Search results for "Spectral"

showing 10 items of 3116 documents

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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Ground-state spin of 59Mn

2001

Beta decay of $^{59}$Mn has been studied at PSB-ISOLDE, CERN. The intense and pure Mn beam was produced using the Resonance Ionization Laser Ion Source (RILIS). Based on the measured $\beta$-decay rates the ground-state spin and parity are proposed to be $J^{\pi}$ = 5/2$^{-}$. This result is consistent with the systematic trend of the odd-A Mn nuclei and extends the systematics one step further towards the neutron drip line.

PhysicsNuclear and High Energy Physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Hadron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Ion sourceSpectral lineExcited stateNuclear fusionNuclear drip lineAtomic physicsNuclear ExperimentGround stateParticle Physics - ExperimentRadioactive decayThe European Physical Journal A
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Present status of the caloric curve of nuclei

1998

Abstract Spectator decay was studied for the system Au + Au at an energy of 1000 A·MeV and the decay of the interaction region at energies between 50 and 200 A·MeV. In both cases temperatures were derived from several double-ratios of neighboring isotopes and from the population of excited states in 5 Li and 4 He. Agreement was found among the different isotope temperatures and also among the two excited state temperatures. The comparison of isotope and excited state temperatures, however, reveals large differences, which cannot be explained by feeding corrections. At incident energies between 600 and 1000 A·MeV the energy spectra of fragments and also neutrons of the decaying projectile sp…

PhysicsNuclear and High Energy Physicseducation.field_of_studyIsotopeProjectileNuclear TheoryPopulationSpectral lineCaloric curveExcited stateIncident energyNeutronAtomic physicsNuclear ExperimenteducationNuclear Physics A
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Properties of isomeric states and the ?d 3/2-vi 13/2 multiplet in194Au

1977

The level structure of194Au has been studied by observing prompt and delayedγ-rays following194Pt(p,n) and195Pt(p,2n) reactions. The conversion electron andγ-ray spectra from the decay of the 0.42s (10−) and 0.60s (5+) isomers at 476 keV and 107.4 keV, respectively, have been measured using the He-jet method. The half-lives of the 6+ (278.2 keV, 1.1±0.4 ns), 7+ (224.6 keV, 2.6±0.2 ns) and 8+ (406.8 keV, 2.9±0.4 ns) members of theπd3/2-vi13/2 multiplet have been obtained from the time distributions between cyclotron beam pulses andγ-rays depopulating these levels. A calculation made assuming a pure two-particle configuration for the multiplet predicts very well theB(E2) values for the transi…

PhysicsNuclear and High Energy PhysicslawCyclotronLevel structureNuclear fusionElementary particleElectronAtomic physicsMultipletBeam (structure)Spectral linelaw.inventionZeitschrift f�r Physik A Atoms and Nuclei
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