Search results for "nuclear physics"

showing 10 items of 5307 documents

Intense source of slow positrons from pulsed electron accelerators

1984

A pulsed LINAC is used for pair production in a tantalum target of 2.5 radiation lengths in an energy range from 80 to 260 MeV. Several well-annealed tungsten vanes are placed immediately behind the target and thermalize a small fraction of the fast positrons. The slow positrons are extracted from the target region and magnetically guided over a distance of 17 m to the detector at the end of an S-shaped solenoid. Two Nal detectors with well-known detection efficiency are used to register the 511 keV annihilationγ-rays. To reduce pile-up effects 50 mm of Pb were placed in front of the detectors. At an average electron current of 1 μA we could detect about 107 slow positrons per second. The p…

PhysicsRange (particle radiation)Physics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsGeneral EngineeringParticle acceleratorSolenoidGeneral ChemistryElectronRadiationLinear particle acceleratorlaw.inventionNuclear physicsPositronPair productionlawPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentGeneral Materials ScienceAtomic physicsApplied Physics A Solids and Surfaces
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High-voltage monitoring with a solenoid retarding spectrometer at the KATRIN experiment

2014

The KATRIN experiment will measure the absolute mass scale of neutrinos with a sensitivity of m(ν) = 200meV/c(2) by means of an electrostatic spectrometer set close to the tritium β-decay endpoint at 18.6keV. Fluctuations of the energy scale must be under control within ±60mV (±3ppm). Since a precise voltage measurement in the range of tens of kV is on the edge of current technology, a nuclear standard will be deployed additionally. Parallel to the main spectrometer the same retarding potential will be applied to the monitor spectrometer to measure 17.8-keV K-conversion electrons of (83m)Kr. This article describes the setup of the monitor spectrometer and presents its first measurement resu…

PhysicsRange (particle radiation)SpectrometerPhysics::Instrumentation and DetectorsMeasure (physics)High voltageSolenoidNuclear physicsDetectors and Experimental TechniquesNeutrinoInstrumentationMathematical PhysicsKATRINVoltageJournal of Instrumentation
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Lifetime measurements of excited states in W162 and W164 and the evolution of collectivity in rare-earth nuclei

2017

Lifetimes of the first excited 2(+) states in the extremely neutron- deficient W-162 and W-164 nuclei have been measured using the recoil distance Doppler shift technique. Experimental B(E2) data f ...

PhysicsRare earth nuclei010308 nuclear & particles physicsNuclear Theory7. Clean energy01 natural sciencesNuclear physicssymbols.namesakeRecoilExcited state0103 physical sciencessymbolsNeutronAtomic physicsNuclear Experiment010306 general physicsDoppler effectPhysical Review C
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Improving the nuclear physics input along the rp-process path

2007

The level structure of 30 S was studied at the NSCL by using neutron removal reactions with a radioactive 31 S beam. The γ -decay from excited states in 30 S was measured in a Ge-detector array. The results discussed for this work will reduce the uncertainties in the determination of the astrophysical 29 P(p, γ ) 30 S reaction rate under rp -process conditions.

PhysicsReaction rateNuclear physicsNuclear and High Energy PhysicsWork (thermodynamics)Excited statePath (graph theory)Level structureNeutronrp-processAtomic physicsNuclear ExperimentBeam (structure)Nuclear Physics A
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Neutrino flux prediction at MiniBooNE

2009

The booster neutrino experiment (MiniBooNE) searches for nu(mu)->nu(e) oscillations using the O(1 GeV) neutrino beam produced by the booster synchrotron at the Fermi National Accelerator Laboratory). The booster delivers protons with 8 GeV kinetic energy (8.89 GeV/c momentum) to a beryllium target, producing neutrinos from the decay of secondary particles in the beam line. We describe the Monte Carlo simulation methods used to estimate the flux of neutrinos from the beam line incident on the MiniBooNE detector for both polarities of the focusing horn. The simulation uses the Geant4 framework for propagating particles, accounting for electromagnetic processes and hadronic interactions in the…

PhysicsResearch Groups and Centres\Physics\Low Temperature PhysicsNuclear and High Energy PhysicsParticle physicsMesonFaculty of Science\PhysicsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesHigh Energy Physics - ExperimentMassless particleMiniBooNENuclear physicsHigh Energy Physics - Experiment (hep-ex)PionPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentFermilabNeutrinoNuclear ExperimentNeutrino oscillationLeptonPhysical Review D
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Low-lying excitations in Ni 72

2016

A. I. Morales et al.; 14 págs.; 9 figs.; 3 tabs.

PhysicsSIMPLE (dark matter experiment)Nuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsFissionNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsExcited state0103 physical sciencesNeutronAtomic physics010306 general physics
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EXTRACTION OF THE Λ(1405) POLES FROM π0Σ0 PHOTOPRODUCTION DATA

2014

In this contribution we review a work where we showed how to extract the position of the two Λ(1405) poles from experimental photoproduction data which have been measured recently in the γp → K+π0Σ0 reaction at Jefferson Lab. Using a potential motivated by chiral dynamics but with free parameters, we solve the Bethe Salpeter equation in the coupled channels [Formula: see text] and πΣ in isospin I=0 and parameterize the amplitude for the photonuclear reaction in terms of a linear combination of the πΣ → πΣ and [Formula: see text] scattering amplitudes in I=0, with a different linear combination for each energy. Good fits to the data are obtained which lead to two poles at 1385 - 68i MeV and…

PhysicsScattering amplitudeNuclear physicsParticle physicsAmplitudeBethe–Salpeter equationUnitarityIsospinHyperonLinear combinationFree parameterInternational Journal of Modern Physics: Conference Series
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Electroproduction of hyperons

1997

Abstract We present some estimates for the reaction ep → e ′ Σ + . At small scattering angles, the differential cross section is completely determined by the experimental data for the radiative decay Σ + → pγ . For kinematical values typical of the proposed parity experiment at MAMI, we find a suppression factor of about 5 · 10 −15 as compared to elastic electron scattering. On the basis of conservative models for the transition form factors, this ratio might increase by about a factor of 20 at backward angles. Even higher values could be expected if the presently unknown convection currents should turn out to be large. Due to the parity violation involved in this process, we also expect a …

PhysicsScattering cross-sectionConvectionNuclear and High Energy PhysicsParticle physicsScatteringmedia_common.quotation_subjectHyperonElastic electronParity (physics)ElectronAsymmetryNuclear physicsmedia_commonPhysics Letters B
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Threshold Electroproduction of Charged Pions from Light Nuclei

1977

Double-differential cross sections for the electroproduction of pions of both charges have been measured. We compare the data obtained for production near threshold from $^{12}\mathrm{C}$ and $^{16}\mathrm{O}$ with theoretical treatments employing both shell-model and sum-rule nuclear descriptions with full inclusion of the final-state interaction.

PhysicsScattering cross-sectionLight nucleusNuclear TheorySHELL modelGeneral Physics and Astronomychemistry.chemical_elementNuclear physicsNear thresholdPionchemistryProduction (computer science)Atomic physicsNuclear ExperimentCarbonPhysical Review Letters
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Measurement of ϕ -meson production at forward rapidity in p+p collisions at s=510  GeV and its energy dependence from s=200  GeV to 7 TeV

2018

The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the differential cross section of φ(1020)-meson production at forward rapidity in p+p collisions at s=510 GeV via the dimuon decay channel. The partial cross section in the rapidity and pT ranges 1.2

PhysicsScattering cross-sectionMeson production010308 nuclear & particles physicsNuclear TheoryStrangeness01 natural sciencesNuclear physics0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderPhysical Review D
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