Search results for "53"

showing 10 items of 2908 documents

Photoproduction of $\eta$ $\pi$ pairs off nucleons and deuterons

2016

Quasi-free photoproduction of $\pi\eta$-pairs has been investigated from threshold up to incident photon energies of 1.4 GeV, respectively up to photon-nucleon invariant masses up to 1.9 GeV. Total cross sections, angular distributions, invariant-mass distributions of the $\pi\eta$ and meson-nucleon pairs, and beam-helicity asymmetries have been measured for the reactions $\gamma p\rightarrow p\pi^0\eta$, $\gamma n\rightarrow n\pi^0\eta$, $\gamma p\rightarrow n\pi^+\eta$, and $\gamma n\rightarrow p\pi^-\eta$ from nucleons bound inside the deuteron. For the $\gamma p$ initial state data for free protons have also been analyzed. Finally, the total cross sections for quasi-free production of $…

PhysicsNuclear and High Energy PhysicsPhotonProton010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciences01 natural sciences7. Clean energyNuclear physicsDeuteriumREACTION GAMMA-P ; TAGGED PHOTON SPECTROMETER ; I-CIRCLE-DOT ; MESON PHOTOPRODUCTION ; HIGH-STATISTICS ; PROTON ; THRESHOLD ; MAMI ; POLARIZATION ; PI(0)-PAIRS0103 physical sciencesPiNeutronHigh Energy Physics::Experimentddc:530Decay chainNuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear ExperimentNuclear ExperimentCrystal Ball
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Production and characterization of a custom-made 228Th source with reduced neutron source strength for the Borexino experiment

2012

A custom-made 228Th source of several MBq activity was produced for the Borexino experiment for studying the external background of the detector. The aim was to reduce the unwanted neutron emission produced via (alpha,n) reactions in ceramics used typically for commercial 228Th sources. For this purpose a ThCl4 solution was converted chemically into ThO2 and embedded into a gold foil. The paper describes the production and the characterization of the custom-made source by means of gamma-activity, dose rate and neutron source strength measurements. From gamma-spectroscopic measurements it was deduced that the activity transfer from the initial solution to the final source was >91% (at 68%…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsDosimeterIsotope530 PhysicsNeutron emission3105 InstrumentationRadiochemistryFOS: Physical sciencesThoriumchemistry.chemical_elementInstrumentation and Detectors (physics.ins-det)10192 Physics InstituteNuclear physicschemistryMeasuring instrumentNeutron source3106 Nuclear and High Energy PhysicsInstrumentationBorexinoIsotopes of thoriumNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Coherent Smith-Purcell radiation for minimally invasive bunch length measurement at the subpicosecond time scale

2021

Physical review accelerators and beams 24(4), 042803 (2021). doi:10.1103/PhysRevAccelBeams.24.042803

PhysicsNuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsbusiness.industryScale (descriptive set theory)QC770-798Surfaces and InterfacesRadiation53001 natural sciencesMeasure (mathematics)Superconducting acceleratorSpace chargeLength measurementOpticsNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesCathode rayPhysics::Accelerator Physicsddc:530010306 general physicsbusinessBeam (structure)Physical Review Accelerators and Beams
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Cross section ratio and angular distributions of the reaction p + d -> 3He + eta at 48.8 MeV and 59.8 MeV excess energy

2014

We present new data for angular distributions and on the cross section ratio of the p + d -> 3He + eta reaction at excess energies of Q = 48.8 MeV and Q = 59.8 MeV. The data have been obtained at the WASA-at-COSY experiment (Forschungszentrum J\"ulich) using a proton beam and a deuterium pellet target. While the shape of obtained angular distributions show only a slow variation with the energy, the new results indicate a distinct and unexpected total cross section fluctuation between Q = 20 MeV and Q = 60 MeV, which might indicate the variation of the production mechanism within this energy interval.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear TheoryIntermediate EnergiesEta01 natural sciences7. Clean energyNuclear physicsCross section (physics)Tensor Analyzing PowerDeuteriumNear-Threshold0103 physical sciencesEnergy intervalPhysics::Accelerator Physicsddc:530010306 general physicsNuclear ExperimentExcess energyNuclear ExperimentBeam (structure)
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Lower bound on the proton charge radius from electron scattering data

2019

The proton charge-radius determinations from the electromagnetic form-factor measurements in electron-proton scattering require an extrapolation to zero momentum transfer ($Q^2=0$) which is prone to model-dependent assumptions. We show that the data at finite momentum transfer can be used to establish a rigorous lower bound on the proton charge radius. Using the available $ep$ data at low $Q^2$, we obtain $R_E > 0.850(1)$ fm as the lower bound on the proton radius. This reaffirms the discrepancy between the $ep$ and muonic-hydrogen values, while bypassing the model-dependent assumptions that go into the fitting and extrapolation of the $ep$ data.

PhysicsNuclear and High Energy PhysicsProtonNuclear Theory010308 nuclear & particles physicsScattering530 PhysicsMomentum transferExtrapolationFOS: Physical sciencesCharge densityRadius01 natural sciencesUpper and lower boundslcsh:QC1-999Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Charge radius0103 physical sciencesNuclear Experiment (nucl-ex)Atomic physics010306 general physicsNuclear Experimentlcsh:Physics
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Technical design report for the $\overline{{\rm{P}}}\mathrm{ANDA}$ Barrel DIRC detector

2019

The $\overline{{\rm{P}}}\mathrm{ANDA}$ (anti-Proton ANnihiliation at DArmstadt) experiment will be one of the four flagship experiments at the new international accelerator complex FAIR (Facility for Antiproton and Ion Research) in Darmstadt, Germany. $\overline{{\rm{P}}}\mathrm{ANDA}$ will address fundamental questions of hadron physics and quantum chromodynamics using high-intensity cooled antiproton beams with momenta between 1.5 and 15 GeV/c and a design luminosity of up to 2 × 1032 cm−2 s−1. Excellent particle identification (PID) is crucial to the success of the $\overline{{\rm{P}}}\mathrm{ANDA}$ physics program. Hadronic PID in the barrel region of the target spectrometer will be per…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Large Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHadronDetectorBarrel (horology)7. Clean energy01 natural sciencesRing-imaging Cherenkov detectorParticle identificationCharged particleNuclear physics0103 physical sciencesHigh Energy Physics::Experimentddc:530010306 general physicsNuclear Experiment
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Exclusive ϱ0 and φ muoproduction at large Q2

1994

Abstract Exclusive ϱ 0 and φ muoproduction on deuterium, carbon and calcium has been studied in the kinematic range 2 Q 2 2 and 40 Q 2 dependence of the cross sections, the transverse momentum distributions for the vector mesons, the decay angular distributions and, in the case of the ϱ 0 , nuclear effects. The data for 0 production are compatible with a diffractive mechanism. The distinct features of φ production are a smaller cross section and less steep p t 2 distributions than those for the 0 mesons.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsMesonHADRONSMUON SCATTERINGTRANSVERSE-MOMENTUMPROTONQCD530Nuclear physicsCross section (physics)RATIOAngular distributionDeuteriumTransverse momentumDEEP INELASTIC-SCATTERING; MUON SCATTERING; TRANSVERSE-MOMENTUM; PROTON; HADRONS; RATIO; QCDDEEP INELASTIC-SCATTERINGNuclear Physics B
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Recent progress in laser spectroscopy of the actinides

2020

The interest to perform laser spectroscopy in the heaviest elements arises from the strong impact of relativistic effects, electron correlations and quantum electrodynamics on their atomic structure. Once this atomic structure is well understood, laser spectroscopy also provides access to nuclear properties such as spins, mean square charge radii and electromagnetic moments in a nuclear-model independent way. This is of particular interest for the heaviest actinides around $N = 152$, a region of shell stabilized deformed nuclei. The experimental progress of laser spectroscopy in this region benefitted from continuous methodological and technical developments such as the introduction of buff…

PhysicsNuclear and High Energy PhysicsSpins010308 nuclear & particles physicsAtomic Physics (physics.atom-ph)Nuclear Theorychemistry.chemical_elementFOS: Physical sciencesCharge (physics)ActinideElectron01 natural sciencesPhysics - Atomic Physics3. Good healthNuclear physicschemistry0103 physical sciencesddc:530NobeliumNuclide010306 general physicsRelativistic quantum chemistrySpectroscopyNuclear ExperimentProgress in Particle and Nuclear Physics
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Coulomb and nuclear excitations of narrow resonances in 17Ne

2016

Physics letters / B 759, 200 - 205 (2016). doi:10.1016/j.physletb.2016.05.073

PhysicsNuclear and High Energy PhysicsTeoría de los quantaInternal energySpins010308 nuclear & particles physicsProjectile310601 natural sciences530lcsh:QC1-999Mass formulaNuclear physics0103 physical sciencesPhysical SciencesCoulombIsobaric processFysikddc:530Atomic physics010306 general physicsMultipletExcitationlcsh:PhysicsPhysics Letters B
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Modelling of the magnetic field structures and first measurements of heat fluxes for TEXTOR-DED operation

2004

The dynamic ergodic divertor (DED) was recently installed at the TEXTOR tokamak. One of the aims of the DED is to control and study heat and particle deposition on a plasma wall via modification of the plasma edge by external perturbation coils. Sixteen perturbation coils are mounted on the high-field side of the torus. The external magnetic perturbation creates a zone of chaotic field lines at the plasma edge by destroying several resonant surfaces. These structures have the properties of an open chaotic system while the field lines intersect the tokamak vessel. In order to study the topology of the field lines in different regimes, a set of tools called Atlas was created. Atlas uses a sym…

PhysicsNuclear and High Energy PhysicsTokamakField lineDivertorChaoticPerturbation (astronomy)TorusPlasmaCondensed Matter PhysicsComputational physicslaw.inventionMagnetic fieldJlawPhysics::Plasma Physicsddc:530Atomic physics
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