Search results for "QC770"

showing 10 items of 270 documents

Updated global analysis of neutrino oscillations in the presence of eV-scale sterile neutrinos

2018

We discuss the possibility to explain the anomalies in short-baseline neutrino oscillation experiments in terms of sterile neutrinos. We work in a 3+1 framework and pay special attention to recent new data from reactor experiments, IceCube and MINOS+. We find that results from the DANSS and NEOS reactor experiments support the sterile neutrino explanation of the reactor anomaly, based on an analysis that relies solely on the relative comparison of measured reactor spectra. Global data from the $\nu_e$ disappearance channel favour sterile neutrino oscillations at the $3\sigma$ level with $\Delta m^2_{41} \approx 1.3$ eV$^2$ and $|U_{e4}| \approx 0.1$, even without any assumptions on predicte…

Nuclear and High Energy PhysicsSterile neutrinoParticle physicsFOS: Physical sciences01 natural sciences7. Clean energySpectral lineHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530010306 general physicsNeutrino oscillationMixing (physics)Particle Physics - PhenomenologyPhysicshep-ex010308 nuclear & particles physicsOscillationPhysicsHigh Energy Physics::Phenomenologyhep-ph3. Good healthHigh Energy Physics - PhenomenologyMINOSBeyond Standard Modellcsh:QC770-798High Energy Physics::ExperimentAnomaly (physics)NeutrinoParticle Physics - ExperimentJournal of High Energy Physics
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A search for neutrino–antineutrino mass inequality by means of sterile neutrino oscillometry

2015

The investigation of the oscillation pattern induced by the sterile neutrinos might determine the oscillation parameters, and at the same time, allow to probe CPT symmetry in the leptonic sector through neutrino-antineutrino mass inequality. We propose to use a large scintillation detector like JUNO or LENA to detect electron neutrinos and electron antineutrinos from MCi electron capture or beta decay sources. Our calculations indicate that such an experiment is realistic and could be performed in parallel to the current research plans for JUNO and RENO. Requiring at least 5$\sigma$ confidence level and assuming the values of the oscillation parameters indicated by the current global fit, w…

Nuclear and High Energy PhysicsSterile neutrinoParticle physicsPhysics - Instrumentation and DetectorsElectron captureCPT symmetryFOS: Physical sciencesElectronHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)sterile neutrinoslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrino oscillationPhysicsta114OscillationHigh Energy Physics::PhenomenologyInstrumentation and Detectors (physics.ins-det)oscillation patternHigh Energy Physics - Phenomenologyelectron antineutrinoslcsh:QC770-798High Energy Physics::ExperimentNeutrinoGALLEXelectron neutrinos
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Global bounds on the Type-III Seesaw

2020

We derive general bounds on the Type-III Seesaw parameters from a global fit to flavor and electroweak precision data. We explore and compare three Type-III Seesaw realizations: a general scenario, where an arbitrary number of heavy triplets is integrated out without any further assumption, and the more constrained cases in which only 3 or 2 (minimal scenario) additional heavy states are included. The latter assumption implies rather non-trivial correlations in the Yukawa flavor structure of the model so as to reproduce the neutrino masses and mixings as measured in neutrino oscillations experiments and thus qualitative differences can be found with the more general scenario. In particular,…

Nuclear and High Energy PhysicsStructure (category theory)FOS: Physical sciencesType (model theory)01 natural sciencesPartícules (Física nuclear)Theoretical physicsOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsNeutrino oscillationPhysics010308 nuclear & particles physicsElectroweak interactionBeyond Standard Model; Neutrino PhysicsHigh Energy Physics::PhenomenologyYukawa potentialFísicaHigh Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798NeutrinoJournal of High Energy Physics
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Sensitivity of a tonne-scale NEXT detector for neutrinoless double-beta decay searches

2021

The NEXT collaboration: et al.

Nuclear and High Energy Physicschemistry.chemical_elementQC770-798Parameter space01 natural sciences7. Clean energyAtomicNuclear physicsXenonParticle and Plasma PhysicsDouble beta decayNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesDark Matter and Double Beta Decay (experiments)NuclearSensitivity (control systems)010306 general physicsMathematical PhysicsPhysicsQuantum Physics010308 nuclear & particles physicsRaigs beta -- DesintegracióDetectorMolecularDetectorsNuclear & Particles PhysicschemistryBeta rays -- DecayNeutrinoTonneOrder of magnitudeJournal of High Energy Physics
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Numerical exploration of three relativistic particles in a finite volume including two-particle resonances and bound states

2019

In this work, we use an extension of the quantization condition, given in Ref. [1], to numerically explore the finite-volume spectrum of three relativistic particles, in the case that two-particle subsets are either resonant or bound. The original form of the relativistic three-particle quantization condition was derived under a technical assumption on the two-particle K matrix that required the absence of two-particle bound states or narrow two-particle resonances. Here we describe how this restriction can be lifted in a simple way using the freedom in the definition of the K-matrix-like quantity that enters the quantization condition. With this in hand, we extend previous numerical studie…

Nuclear and High Energy Physicsnucl-thNuclear TheoryAtomic Physics (physics.atom-ph)Other Fields of Physicshep-latFOS: Physical sciencesLattice QCDphysics.atom-ph01 natural sciencesPhysics - Atomic PhysicsRelativistic particleNuclear Theory (nucl-th)Quantization (physics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. Radioactivitycond-mat.stat-mech010306 general physicsScattering AmplitudesCondensed Matter - Statistical MechanicsParticle Physics - PhenomenologyPhysicsFinite volume methodStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsScatteringHigh Energy Physics - Lattice (hep-lat)hep-phParticle Physics - LatticeLattice QCDScattering amplitudeHigh Energy Physics - PhenomenologyAmplitudeNuclear Physics - Theorylcsh:QC770-798
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Constraints on nuclear parton distributions from dijet photoproduction at the LHC

2019

Using QCD calculations of the cross section of inclusive dijet photoproduction in Pb-Pb ultraperipheral collisions in the LHC kinematics as pseudo-data, we study the effect of including these data using the Bayesian reweighting technique on nCTEQ15, nCTEQ15np, and EPPS16 nuclear parton distribution functions (nPDFs). We find that, depending on the assumed error of the pseudo-data, it leads to a significant reduction of the nPDF uncertainties at small values of the momentum fraction $x_A$. Taking the error to be 5\%, the uncertainty of nCTEQ15 and nCTEQ15np nPDFs reduces approximately by a factor of two at $x_A=10^{-3}$. At the same time, the reweighting effect on EPPS16 nPDFs is much smalle…

PB-PB COLLISIONSParticle physicsNuclear TheoryPhysics and Astronomy (miscellaneous)FOS: Physical scienceslcsh:AstrophysicsPartonhiukkasfysiikka114 Physical sciences01 natural sciencesCOLLIDERNuclear Theory (nucl-th)MomentumCross section (physics)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuantum ChromodynamicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentEngineering (miscellaneous)PhysicsQuantum chromodynamicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics - Phenomenologynuclear parton distribution functionsDistribution functionlcsh:QC770-798ydinfysiikkaVECTOR-MESONSParametrization
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Higgs-like spectator field as the origin of structure

2021

We show that the observed primordial perturbations can be entirely sourced by a light spectator scalar field with a quartic potential, akin to the Higgs boson, provided that the field is sufficiently displaced from vacuum during inflation. The framework relies on the indirect modulation of reheating, which is implemented without any direct coupling between the spectator field and the inflaton and does not require non-renormalisable interactions. The scenario gives rise to local non-Gaussianity with $f_{\rm NL}\simeq 5$ as the typical signal. As an example model where the indirect modulation mechanism is realised for the Higgs boson, we study the Standard Model extended with right-handed neu…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics and Astronomy (miscellaneous)Field (physics)FOS: Physical sciencesQC770-798Astrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicskosmologia01 natural sciences7. Clean energy114 Physical sciencesPhysics Particles & FieldsStandard ModelHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. RadioactivityQuartic function0103 physical sciences0206 Quantum Physics010303 astronomy & astrophysicsEngineering (miscellaneous)kosminen inflaatioInflation (cosmology)PhysicsScience & Technology010308 nuclear & particles physicsPhysicsHiggsin bosoniHigh Energy Physics::Phenomenologyhiukkasfysiikan standardimallihep-phInflatonPERTURBATIONSNuclear & Particles PhysicsQB460-466High Energy Physics - Phenomenologykosminen taustasäteilyPhysical Sciences0202 Atomic Molecular Nuclear Particle and Plasma Physicsastro-ph.COHiggs bosonNeutrinoScalar fieldAstrophysics - Cosmology and Nongalactic AstrophysicsThe European Physical Journal C
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Flavor versus mass eigenstates in neutrino asymmetries: implications for cosmology

2017

We show that, if they exist, lepton number asymmetries ($L_\alpha$) of neutrino flavors should be distinguished from the ones ($L_i$) of mass eigenstates, since Big Bang Nucleosynthesis (BBN) bounds on the flavor eigenstates cannot be directly applied to the mass eigenstates. Similarly, Cosmic Microwave Background (CMB) constraints on mass eigenstates do not directly constrain flavor asymmetries. Due to the difference of mass and flavor eigenstates, the cosmological constraint on the asymmetries of neutrino flavors can be much stronger than conventional expectation, but not uniquely determined unless at least the asymmetry of the heaviest neutrino is well constrained. Cosmological constrain…

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics and Astronomy (miscellaneous)media_common.quotation_subjectHigh Energy Physics::LatticeCosmic microwave backgroundCosmic background radiationFOS: Physical scienceslcsh:AstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesAsymmetryCosmologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesislcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Eigenvalues and eigenvectorsmedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyLepton numberHigh Energy Physics - Phenomenologylcsh:QC770-798High Energy Physics::ExperimentNeutrinoAstrophysics - Cosmology and Nongalactic Astrophysics
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The seesaw path to leptonic CP violation

2016

Future experiments such as SHiP and high-intensity $e^+ e^-$ colliders will have a superb sensitivity to heavy Majorana neutrinos with masses below $M_Z$. We show that the measurement of the mixing to electrons and muons of one such state could imply the discovery of leptonic CP violation in the context of seesaw models. We quantify in the minimal model the CP discovery potential of these future experiments, and demonstrate that a 5$\sigma$ CL discovery of leptonic CP violation would be possible in a very significant fraction of parameter space.

Particle physicsHeavy NeutrinoPhysics and Astronomy (miscellaneous)FOS: Physical sciencesSeesaw Modellcsh:AstrophysicsContext (language use)Parameter space01 natural sciencesMinimal modelHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrySterile Neutrinolcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Particle Physics - PhenomenologyHeavy StatePhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyLight Neutrino Massehep-phHigh Energy Physics - PhenomenologyMAJORANAlcsh:QC770-798CP violationHigh Energy Physics::ExperimentNeutrino
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How to discover QCD Instantons at the LHC

2020

Topological Effects in the Standard Model: Instantons, Sphalerons and Beyond at LHC, Geneva, Switzerland, 16 Dec 2020 - 18 Dec 2020; The European physical journal / C 81(7), 624 (2021). doi:10.1140/epjc/s10052-021-09412-1

Particle physicsInstantonp p: scatteringPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeFOS: Physical sciencesquantum [tunneling]QC770-798AstrophysicsComputer Science::Digital Libraries01 natural sciences530Standard Modelvacuum statetopologicalHigh Energy Physics::TheoryCross section (physics)High Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivityasymmetry [baryon]0103 physical sciencesscattering [p p]ddc:530quantum chromodynamics: instantonLimit (mathematics)010306 general physicsEngineering (miscellaneous)Quantum tunnellingtunneling: quantumQuantum chromodynamicsPhysicsLarge Hadron Colliderelectroweak interaction010308 nuclear & particles physicsHigh Energy Physics::Phenomenologysymmetry breaking: chiralQB460-466High Energy Physics - PhenomenologyCERN LHC Collinstanton [quantum chromodynamics]confinementbaryon: asymmetryComputer Science::Mathematical Softwarechiral [symmetry breaking]Non-perturbativesignature
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