Search results for " Asymmetry"

showing 10 items of 263 documents

Numerical study of leptogenesis in a 5D split fermion model with bulk neutrinos

2010

We study numerically a 5D hybrid model which incorporates a split fermion scenario and bulk neutrinos. We perform a Monte Carlo analysis of the model in order to find the regions in the parameter space allowing for realization of the leptogenesis. We find that higher order Yukawa terms must be included in order the model to produce a CP violation and net baryon number sufficient for the creation of the observed baryon asymmetry of the Universe.

PhysicsNuclear and High Energy PhysicsParticle physicsta114media_common.quotation_subjectHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesAsymmetryBaryonBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryLeptogenesisCP violationBaryon numbermedia_commonPhysical Review D
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Electroweak phase transition in left-right symmetric models

1998

We study the finite-temperature effective potential of minimal left-right symmetric models containing a bidoublet and two triplets in the scalar sector. We perform a numerical analysis of the parameter space compatible with the requirement that baryon asymmetry is not washed out by sphaleron processes after the electroweak phase transition. We find that the spectrum of scalar particles for these acceptable cases is consistent with present experimental bounds.

PhysicsNuclear and High Energy PhysicsPhase transitionParticle physicsThermal quantum field theoryCritical phenomenaHigh Energy Physics::PhenomenologyScalar (mathematics)Electroweak interactionFísicaFOS: Physical sciencesParameter spaceSphaleronHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryPhysical Review D
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Photoproduction of π 0 mesons off protons and neutrons in the second and third nucleon resonance regions

2018

Photoproduction of mesons off quasi-free nucleons bound in the deuteron allows to study the electromagnetic excitation spectrum of the neutron and the isospin structure of the excitation of nucleon resonances. The database for such reactions is much more sparse than for free proton targets. Single $\pi^0$ photoproduction off quasi-free nucleons from the deuteron was experimentally studied. Nuclear effects were investigated by a comparison of the results for free protons and quasi-free protons and used as a correction for the quasi-free neutron data. The experiment was performed at the tagged photon beam of the Mainz MAMI accelerator for photon energies between 0.45~GeV and 1.4~GeV, using an…

PhysicsNuclear reactionProtonMeson010308 nuclear & particles physicsHadronNuclear Theory7. Clean energy01 natural sciences3. Good healthNuclear physicsPionIsospin0103 physical sciencestagged photon spectrometer ; polarization observable E ; cross-sections ; pion-photoproduction ; baryon resonances ; deuteron ; MAMI ; asymmetry ; microtron ; thresholdNeutronddc:530010306 general physicsNucleonNuclear ExperimentNuclear Experiment
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Insensitivity of leptogenesis with flavour effects to low energy leptonic CP violation

2007

If the baryon asymmetry of the Universe is produced by leptogenesis, CP violation is required in the lepton sector. In the seesaw extension of the standard model with three hierarchical right-handed neutrinos, we show that the baryon asymmetry is insensitive to the Pontecorvo-Maki-Nagakawa-Sakata phases: thermal leptogenesis can work for any value of the observable phases. This result was well known when there were no flavor effects in leptogenesis; we show that it remains true when flavor effects are included.

PhysicsParticle physics010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFísica01 natural sciencesAsymmetryBaryonBaryogenesisBaryon asymmetrySeesaw molecular geometryLeptogenesis0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsmedia_common
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Direct limits on the interaction of antiprotons with axion-like dark matter

2019

Astrophysical observations indicate that there is roughly five times more dark matter in the Universe than ordinary baryonic matter, with an even larger amount of the Universe's energy content due to dark energy. So far, the microscopic properties of these dark components have remained shrouded in mystery. In addition, even the five percent of ordinary matter in our Universe has yet to be understood, since the Standard Model of particle physics lacks any consistent explanation for the predominance of matter over antimatter. Inspired by these central problems of modern physics, we present here a direct search for interactions of antimatter with dark matter, and place direct constraints on th…

PhysicsParticle physicsAstrophysics and AstronomyCosmology and Nongalactic Astrophysics (astro-ph.CO)MultidisciplinaryAtomic Physics (physics.atom-ph)010308 nuclear & particles physicsDark matterFOS: Physical sciences01 natural sciencesPhysics - Atomic PhysicsStandard ModelBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryOrders of magnitude (time)AntiprotonAntimatter0103 physical sciencesPräzisionsexperimente - Abteilung Blaum010306 general physicsAxionParticle Physics - ExperimentAstrophysics - Cosmology and Nongalactic Astrophysics
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R parity violation assisted thermal leptogenesis in the seesaw mechanism.

2005

Successful leptogenesis within the simplest type I supersymmetric seesaw mechanism requires the lightest of the three right-handed neutrino supermultiplets to be heavier than $\sim10^9$ GeV. Thermal production of such (s)neutrinos requires very high reheating temperatures which result in an overproduction of gravitinos with catastrophic consequences for the evolution of the universe. In this letter, we let R-parity be violated through a $\lambda_i \hat{N}_i \hat{H}_u \hat{H}_d$ term in the superpotential, where $\hat{N}_i$ are right-handed neutrino supermultiplets. We show that in the presence of this term, the produced lepton-antilepton asymmetry can be enhanced. As a result, even for $\ha…

PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologySuperpotentialFísicaFOS: Physical sciencesGeneral Physics and AstronomyBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetrySeesaw mechanismR-parityLeptogenesisHigh Energy Physics::ExperimentGravitinoNeutrinoPhysical review letters
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Electroweak baryogenesis and dark matter from a singlet Higgs

2012

If the Higgs boson H couples to a singlet scalar S via lambda_m |H|^2 S^2, a strong electroweak phase transition can be induced through a large potential barrier that exists already at zero temperature. In this case properties of the phase transition can be computed analytically. We show that electroweak baryogenesis can be achieved using CP violation from a dimension-6 operator that couples S to the top-quark mass, suppressed by a new physics scale that can be well above 1 TeV. Moreover the singlet is a dark matter candidate whose relic density is < 3% of the total dark matter density, but which nevertheless interacts strongly enough with nuclei (through Higgs exchange) to be just below…

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsPhysics beyond the Standard ModelDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstronomy and Astrophysics01 natural sciencesBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetry0103 physical sciencesHiggs bosonCP violationInvariant massHigh Energy Physics::Experiment010306 general physicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Mass bounds for baryogenesis from particle decays and the inert doublet model

2014

In models for thermal baryogenesis from particle decays, the mass of the decaying particle is typically many orders of magnitude above the TeV scale. We will discuss different ways to lower the energy scale of baryogenesis and present the corresponding lower bounds on the particle's mass. This is done specifically for the inert doublet model with heavy Majorana neutrinos and then we indicate how to extrapolate the results to other scenarios. We also revisit the question of whether or not dark matter, neutrino masses, and the cosmic baryon asymmetry can be explained simultaneously at low energies in the inert doublet model.

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstronomy and AstrophysicsBaryogenesisMAJORANAHigh Energy Physics - PhenomenologyBaryon asymmetryHigh Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)ThermalLeptogenesisParticleHigh Energy Physics::ExperimentNeutrinoBaryon asymmetryAstrophysics - Cosmology and Nongalactic Astrophysics
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Neutrino masses and GUT baryogenesis

2004

We reconsider the GUT-baryogenesis mechanism for generating the baryon asymmetry of the Universe. The baryon asymmetry is produced by the out of equilibrium decay of coloured Higgs bosons at the GUT scale, conserving B-L. If neutrinos are Majorana particles, lepton number violating interactions erase the lepton number excess, but part of the baryon asymmetry may be preserved, provided those interactions are not in thermal equilibrium when the sphaleron processes become effective, at $T \sim 10^{12}~ GeV$. We analyse whether this mechanism for baryogenesis is feasible in a variety of GUT models of fermion masses proposed in the literature, based on horizontal symmetries.

PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFermionLepton numberSphaleronBaryogenesisNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryHiggs bosonHigh Energy Physics::ExperimentNeutrinoParticle Physics - PhenomenologyBosonProceedings of International Workshop on Astroparticle and High Energy Physics — PoS(AHEP2003)
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Measurement of the transverse target and beam-target asymmetries in η meson photoproduction at MAMI

2014

We present new data for the transverse target asymmetry T and the very first data for the beam-target asymmetry F in the $\vec \gamma \vec p\to\eta p$ reaction up to a center-of-mass energy of W=1.9 GeV. The data were obtained with the Crystal-Ball/TAPS detector setup at the Glasgow tagged photon facility of the Mainz Microtron MAMI. All existing model predictions fail to reproduce the new data indicating a significant impact on our understanding of the underlying dynamics of $\eta$ meson photoproduction. The peculiar nodal structure observed in existing T data close to threshold is not confirmed.

PhysicsParticle physicsPhotonProtonMesonNuclear Theorymedia_common.quotation_subjectPartial wave analysisNuclear TheoryGeneral Physics and AstronomyAsymmetryHigh Energy Physics - ExperimentNuclear physicsbeam-target asymmetry F; γ⃗ p⃗ →ηp reaction; Mainz Microtron MAMIHigh Energy Physics::ExperimentNucleonNuclear ExperimentMicrotronNuclear ExperimentCrystal Ballmedia_common
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