal inflationAstrophysics - Cosmology and Nongalactic Astrophysics
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Do current data prefer a nonminimally coupled inflaton?

2015

We examine the impact of a non-minimal coupling of the inflaton to the Ricci scalar, $\frac12 \xi R\phi^2$, on the inflationary predictions. Such a non-minimal coupling is expected to be present in the inflaton Lagrangian on fairly general grounds. As a case study, we focus on the simplest inflationary model governed by the potential $V\propto \phi^2$, using the latest combined 2015 analysis of Planck and BICEP2/Keck Array. We find that the presence of a coupling $\xi$ is favoured at a significance of $99\%$ CL, assuming that nature has chosen the potential $V\propto \phi^2$ to generate the primordial perturbations and a number of e-foldings $N=60$. Within the context of the same scenario, …

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsFOS: Physical sciencesFísicaSigmaAstrophysics::Cosmology and Extragalactic AstrophysicsInflaton01 natural sciencesSpectral lineGeneral Relativity and Quantum Cosmologysymbols.namesake13. Climate action0103 physical sciencessymbolsPlanck010306 general physicsLagrangianAstrophysics - Cosmology and Nongalactic AstrophysicsScalar curvaturePhysical Review D
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