Search results for "signal processing"

showing 10 items of 2451 documents

EUSO-A Space mission searching for Extreme Energy Cosmic Rays and neutrinos

2004

The “Extreme Universe Space Observatory – EUSO” is an international, multi-agency mission, led by ESA, aimed at measuring from a Low Altitude Earth Orbiting Space Platform the flux and investigating the nature and origin of the charged and neutral particles of the Extreme Energy Cosmic Ray (EECR) with energy above the conventional value (E = 5×10 19 eV) of the Greisen Zatsepin and Kuzmin (GZK) effect E GZK = 5×10 19 eV). EUSO will pioneer the observation from Space of EECR-induced Extensive Air Showers (EASs), making measurements of the primary energy, arrival direction and possibly composition of the incoming flux by using a sensitive area and target volume far greater than achievable from…

PhysicsNuclear and High Energy PhysicsPrimary energyAstrophysics::High Energy Astrophysical Phenomenamedia_common.quotation_subjectultra high energy cosmic rays extended air showers international space stationAstrophysics::Instrumentation and Methods for AstrophysicsPlanning target volumeAstronomyFluxCosmic rayAstrophysicsSpace (mathematics)Atomic and Molecular Physics and OpticsUniversePhysics::Space PhysicsNeutrinoEnergy (signal processing)media_common
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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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Proton radioactivity of117La

2001

A new more precise measurement of the ground-state proton decay of ${}^{117}\mathrm{La}$ is presented $[{E}_{p}=806(5) \mathrm{keV},$ ${t}_{1/2,p}=26(3)$ ms]. ${}^{117}\mathrm{La}$ was produced via the $p4n$ fusion-evaporation channel by bombarding a ${}^{64}\mathrm{Zn}$ target with 310 and 295 MeV ${}^{58}\mathrm{Ni}$ beams. The proton decay rate is consistent with emission from a prolate deformed ${3/2}^{+}$ or ${3/2}^{\ensuremath{-}}$ Nilsson state. No evidence is found for a previously reported proton decay from a high spin isomer in ${}^{117}\mathrm{La}.$ An upper limit for the production cross section for proton decay of ${}^{116}\mathrm{La}$ at a bombarding energy of 325 MeV was esta…

PhysicsNuclear and High Energy PhysicsProtonProton decayNuclear TheoryProlate spheroidNuclear physicsPhysics::Accelerator PhysicsProduction (computer science)Proton emissionAtomic physicsNuclear ExperimentEnergy (signal processing)Spin-½Physical 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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Initial-state radiation measurement of thee+e−→π+π−π+π−cross section

2012

We study the process e+e- -> pi+pi-pi+pi-gamma, with a photon emitted from the initial-state electron or positron, using 454.3 fb^-1 of data collected with the BABAR detector at SLAC, corresponding to approximately 260,000 signal events. We use these data to extract the non-radiative sigma(e+e- ->pi+pi-pi+pi-) cross section in the energy range from 0.6 to 4.5 Gev. The total uncertainty of the cross section measurement in the peak region is less than 3%, higher in precision than the corresponding results obtained from energy scan data.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Photon010308 nuclear & particles physicsDetectorElectron01 natural sciencesNuclear physicsCross section (physics)Positron0103 physical sciencesPiHigh Energy Physics::ExperimentAtomic physics010306 general physicsEnergy (signal processing)Physical Review D
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A novel method for obtaining continuous stopping power curves

2001

Abstract A new method has been developed for obtaining continuous stopping power curves in transmission geometry. In the method both the incident energy of the particle and its energy after passing through the sample foil are extracted directly from the semiconductor detector. Full range of energies is measured simultaneously eliminating step-by-step measurements and providing continuous data. A time-of-flight (TOF) spectrometer provides unambiguous matching of relevant particle groups from the run with and without absorber. Suitable energy distribution of incident particles was achieved by choosing the right thickness and tilting angle of a scattering foil. The method is very fast and reli…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Spectrometerbusiness.industrySemiconductor detectorTime of flightOpticsCalibrationStopping power (particle radiation)Specific energybusinessInstrumentationEnergy (signal processing)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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FLUXEN portable equipment for direct X-ray spectra measurements

2004

Abstract The proper use of imaging equipment in radiological units is based on an appropriate knowledge of the physical characteristics of the X-ray beam used. The FLUXEN PROJECT is working on a portable apparatus which, together with dedicated software, is able to perform an exact spectral reconstruction of the radiation produced in diagnostic X-ray tubes. The apparatus characterizes the energy spectrum of radiological tubes and also provides a measurement of the emitted flux. The acquisition system is based on a commercial CZT detector (3×3×2 mm 3 ), produced by AMPTEK, cooled by a Peltier cell, with a high efficiency in the diagnostic X-ray energy range and modified in the shaping electr…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)X-ray spectraX ray spectrographs X rays air kerma CZTbusiness.industryRadiationSignalSpectral lineCZTOpticsSoftwareX-ray spectra; direct measurement; CZTElectronicsdirect measurementbusinessInstrumentationBeam (structure)Energy (signal processing)
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Investigation of the elastic and inelastic scattering of He-3 from Be-9 in the energy range 30-60 MeV

2018

We have measured the differential cross-sections for the elastic as well as inelastic scattering populating the 2.43[Formula: see text]MeV [Formula: see text] excited state in [Formula: see text] using [Formula: see text] beams at energies of 30, 40 and 47[Formula: see text]MeV on a [Formula: see text] target. The experimental results for the elastic scattering were analyzed within the framework of the optical model using the Woods–Saxon and double-folding potentials. The theoretical calculations for the concerned excited states were performed using the coupled-channel method. The optimal deformation parameters for the excited states of [Formula: see text] nucleus were extracted.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)ta114010308 nuclear & particles physicsAstrophysics::Instrumentation and Methods for AstrophysicsGeneral Physics and AstronomyComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)inelastic scatteringInelastic scattering01 natural sciencesdeformation parametersDEUTERONSnuclear physicsExcited state0103 physical sciencesscattering (physics)Computer Science::General Literaturesirontacoupled-channel methodsAtomic physicsElastic scattering010306 general physicsydinfysiikkaEnergy (signal processing)International journal of modern physics e-Nuclear physics
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First observation of excited states inPo192

1996

\ensuremath{\gamma} rays following the $^{160}\mathrm{Dy}$${(}^{36}$Ar,4n${)}^{192}$Po reaction have been identified by employing a high-transmission gas-filled separator in recoil decay tagging measurements. The deduced level scheme reveals a flattening of the energy systematics, when going towards the neutron midshell indicating that the deformed intruder structures have become yrast. \textcopyright{} 1996 The American Physical Society.

PhysicsNuclear and High Energy PhysicsRecoilExcited stateYrastNeutronAtomic physicsEnergy (signal processing)FlatteningPhysical Review C
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Shape coexistence in183Tl

2001

Prompt and delayed $\ensuremath{\gamma}$ rays originating from the neutron deficient nucleus ${}^{183}\mathrm{Tl}$ have been observed using the recoil-decay tagging and recoil gating techniques. The band-head energy of the prolate $\ensuremath{\pi}{i}_{13/2}$ yrast band has been determined. The yrast structure has also been confirmed up to the ${(33/2}^{+})$ state. In addition, a candidate for the ${(11/2}^{\ensuremath{-}})$ level based on the $\ensuremath{\pi}{(h}_{11/2}{)}^{\ensuremath{-}1}$ configuration has been observed.

PhysicsNuclear and High Energy PhysicsRecoilYrastNeutronProlate spheroidAtomic physicsEnergy (signal processing)Physical Review C
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