Search results for "Particle physics"

showing 10 items of 6826 documents

New cosmological bounds on hot relics: Axions $\&$ Neutrinos

2020

Axions, if realized in nature, can be copiously produced in the early universe via thermal processes, contributing to the mass-energy density of thermal hot relics. In light of the most recent cosmological observations, we analyze two different thermal processes within a realistic mixed hot-dark-matter scenario which includes also massive neutrinos. Considering the axion-gluon thermalization channel we derive our most constraining bounds on the hot relic masses $m_a < 7.46$ eV and $\sum m_��< 0.114$ eV both at 95 per cent CL; while studying the axion-pion scattering, without assuming any specific model for the axion-pion interactions and remaining in the range of validity of the chira…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics::Instrumentation and Detectorsmedia_common.quotation_subjectDark matterCosmic background radiationFOS: Physical sciencescosmic background radiation; cosmological parameters; dark matter; early Universe; cosmology: observations;7. Clean energy01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciences010306 general physicsAxionmedia_commonPhysics010308 nuclear & particles physicsHot dark matterHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsUniverseHigh Energy Physics - Phenomenology13. Climate actionSpace and Planetary ScienceStrong CP problemNeutrinoAstrophysics - Cosmology and Nongalactic Astrophysics
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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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How to relax the cosmological neutrino mass bound

2019

We study the impact of non-standard momentum distributions of cosmic neutrinos on the anisotropy spectrum of the cosmic microwave background and the matter power spectrum of the large scale structure. We show that the neutrino distribution has almost no unique observable imprint, as it is almost entirely degenerate with the effective number of neutrino flavours, $N_{\mathrm{eff}}$, and the neutrino mass, $m_{\nu}$. Performing a Markov chain Monte Carlo analysis with current cosmological data, we demonstrate that the neutrino mass bound heavily depends on the assumed momentum distribution of relic neutrinos. The message of this work is simple and has to our knowledge not been pointed out cle…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)cosmological neutrinosPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaCosmic microwave backgroundFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysicscosmological parameters from LSS01 natural sciencesCosmologyMomentumsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)cosmological0103 physical sciencesPhysicsCOSMIC cancer database010308 nuclear & particles physicsMatter power spectrumHigh Energy Physics::Phenomenologycosmological parameters from CMBRAstronomy and AstrophysicsObservableMarkov chain Monte Carloneutrino masses from cosmologyHigh Energy Physics - Phenomenologyparameters from CMBRsymbolsHigh Energy Physics::ExperimentNeutrinoAstrophysics - Cosmology and Nongalactic Astrophysics
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Chern-Simons anomaly as polarization effect

2011

The parity violating Chern-Simons term in the epoch before the electroweak phase transition can be interpreted as a polarization effect associated to massless right-handed electrons (positrons) in the presence of a large-scale seed hypermagnetic field. We reconfirm the viability of a unified seed field scenario relating the cosmological baryon asymmetry and the origin of the protogalactic large-scale magnetic fields observed in astronomy.

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)media_common.quotation_subjectChern–Simons theoryFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesAsymmetryBaryon asymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsmedia_commonPhysics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyFísicaAstronomy and AstrophysicsParity (physics)Massless particleBaryonHigh Energy Physics - PhenomenologyLeptogenesisHigh Energy Physics::ExperimentAstrophysics - Cosmology and Nongalactic Astrophysics
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Asymmetric Dark Matter and Dark Radiation

2012

Asymmetric Dark Matter (ADM) models invoke a particle-antiparticle asymmetry, similar to the one observed in the Baryon sector, to account for the Dark Matter (DM) abundance. Both asymmetries are usually generated by the same mechanism and generally related, thus predicting DM masses around 5 GeV in order to obtain the correct density. The main challenge for successful models is to ensure efficient annihilation of the thermally produced symmetric component of such a light DM candidate without violating constraints from collider or direct searches. A common way to overcome this involves a light mediator, into which DM can efficiently annihilate and which subsequently decays into Standard Mod…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)media_common.quotation_subjectCosmic microwave backgroundDark matterFOS: Physical sciences01 natural sciencesStandard Modelsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPlanck010306 general physicsParticle Physics - Phenomenologymedia_commonPhysicsCosmologia010308 nuclear & particles physicsMatter power spectrumAstronomy and AstrophysicsUniverseBaryonHigh Energy Physics - Phenomenology13. Climate actionDark radiationsymbolsAstrophysics - Cosmology and Nongalactic Astrophysics
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Constraining the cosmic radiation density due to lepton number with Big Bang Nucleosynthesis

2011

The cosmic energy density in the form of radiation before and during Big Bang Nucleosynthesis (BBN) is typically parameterized in terms of the effective number of neutrinos N_eff. This quantity, in case of no extra degrees of freedom, depends upon the chemical potential and the temperature characterizing the three active neutrino distributions, as well as by their possible non-thermal features. In the present analysis we determine the upper bounds that BBN places on N_eff from primordial neutrino--antineutrino asymmetries, with a careful treatment of the dynamics of neutrino oscillations. We consider quite a wide range for the total lepton number in the neutrino sector, eta_nu= eta_{nu_e}+e…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)media_common.quotation_subjectFOS: Physical sciences01 natural sciences7. Clean energysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesisNucleosynthesis0103 physical sciencesPlanck010306 general physicsNeutrino oscillationmedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaAstronomy and AstrophysicsLepton numberUniverseHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentNeutrinoElectron neutrinoAstrophysics - Cosmology and Nongalactic Astrophysics
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Study of dimuon production in photon-photon collisions and measurement of QED photon structure functions at LEP

2001

Muon pair production in the process e+e- -> e+e-mu+mu- is studied using the data taken at LEP1 (sqrt(s) \simeq m_Z) with the DELPHI detector during the years 1992-1995. The corresponding integrated luminosity is 138.5 pb^{-1}. The QED predictions have been tested over the whole Q^2 range accessible at LEP1 (from several GeV^2/c^4 to several hundred GeV^2/c^4) by comparing experimental distributions with distributions resulting from Monte Carlo simulations using various generators. Selected events are used to extract the leptonic photon structure function F_2^\gamma. Azimuthal correlations are used to obtain information on additional structure functions, F_A^\gamma and F_B^\gamma, which orig…

Particle physicsE+E ANNIHILATIONPhotonPhysics and Astronomy (miscellaneous)PAIR PRODUCTIONAstrophysics::High Energy Astrophysical Phenomena4-LEPTON FINAL-STATES; GAMMA-GAMMA-COLLISIONS; MONTE-CARLO SIMULATION; PAIR PRODUCTION; AZIMUTHAL CORRELATIONS; RADIATIVE-CORRECTIONS; E+E ANNIHILATION; MUON PAIRS; 4TH ORDER; SCATTERINGMONTE-CARLO SIMULATIONMonte Carlo methodFOS: Physical sciences01 natural sciences7. Clean energyPartícules (Física nuclear)High Energy Physics - ExperimentAZIMUTHAL CORRELATIONSHigh Energy Physics - Experiment (hep-ex)4TH ORDER0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSSCATTERING010306 general physicsEngineering (miscellaneous)DELPHIPhysicsMuonLuminosity (scattering theory)010308 nuclear & particles physicsMUON PAIRSHigh Energy Physics::PhenomenologyGAMMA-GAMMA-COLLISIONSLARGE ELECTRON POSITRON COLLIDERPhoton structure function3. Good healthScattering amplitude4-LEPTON FINAL-STATESPair productionPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSProduction (computer science)Física nuclearHigh Energy Physics::ExperimentParticle Physics - Experiment
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Cross-sections and leptonic forward-backward asymmetries from the Z(0) running of LEP

2000

During 1993 and 1995 LEP was run at 3 energies near the Z $^0$ peak in order to give improved measurements of the mass and width of the resonance. During 1994, LEP operated only at the Z $^0$ peak. In total DELPHI accumulated data corresponding to an integrated luminosity of approximately 116 pb $^{-1}$ . Analyses of the hadronic cross-sections and of the cross-sections and forward-backward asymmetries in the leptonic channels used the most precise evaluations of the LEP energies. In the dimuon channel, events with a photon radiated from the initial state have been used to probe the cross-sections and asymmetries down to PETRA energies. Model independent fits to all DELPHI lineshape and asy…

Particle physicsE+E ANNIHILATIONPhysics and Astronomy (miscellaneous)Electron–positron annihilationSQUARE-ROOT-S=29 GEVHadronCHARGE ASYMMETRIES01 natural sciencesResonance (particle physics)LuminosityStandard ModelNuclear physicsMONTE-CARLOSLC ENERGIES0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSANGLE BHABHA SCATTERING010306 general physicsEngineering (miscellaneous)DELPHIPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)Weinberg angleMUON-PAIR PRODUCTIONSQUARE-ROOT-SLARGE ELECTRON POSITRON COLLIDEROF-MASS ENERGIESPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica nuclearMUON-PAIR PRODUCTION; ANGLE BHABHA SCATTERING; OF-MASS ENERGIES; SQUARE-ROOT-S; MONTE-CARLO; RADIATIVE-CORRECTIONS; SQUARE-ROOT-S=29 GEV; CHARGE ASYMMETRIES; E+E ANNIHILATION; SLC ENERGIESParticle Physics - Experiment
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Observation of the Decay B+→K+K−π+

2007

We report the observation of charmless hadronic decays of charged B mesons to the final state K + K − π + . Using a data sample of 347.5     fb − 1 collected at the Υ ( 4 S ) resonance with the BABAR detector, we observe 429 ± 43 signal events with a significance of 9.6 σ . We measure the inclusive branching fraction B ( B + → K + K − π + ) = [ 5.0 ± 0.5 ( stat ) ± 0.5 ( syst ) ] × 10 − 6 . Inspection of the Dalitz plot of signal candidates shows a broad structure peaking near 1.5     GeV / c 2 in the K + K − invariant mass distribution. We find the direct C P asymmetry to be consistent with zero.

Particle physicsElectron–positron annihilationDalitz plotHadronGeneral Physics and AstronomyDalitz plotCharged particle01 natural sciencesResonanceNuclear physicsCharmless hadronic decay0103 physical sciencesB mesonInvariant massNuclear Experiment010306 general physicsBoronPhysicsSignal analysi010308 nuclear & particles physicsBranching fractionParticle physicsResonanceMesonPair productionHigh Energy Physics::ExperimentBranching fractionFísica de partículesExperiments
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Study of e+e−→γωJ/ψ and Observation of X(3872)→ωJ/ψ

2019

We study the e^{+}e^{-}→γωJ/ψ process using 11.6  fb^{-1} e^{+}e^{-} annihilation data taken at center-of-mass energies from sqrt[s]=4.008  GeV to 4.600 GeV with the BESIII detector at the BEPCII storage ring. The X(3872) resonance is observed for the first time in the ωJ/ψ system with a significance of more than 5σ. The relative decay ratio of X(3872)→ωJ/ψ and π^{+}π^{-}J/ψ is measured to be R=1.6_{-0.3}^{+0.4}±0.2, where the first uncertainty is statistical and the second systematic (the same hereafter). The sqrt[s]-dependent cross section of e^{+}e^{-}→γX(3872) is also measured and investigated, and it can be described by a single Breit-Wigner resonance, referred to as the Y(4200), with …

Particle physicsElectron–positron annihilationGeneral Physics and Astronomy01 natural sciencesSpectral linelaw.inventionLuminosityNuclear physicsCross section (physics)law0103 physical sciencesInvariant massCollider010306 general physicsPhysicsAnnihilationMass distribution010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)ResonanceBaryonPhase spaceHigh Energy Physics::ExperimentCenter of massAtomic physicsEnergy (signal processing)Storage ringBar (unit)X(3872)Physical Review Letters
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