Search results for "signal processing"

showing 10 items of 2451 documents

Total-variation-based methods for gravitational wave denoising

2014

We describe new methods for denoising and detection of gravitational waves embedded in additive Gaussian noise. The methods are based on Total Variation denoising algorithms. These algorithms, which do not need any a priori information about the signals, have been originally developed and fully tested in the context of image processing. To illustrate the capabilities of our methods we apply them to two different types of numerically-simulated gravitational wave signals, namely bursts produced from the core collapse of rotating stars and waveforms from binary black hole mergers. We explore the parameter space of the methods to find the set of values best suited for denoising gravitational wa…

PhysicsNuclear and High Energy PhysicsGravitational waveNoise (signal processing)Noise reductionFOS: Physical sciencesImage processingGeneral Relativity and Quantum Cosmology (gr-qc)Total variation denoisingGeneral Relativity and Quantum Cosmologysymbols.namesakeClassical mechanicsBinary black holeGaussian noisesymbolsWaveformAstrophysics - Instrumentation and Methods for AstrophysicsInstrumentation and Methods for Astrophysics (astro-ph.IM)AlgorithmPhysical Review D
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Rotational bands in99Sr

1984

The β-decay of 59 ms99Rb has been studied at OSTIS. As is confirmed by RPA calculations with Nilsson model wave functions, the lowest energy levels in99Sr are consistent with rotational bands built on the [411 3/2], [413 5/2] and [422 3/2] Nilsson neutron configurations at 0, 423 and 1071 keV, respectively. All three bands have similar values of the inertial parameter ħ2/2θ indicating a nearly rigid rotor.

PhysicsNuclear and High Energy PhysicsInertial frame of referenceNuclear fusionNeutronRigid rotorAtomic physicsWave functionEnergy (signal processing)Zeitschrift f�r Physik A Atoms and Nuclei
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Decay studies ofAu170,171,Hg171–173, andTl176

2004

The $^{170,171}\mathrm{Au}$ isotopes were produced in the fusion-evaporation reaction of a $^{78}\mathrm{Kr}$ ion beam with a $^{96}\mathrm{Ru}$ target. For $^{170}\mathrm{Au}$ the proton and $\ensuremath{\alpha}$ emission from the ground state were observed for the first time and the decay of the isomeric state was measured with improved accuracy. In addition, the decay of $^{171}\mathrm{Au}$ was measured with high statistics. A new $\ensuremath{\alpha}$-emitting nucleus $^{171}\mathrm{Hg}$ and the previously known $^{172}\mathrm{Hg}$ and $^{167,168,169,170}\mathrm{Pt}$ isotopes were also studied. The ground-state proton emission was identified for a new proton emitter $^{176}\mathrm{Tl}$ …

PhysicsNuclear and High Energy PhysicsIon beamProtonAlpha decayProton emissionAtomic physicsNuclear ExperimentGround stateRecoil separatorEnergy (signal processing)IonPhysical Review C
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High-resolution study of Gamow-Teller transitions in the47Ti(3He,t)47V reaction

2013

In this work we have studied ${T}_{z}=+2\ensuremath{\rightarrow}+1$, Gamow-Teller (GT) transitions in the $^{48}\mathrm{Ti}(^{3}\mathrm{He},t)^{48}\mathrm{V}$ charge-exchange reaction at 140 MeV/nucleon and ${0}^{\ensuremath{\circ}}$ at the Research Center for Nuclear Physics, Osaka. From the high-resolution facility, consisting of a high-dispersion beamline and the Grand Raiden spectrometer, the spectrum had an energy resolution of 21 keV, among the best achieved. Individual GT transitions were observed and GT strength was derived for each state populated up to an excitation energy of 12 MeV. The total sum of the $B$(GT) strength observed in discrete states was 4.0, which is 33% of the sum…

PhysicsNuclear and High Energy PhysicsIsospinSHELL modelHigh resolutionAtomic physicsNuclear ExperimentNucleonEnergy (signal processing)ExcitationPhysical Review C
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Measurement of the two neutrino double beta decay half-life of Zr-96 with the NEMO-3 detector

2010

Using 9.4 g of Zr-96 and 1221 days of data from the NEMO-3 detector corresponding to 0.031 kg yr, the obtained 2vbb decay half-life measurement is [2.35 +/- 0.14(stat) +/- 0.16(syst)] x 10^19 yr. Different characteristics of the final state electrons have been studied, such as the energy sum, individual electron energy, and angular distribution. The 2v nuclear matrix element is extracted using the measured 2vbb half-life and is 0.049 +/- 0.002. Constraints on 0vbb decay have also been set.

PhysicsNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsDetectorFOS: Physical sciencesHalf-lifeElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesNuclear physicsRadioactivityAngular distributionDouble beta decay0103 physical sciencesNuclear Experiment (nucl-ex)Neutrino010306 general physicsNuclear ExperimentEnergy (signal processing)
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Radioactivity of neutron-rich oxygen fluorine and neon isotopes

1999

The $\ensuremath{\gamma}$ radiation and neutrons emitted following the $\ensuremath{\beta}$ decays of ${}^{24}\mathrm{O},$ ${}^{25--27}\mathrm{F},$ and ${}^{28\ensuremath{-}30}\mathrm{Ne}$ have been measured. The nuclides were produced in the quasifragmentation of a 2.8 GeV ${}^{36}\mathrm{S}$ beam, separated in-flight and identified through time-of-flight and energy-loss measurements. The ions were stopped in a silicon detector telescope, which was used to detect the $\ensuremath{\beta}$ particles emitted in their subsequent radioactive decay. The coincident $\ensuremath{\gamma}$ rays were measured using four large volume germanium detectors mounted close to the implantation point and the …

PhysicsNuclear and High Energy PhysicsIsotopes of germanium010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaGamma ray[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsInternal conversionIsotopes of neon13. Climate action0103 physical sciencesBeta particleIsotopes of zirconiumNuclear Experiment010306 general physicsRadioactive decayEnergy (signal processing)
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QECvalues of the superallowedβemittersC10,Ar34,Ca38, andV46

2011

The ${Q}_{\mathrm{EC}}$ values of the superallowed ${\ensuremath{\beta}}^{+}$ emitters $^{10}\mathrm{C}$, $^{34}\mathrm{Ar}$, $^{38}\mathrm{Ca}$, and $^{46}\mathrm{V}$ have been measured with the JYFLTRAP Penning-trap mass spectrometer to be 3648.12(8), 6061.83(8), 6612.12(7), and 7052.44(10) keV, respectively. All four values are substantially improved in precision over previous results. Of the well-known superallowed emitters, only $^{14}\mathrm{O}$ has yet to have had its ${Q}_{\mathrm{EC}}$ value measured with a Penning trap.

PhysicsNuclear and High Energy PhysicsLight nucleusQ valueIsotopes of vanadiumAtomic physicsNuclear ExperimentPenning trapEnergy (signal processing)Physical Review C
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Kπ=8−isomers andKπ=2−octupole vibrations inN=150shell-stabilized isotones

2008

Isomers have been populated in {sup 246}Cm and {sup 252}No with quantum numbers K{sup {pi}}=8{sup -}, which decay through K{sup {pi}}=2{sup -} rotational bands built on octupole vibrational states. For N=150 isotones with (even) atomic number Z=94-102, the K{sup {pi}}=8{sup -} and 2{sup -} states have remarkably stable energies, indicating neutron excitations. An exception is a singular minimum in the 2{sup -} energy at Z=98, due to the additional role of proton configurations. The nearly constant energies, in isotones spanning an 18% increase in Coulomb energy near the Coulomb limit, provide a test for theory. The two-quasiparticle K{sup {pi}}=8{sup -} energies are described with single-pa…

PhysicsNuclear and High Energy PhysicsMean field theoryProtonQuasiparticleWoods–Saxon potentialAtomic numberAtomic physicsQuantum numberRandom phase approximationEnergy (signal processing)Physical Review C
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Pulse shape analysis of signals from BaF2 and CeF3 scintillators for neutron capture experiments

2006

The scope of this work is to study the characteristics of BaF2 and CeF3 signals using fast digitizers, which allow the sampling of the signal at very high frequencies and the application of the fitting method for analysis of the recorded pulses. By this procedure particle identification and the reconstruction of pile-up events can be improved, while maintaining the energy and time-of-flight resolution as compared to traditional methods. The reliability of the technique and problems connected with data acquisition are discussed with respect to accurate measurements of neutron capture cross-sections.

PhysicsNuclear and High Energy PhysicsNeutron captureData acquisitionSampling (signal processing)AcousticsScintillatorInstrumentationSignalReliability (statistics)Particle identificationEnergy (signal processing)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Dependence of direct neutron capture on nuclear-structure models

1998

The prediction of cross sections for nuclei far off stability is crucial in the field of nuclear astrophysics. We calculate direct neutron capture on the even-even isotopes $^{124-145}$Sn and $^{208-238}$Pb with energy levels, masses, and nuclear density distributions taken from different nuclear-structure models. The utilized structure models are a Hartree-Fock-Bogoliubov model, a relativistic mean field theory, and a macroscopic-microscopic model based on the finite-range droplet model and a folded-Yukawa single-particle potential. Due to the differences in the resulting neutron separation and level energies, the investigated models yield capture cross sections sometimes differing by orde…

PhysicsNuclear and High Energy PhysicsNuclear TheoryAstrophysics (astro-ph)Nuclear TheoryNuclear structureFOS: Physical sciencesAstrophysicsNuclear Theory (nucl-th)Nuclear physicsNeutron captureMean field theoryNuclear astrophysicsr-processNeutronAtomic physicsNuclear densityEnergy (signal processing)
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