Search results for "Magnitude"

showing 10 items of 501 documents

Constraining Majorana neutrino electromagnetic properties from the LMA-MSW solution of the solar neutrino problem

2002

In this paper we use solar neutrino data to derive stringent bounds on Majorana neutrino transition moments (TMs). Should such be present, they would contribute to the neutrino--electron scattering cross section and hence alter the signal observed in Super-Kamiokande. Motivated by the growing robustness of the LMA-MSW solution of the solar neutrino problem indicated by recent data, and also by the prospects of its possible confirmation at KamLAND, we assume the validity of this solution, and we constrain neutrino TMs by using the latest global solar neutrino data. We find that all elements of the TM matrix can be bounded at the same time. Furthermore, we show how reactor data play a complem…

PhysicsNuclear and High Energy PhysicsParticle physicsOscillationSolar neutrinoHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSolar neutrino problemMatrix (mathematics)MAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoBorexinoOrder of magnitude
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Confusing non-standard neutrino interactions with oscillations at a neutrino factory

2002

Most neutrino mass theories contain non-standard interactions (NSI) of neutrinos which can be either non-universal (NU) or flavor-changing (FC). We study the impact of such interactions on the determination of neutrino mixing parameters at a neutrino factory using the so-called ``golden channels'' \pnu{e}\to\pnu{\mu} for the measurement of \theta_{13}. We show that a certain combination of FC interactions in neutrino source and earth matter can give exactly the same signal as oscillations arising due to \theta_{13}. This implies that information about \theta_{13} can only be obtained if bounds on NSI are available. Taking into account the existing bounds on FC interactions, this leads to a …

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Neutrino FactoryHigh Energy Physics::ExperimentSensitivity (control systems)NeutrinoNeutrino oscillationOrder of magnitudeMixing (physics)
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Radiative corrections for Dalitz decays of π0, η(′) and Σ0

2020

Abstract We briefly summarize current experimental and theoretical results on the π 0 Dalitz decay, and provide a new value for the ratio R = Γ ( π 0 → e + e − γ ( γ ) ) / Γ ( π 0 → γ γ ) = 11.978 ( 6 ) × 10 − 3 , which is by two orders of magnitude more precise than the current PDG average. This value is obtained using the complete set of the next-to-leading-order radiative corrections in the QED sector, and incorporates up-to-date values of the π 0 -transition-form-factor slope. Furthermore, we present the complete set of radiative corrections for the Dalitz decays η ( ′ ) → l + l − γ beyond the soft-photon approximation. The corrections inevitably depend on the η ( ′ ) → γ ⁎ γ ( ⁎ ) tran…

PhysicsNuclear and High Energy PhysicsParticle physicsRadiative transferOrder of magnitudeNuclear and Particle Physics Proceedings
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A trigger system for measurements of proton-induced rare hadronic reactions around Tp=400MeV

2008

Abstract We developed a trigger system for the measurement of proton-induced rare hadronic reactions around the beam kinetic energy T p = 400 MeV based on highly segmented trigger scintillation detectors and programmable logic modules. The trigger system was designed to enhance events with the negative-pion production by the difference of the curvatures of the particle tracks in a magnetic field. Since the production cross-section of the negative-pion by the proton-induced reactions was smaller by about 3 orders of magnitude than the total cross-section around the beam energy, we expected large reduction of the trigger rate by the negative-pion selection. The construction of the trigger sys…

PhysicsNuclear and High Energy PhysicsParticle physicsScintillationProtonOrders of magnitude (temperature)Nuclear TheoryDetectorHadronKinetic energyMagnetic fieldNuclear physicsPhysics::Accelerator PhysicsNuclear ExperimentInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Bounds on the Solar Antineutrino total Flux and Energy spectrum from the SK experiment

1999

A search for inverse beta decay electron antineutrinos has been carried out using the 825 days sample of solar data obtained at SK. The absence of a significant signal, that is, contributions to the total SK background and their angular variations has set upper bounds on a) the absolute flux of solar antineutrinos originated from ${}^8 B$ neutrinos $��_{\bar��}({}^8 B)=< 1.8\times 10^5 cm^{-2} s^{-1}$ which is equivalent to an averaged conversion probability bound of P<3.5% (SSM-BP98 model) and b) their differential energy spectrum, the conversion probability is smaller than 8% for all $E_{e,vis}>6.5$ MeV going down the 5% level above $E_{e,vis}\approx 10$ MeV. It is shown that an …

PhysicsNuclear and High Energy PhysicsParticle physicsSolar neutrinoFluxFOS: Physical sciencesElectronApproxHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Inverse beta decayMagnitude (astronomy)High Energy Physics::ExperimentNeutrinoBar (unit)
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ProjectileΔand target Roper excitation in thep(d,d′)Xreaction

2000

In this paper we compare a model that contains the mechanisms of $\ensuremath{\Delta}$ excitation in the projectile and Roper excitation in the target with experimental data from two ${(d,d}^{\ensuremath{'}})$ experiments on a proton target. The agreement of the theory with the experiment is fair for the data taken at ${T}_{d}=2.3$ GeV. The $\ensuremath{\Delta}$ excitation in the projectile is predicted close to the observed energy with the correct width. The theory, however, underpredicts by about 40% the cross sections measured at ${T}_{d} = 1.6$ GeV at angles where the cross section has fallen by about two orders of magnitude. The analysis done here allows us to extract an approximate st…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsProjectile01 natural sciencesNuclear physicsCross section (physics)0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsNuclear theoryExcitationEnergy (signal processing)Order of magnitudePhysical Review C
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Quantum decoherence and neutrino data

2006

In this work we perform global fits of microscopic decoherence models of neutrinos to all available current data, including LSND and KamLAND spectral distortion results. In previous works on related issues the models used were supposed to explain LSND results by means of quantum gravity induced decoherence. However those models were purely phenomenological without any underlying microscopic basis. It is one of the main purposes of this article to use detailed microscopic decoherence models with complete positivity, to fit the data.The decoherence in these models has contributions not only from stochastic quantum gravity vacua operating as a medium, but also from conventional uncertainties i…

PhysicsNuclear and High Energy PhysicsQuantum decoherenceOscillationFOS: Physical sciencesFísicaNeutrino beamHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsQuantum gravityHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationOrder of magnitudeEnergy (signal processing)Nuclear Physics B
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Quasielastic Versus Inelastic and Deep Inelastic Lepton Scattering in Nuclei at x > 1

1997

We have made a thorough investigation of the nuclear structure function W_2A in the region of 0.8 < x < 1.5 and Q^2 < 20 GeV^2, separating the quasielastic and inelastic plus deep inelastic contributions. The agreement with present experimental data is good giving support to the results for both channels. Predictions are made in yet unexplored regions of x and Q^2 to assert the weight of the quasielastic or inelastic channels. We find that at Q^2 < 4 GeV^2 the structure function is dominated by the quasielastic contributions for x < 1.5, while for values of Q^2 > 15 GeV^2 and the range of x studied the inelastic channels are over one order of magnitude bigger than the quas…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Nuclear TheoryScatteringNuclear TheoryStructure functionNuclear structureFísicaFOS: Physical sciencesFunction (mathematics)Nuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Nuclear ExperimentOrder of magnitudeLepton
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DIRECT PRODUCTION OF PIONIC ATOMS FROM RADIATIVE TRAPPING OF PIONS IN FLIGHT

1992

Abstract The reaction π−A→(πb−A)γ with Tπ=10−30 MeV producing a π− bound in the nucleus is studied to see its viability as an instrument to produce deeply bound pionic atoms in nuclei. We obtain cross sections of the order of tens of μb/ (sr MeV) for the production of the 1s and 2p states of 208Pb and negligible background from radiative pion capture and the other sources. The negligible background expected in the present reaction is unique among all other reactions so far proposed. The cross sections obtained are three orders of magnitude bigger than those in the best electromagnetic reactions previously proposed. The small background, the large cross sections and the present available flu…

PhysicsNuclear and High Energy PhysicsResolution (electron density)Nuclear TheoryTrappingNuclear physicsDirect productionPionmedicine.anatomical_structureLow energyOrders of magnitude (time)Radiative transfermedicineAtomic physicsNuclear ExperimentNucleus
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Ground-state binding energy of HΛ4 from high-resolution decay-pion spectroscopy

2016

Abstract A systematic study on the Λ ground state binding energy of hyperhydrogen H Λ 4 measured at the Mainz Microtron MAMI is presented. The energy was deduced from the spectroscopy of mono-energetic pions from the two-body decays of hyperfragments, which were produced and stopped in a 9Be target. First data, taken in the year 2012 with a high resolution magnetic spectrometer, demonstrated an almost one order of magnitude higher precision than emulsion data, while being limited by systematic uncertainties. In 2014 an extended measurement campaign was performed with improved control over systematic effects, increasing the yield of hypernuclei and confirming the observation with two indepen…

PhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsBinding energy01 natural sciencesNuclear physicsPion0103 physical sciencesSymmetry breaking010306 general physicsSpectroscopyGround stateMicrotronOrder of magnitudeNuclear Physics A
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