Search results for " oscillation"

showing 10 items of 845 documents

Cornering solar radiative-zone fluctuations with KamLAND and SNO salt

2003

We update the best constraints on fluctuations in the solar medium deep within the solar Radiative Zone to include the new SNO-salt solar neutrino measurements. We find that these new measurements are now sufficiently precise that neutrino oscillation parameters can be inferred independently of any assumptions about fluctuation properties. Constraints on fluctuations are also improved, with amplitudes of 5% now excluded at the 99% confidence level for correlation lengths in the range of several hundred km. Because they are sensitive to correlation lengths which are so short, these solar neutrino results are complementary to constraints coming from helioseismology.

PhysicsParticle physics010308 nuclear & particles physicsSolar neutrinoAstrophysics (astro-ph)FísicaFOS: Physical sciencesAstronomy and AstrophysicsAstrophysics01 natural sciencesRadiation zoneComputational physicsHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesPhysics::Space PhysicsRange (statistics)Astrophysics::Solar and Stellar AstrophysicsHigh Energy Physics::ExperimentHelioseismology010306 general physicsNeutrino oscillation
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Search for CP Violation in Neutrino and Antineutrino Oscillations by the T2K Experiment with 2.2×1021 Protons on Target

2018

The T2K experiment measures muon neutrino disappearance and electron neutrino appearance in accelerator-produced neutrino and antineutrino beams. With an exposure of $14.7(7.6)\times 10^{20}$ protons on target in neutrino (antineutrino) mode, 89 $\nu_e$ candidates and 7 anti-$\nu_e$ candidates were observed while 67.5 and 9.0 are expected for $\delta_{CP}=0$ and normal mass ordering. The obtained $2\sigma$ confidence interval for the $CP$ violating phase, $\delta_{CP}$, does not include the $CP$-conserving cases ($\delta_{CP}=0,\pi$). The best-fit values of other parameters are $\sin^2\theta_{23} = 0.526^{+0.032}_{-0.036}$ and $\Delta m^2_{32}=2.463\pm0.065\times10^{-3} \mathrm{eV}^2/c^4$.

PhysicsParticle physics010308 nuclear & particles physicsT2K experimentGeneral Physics and Astronomy01 natural sciencesNeutrino detector0103 physical sciencesCP violationMuon neutrinoNeutrino010306 general physicsNeutrino oscillationElectron neutrinoPhysical Review Letters
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Non-standard interactions: Atmospheric versus neutrino factory experiments

2001

We consider the potential of a generic neutrino factory (NUFACT) in probing non-standard neutrino-matter interactions (NSI). We find that the sensitivity to flavour-changing (FC) NSI can be substantially improved with respect to present atmospheric neutrino data, especially at energies higher than approximately 50 GeV, where the effect of the tau mass is small. For example, a 100 GeV NUFACT can probe FC neutrino interactions at the level of few $|\epsilon| < {few} \times 10^{-4}$ at 99 % C.L.

PhysicsParticle physicsAtmospheric neutrinosNuclear and High Energy PhysicsNeutrino mass and mixingNeutrino oscillationsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyNeutrino factoryFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Neutrino FactoryHigh Energy Physics::ExperimentSensitivity (control systems)Atmospheric neutrinoNeutrino
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Observability of the Neutrino Charge Radius

2002

It is shown that the probe-independent charge radius of the neutrino is a physical observable; as such, it may be extracted from experiment, at least in principle. This is accomplished by expressing a set of experimental ${\ensuremath{\nu}}_{\ensuremath{\mu}}\mathrm{\text{\ensuremath{-}}}e$ cross sections in terms of the finite charge radius and two additional gauge- and renormalization-group-invariant quantities, corresponding to the electroweak effective charge and mixing angle.

PhysicsParticle physicsCharge radiusQuantum mechanicsElectroweak interactionGeneral Physics and AstronomyMeasurements of neutrino speedObservableGauge (firearms)NeutrinoNeutrino oscillationEffective nuclear chargePhysical Review Letters
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Ultralight dark photon as a model for early universe dark matter

2019

Dark photon is a massive vector field which interacts only with the physical photon through the kinetic mixing. This coupling is assumed to be weak so that the dark photon becomes almost unobservable in processes with elementary particles, but can serve as a dark matter particle. We argue that in very early Universe ($z>3000$) this vector field may have the equation of state of radiation ($w=1/3$) but later behaves as cold dark matter ($w=0$). This may slightly change the expansion rate of the Universe at early time and reduce the value of the sound horizon of baryon acoustic oscillations (standard ruler). As a result, in this model the value of the Hubble constant appears to be larger than…

PhysicsParticle physicsCold dark matterCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsEquation of state (cosmology)Dark matterOrder (ring theory)FOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsCoupling (probability)01 natural sciencesDark photonsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessymbolsBaryon acoustic oscillations010306 general physicsHubble's lawAstrophysics - Cosmology and Nongalactic Astrophysics
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Constraints on electromagnetic form factors of sub-GeV dark matter from the cosmic microwave background anisotropy

2021

We consider dark matter which have non-zero electromagnetic form factors like electric/magnetic dipole moments and anapole moment for fermionic dark matter and Rayleigh form factor for scalar dark matter. We consider dark matter mass $m_\chi > \cal{ O}({\rm MeV})$ and put constraints on their mass and electromagnetic couplings from CMB and LSS observations. Fermionic dark matter with non-zero electromagnetic form factors can annihilate to $e^+ e^-$ and scalar dark matter can annihilate to $2\gamma$ at the time of recombination and distort the CMB. We analyze dark matter with multipole moments with Planck and BAO observations. We find upper bounds on anapole moment $g_{A}<7.163\times 10^{3} …

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Magnetic momentScalar (mathematics)Dark matterForm factor (quantum field theory)FOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsHigh Energy Physics - PhenomenologyElectric dipole momentHigh Energy Physics - Phenomenology (hep-ph)Baryon acoustic oscillationsMultipole expansionMagnetic dipoleAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Resurrection of large lepton number asymmetries from neutrino flavor oscillations

2016

We numerically solve the evolution equations of neutrino three-flavor density matrices, and show that, even if neutrino oscillations mix neutrino flavors, large lepton number asymmetries are still allowed in certain limits by Big Bang Nucleosynthesis (BBN).

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesLepton numberNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesis0103 physical sciencesMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationFlavorAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Zooming in on neutrino oscillations with DUNE

2018

We examine the capabilities of the DUNE experiment as a probe of the neutrino mixing paradigm. Taking the current status of neutrino oscillations and the design specifications of DUNE, we determine the experiment's potential to probe the structure of neutrino mixing and CP violation. We focus on the poorly determined parameters $\theta_{23}$ and $\delta_{CP}$ and consider both two and seven years of run. We take various benchmarks as our true values, such as the current preferred values of $\theta_{23}$ and $\delta_{CP}$, as well as several theory-motivated choices. We determine quantitatively DUNE's potential to perform a precision measurement of $\theta_{23}$, as well as to test the CP vi…

PhysicsParticle physicsCurrent (mathematics)010308 nuclear & particles physicsFOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino010306 general physicsNeutrino oscillationMixing (physics)
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X-ray photons from late-decaying majoron dark matter

2008

An attractive way to generate neutrino masses as required to account for current neutrino oscillation data involves the spontaneous breaking of lepton number. The resulting majoron may pick up a mass due to gravity. If its mass lies in the kilovolt scale, the majoron can play the role of late-decaying Dark Matter (LDDM), decaying mainly to neutrinos. In general the majoron has also a sub-dominant decay to two photons leading to a mono-energetic emission line which can be used as a test of the LDDM scenario. We compare expected photon emission rates with observations in order to obtain model independent restrictions on the relevant parameters. We also illustrate the resulting sensitivities w…

PhysicsParticle physicsDark matterAstrophysics (astro-ph)High Energy Physics::PhenomenologyCosmic background radiationFOS: Physical sciencesFísicaAstronomy and AstrophysicsAstrophysicsLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHiggs bosonHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMajoron
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A Monochromatic Neutrino Beam to Obtain U(e3) and the CP Phase

2007

The goal for future neutrino facilities is the determination of the [Ue3] mixing and CP violation in neutrino oscillations. This will require precision experiments with a very intense neutrino source. The future experiments such as T2K, NOVA and Double CHOOZ will measure the [Ue3] mixing. In order to explore CP violation, we present a novel method to create a monochromatic neutrino beam based on the recent discovery of nuclei that decay fast through electron capture in a superallowed Gamow-Teller transition. The boost of such radioactive ions will generate an intense monochromatic directional neutrino beam when decaying at high energy in a storage ring with long straight sections. We show t…

PhysicsParticle physicsElectron capturePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaCHOOZSolar neutrino problemNuclear physicsCP violationMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationAIP Conference Proceedings
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