Search results for "SPECTRA"

showing 10 items of 3542 documents

Invariant mass spectrum and α-n correlation function studied in the fragmentation of 6He on a carbon target

1998

13 pags, 5 figures.-- PACS nrs.: 24.60.−t; 25.70.Ef; 27.20.+n.

PhysicsNuclear and High Energy PhysicsReaction mechanismMomentum distributionsBreakupSpectral lineIon[PACS] Reactions induced by unstable nucleiBreakup reactions6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)Halo nucleiFragmentation mechanism[PACS] ResonancesSecondary radioactive beamsInvariant massNeutronHe-5He-6Invariant mass spectra[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsGround stateExotic nucleiNuclear Physics A
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Production cross-sections and neutron polarization in (p,n) reactions at 143 MeV

1963

Abstract Measurements have been made of the energy spectra and polarizations of neutrons emitted at a laboratory angle of 45° from deuterium, lithium and aluminium bombarded by protons of 143 MeV. The results are consistent with the view that neutron production from deuterium proceeds mainly by single quasi-free proton-neutron scattering but that multiple scattering effects predominate in heavier nuclei.

PhysicsNuclear and High Energy PhysicsScatteringAstrophysics::High Energy Astrophysical PhenomenaNuclear Theorychemistry.chemical_elementPolarization (waves)Spectral lineNuclear physicsDeuteriumNeutron generatorchemistryAluminiumPhysics::Accelerator PhysicsNeutronAtomic physicsNuclear ExperimentNuclear Physics
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Neutron yields from thick 12C and 9Be targets irradiated by 50 and 65 MeV deuterons

2001

Abstract Absolute intensities, angular distributions and energy spectra of neutrons emitted from thick 12 C and 9 Be targets irradiated with 50 and 65 MeV deuterons, respectively, have been measured. The neutron spectra were measured by time-of-flight (TOF) technique. The detectors provided continuous coverage from 0° to 60° where a significant angular dependence of emitted neutrons was found. The yield of 0.109(10) neutrons/deuteron from the 9 Be target is a factor of two higher than that from the 12 C target, 0.056(6) neutrons/deuteron. The hardness parameters of the neutron spectra are calculated for the radiation damage studies of the silicon devices.

PhysicsNuclear and High Energy PhysicsSiliconAstrophysics::High Energy Astrophysical PhenomenaNuclear Theorychemistry.chemical_elementSpectral lineNuclear physicschemistryDeuteriumYield (chemistry)Radiation damageNeutronAngular dependenceIrradiationAtomic physicsNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Model-independent fit to Planck and BICEP2 data

2014

Inflation is the leading theory to describe elegantly the initial conditions that led to structure formation in our universe. In this paper, we present a novel phenomenological fit to the Planck, WMAP polarisation (WP) and the BICEP2 datasets using an alternative parameterisation. Instead of starting from inflationary potentials and computing the inflationary observables, we use a phenomenological parameterisation due to Mukhanov, describing inflation by an effective equation-of-state, in terms of the number of e-folds and two phenomenological parameters $\alpha$ and $\beta$. Within such a parametrisation, which captures the different inflationary models in a model-independent way, the valu…

PhysicsNuclear and High Energy PhysicsSpectral indexCosmology and Nongalactic Astrophysics (astro-ph.CO)Structure formationFOS: Physical sciencesSigmaFísicaObservableAstrophysics::Cosmology and Extragalactic AstrophysicsParameter spaceCMB cold spotsymbols.namesakeTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonsymbolsAstronomiaPlanckAstrophysics - Cosmology and Nongalactic Astrophysics
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Circinus X-1 observed with BeppoSAX wide field cameras

1999

Abstract We present a sky image and spectra for various orbital phases of Circinus X-1 observed by B-SAX Wide Field Cameras. We suggest that the spectral shape is dependent on the orbital phase.

PhysicsNuclear and High Energy PhysicsSpectral shape analysisAstrophysics::High Energy Astrophysical Phenomenamedia_common.quotation_subjectPhase (waves)AstronomyAstrophysicsWide fieldAtomic and Molecular Physics and OpticsSpectral lineSkyCircinusmedia_common
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Discrete lineγ-ray spectroscopy in the(50–60)ħspin domain of161,162Er

2000

Very high spin states $(I=50--60\ensuremath{\Elzxh})$ have been observed in the transitional nuclei ${}^{161}\mathrm{Er}$ and ${}^{162}\mathrm{Er}$ using the Euroball $\ensuremath{\gamma}$-ray spectrometer. In ${}^{161}\mathrm{Er},$ three bands are observed well above spin $50\ensuremath{\Elzxh}.$ In the positive parity, positive signature $(+,+\frac{1}{2})$ band a discontinuity in the regular rotational behavior occurs at ${\frac{109}{2}}^{+}$ and a splitting into two branches occurs at ${\frac{97}{2}}^{\ensuremath{-}}$ in the negative parity, positive signature $(\ensuremath{-},+\frac{1}{2})$ band. The $(\ensuremath{-},\ensuremath{-}\frac{1}{2})$ band continues in a regular fashion to ${\…

PhysicsNuclear and High Energy PhysicsSpin statesCondensed matter physicsPairingOblate spheroidNeutronParity (physics)Atomic physicsNuclear ExperimentSpectroscopySpectral linePhysical Review C
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Non-standard interactions with high-energy atmospheric neutrinos at IceCube

2017

Non-standard interactions in the propagation of neutrinos in matter can lead to significant deviations from expectations within the standard neutrino oscillation framework and atmospheric neutrino detectors have been considered to set constraints. However, most previous works have focused on relatively low-energy atmospheric neutrino data. Here, we consider the one-year high-energy through-going muon data in IceCube, which has been already used to search for light sterile neutrinos, to constrain new interactions in the $\mu\tau$-sector. In our analysis we include several systematic uncertainties on both, the atmospheric neutrino flux and on the detector properties, which are accounted for v…

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsMuon010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyHadronFOS: Physical sciencesFlux7. Clean energy01 natural sciencesSpectral line3. Good healthHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesHigh Energy Physics::ExperimentSensitivity (control systems)Neutrino010306 general physicsNeutrino oscillationJournal of High Energy Physics
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The performance of thin layers produced by molecular plating as α-particle sources

2013

Abstract Sources for α-spectroscopy studies were prepared. Constant current density molecular plating was used to produce layers containing the α-particle emitter 147 Sm. Different parameters of the molecular plating process were varied, namely the plating solvent (an isopropanol/isobutanol mixture, pyridine, and N , N -dimethylformamide), the applied deposition time (90, 180, and 360 min), and the surface roughness of the deposition substrate (ca. 10, 20, and 300 nm). Using different analytical techniques, Sm deposition yields, chemical composition of the produced surfaces, surface homogeneity, roughness and morphology were investigated. Alpha spectra were recorded with a Si solid-state de…

PhysicsNuclear and High Energy PhysicsThin layersAnalytical chemistrySurface finishSpectral lineSolventchemistry.chemical_compoundchemistryHomogeneity (physics)Surface roughnessDimethylformamideInstrumentationChemical compositionNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Systematics of nuclear charge distributions in Fe, Co, Ni, Cu, and Zn deduced from muonic x-ray measurements

1976

The results of precise measurements of the energies of the $2{p}_{\frac{3}{2}}\ensuremath{\rightarrow}1{s}_{\frac{1}{2}}$ and $2{p}_{\frac{1}{2}}\ensuremath{\rightarrow}1{s}_{\frac{1}{2}}$ muonic x-ray transitions of $^{54}\mathrm{Fe}$, $^{56}\mathrm{Fe}$, $^{57}\mathrm{Fe}$, $^{58}\mathrm{Fe}$, $^{59}\mathrm{Co}$, $^{58}\mathrm{Ni}$, $^{60}\mathrm{Ni}$, $^{61}\mathrm{Ni}$, $^{62}\mathrm{Ni}$, $^{64}\mathrm{Ni}$, $^{63}\mathrm{Cu}$, $^{65}\mathrm{Cu}$, $^{64}\mathrm{Zn}$, $^{66}\mathrm{Zn}$, $^{68}\mathrm{Zn}$, and $^{70}\mathrm{Zn}$, are reported. Using a highly linear digitally stabilized Ge(Li) spectrometer system, the absolute energies and energy shifts between nuclei were measured with…

PhysicsNuclear and High Energy PhysicsValence (chemistry)ProtonIsotopes of copperCharge densityCharge (physics)Atomic physicsEnergy (signal processing)Effective nuclear chargeSpectral linePhysical Review C
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Lifetime measurement in 195Po

2009

The lifetime of the 17/2+ yrast state in 195Po has been measured using the recoil distance Doppler-shift technique to be $ \tau$ = 43(11) ps. The lifetime was extracted from the singles $ \gamma$ -ray spectra obtained by using the recoil-decay tagging method. The present work provides more information of the coupling schemes, shapes and configuration mixing in neutron-deficient odd-mass Po nuclei.

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)RecoilYrastHadronNuclear fusionAtomic physicsNuclear ExperimentCoupling (probability)Spectral lineMixing (physics)
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