Search results for "decay"

showing 10 items of 2087 documents

Direct measurements of the lifetime of medium-heavy hypernuclei

2018

Abstract The lifetime of a Λ particle embedded in a nucleus (hypernucleus) decreases from that of free Λ decay mainly due to the opening of the Λ N → N N weak decay channel. However, it is generally believed that the lifetime of a hypernucleus attains a constant value (saturation) for medium to heavy hypernuclear masses, yet this hypothesis has been difficult to verify. This paper presents a direct measurement of the lifetime of medium-heavy hypernuclei that were hyper-fragments produced by fission or break-up from heavy hypernuclei initially produced with a 2.34 GeV photon-beam incident on thin Fe, Cu, Ag, and Bi target foils. For each event, fragments were detected in coincident pairs by …

PhysicsNuclear and High Energy PhysicsRange (particle radiation)010308 nuclear & particles physicsFissionHypernuclei ; Lifetime ; Fragment ; Hyper-fragment ; Weak decayWeak interactionHypernucleus01 natural sciencesNuclear physicsCoincident0103 physical sciencesParticle010306 general physicsSaturation (chemistry)Event (particle physics)Nuclear Physics A
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Search for a new light gauge boson in decays of π0 and η

1994

Abstract We have searched for new light gauge bosons produced in π 0 and η decays by studying the kinematically well-constrained reactions p p→π 0 π 0 π 0 and p p→π 0 π 0 η , where one π 0 or the η decays through the emission of a single photon recoiling against a missing state X (where X is a long-lived weakly interacting particle or X →ν ν ). No signal has been observed and branching ratio upper limits of 6 × 10 −5 at 90% C.L. have been obtained for masses of the gauge boson lying between ∼65 MeV and 125 MeV ( π 0 decay), and 6 × 10 −5 at 90% C.L. for X masses between ∼200 MeV and 525 MeV (η decay). The π 0 -decay limit represents a factor of 4 to 8 improvement when compared to the existi…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Gauge bosonParticle physicsPhoton[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]010308 nuclear & particles physicsBranching fractionElementary particle01 natural sciencesUpper and lower boundsNuclear physicsParticle decayPhoton emission0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsParticle Physics - ExperimentPhysics Letters B
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Conversion electron and beta decay spectroscopy at SHIP

2004

Abstract Novel methods for internal conversion electron and β -decay spectroscopy at the focal plane of a recoil separator are discussed. As an example the experimental data collected at the focal plane of the velocity filter SHIP (GSI, Darmstadt) are presented and compared with the results of the GEANT Monte Carlo simulations. It is shown that the simultaneous detection of conversion electrons, γ -rays and X-rays is possible, which significantly broadens the range of applications of this and similar systems.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Monte Carlo methodElectronBeta decayNuclear physicsInternal conversionCardinal pointAlpha decayAtomic physicsNuclear ExperimentSpectroscopyInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A superformula for neutrinoless double beta decay II: The short range part

2000

A general Lorentz-invariant parameterization for the short-range part of the 0vBB decay rate is derived. Combined with the long range part already published this general parameterization in terms of effective B-L violating couplings allows one to extract the 0vBB limits on arbitrary lepton number violating theories.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)SuperformulaDouble beta decayHigh Energy Physics::Experiment
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Search for heavy neutrinos in K + → μ + ν μ decays

2017

The NA62 experiment recorded a large sample of K+→μ+νμ decays in 2007. A peak search has been performed in the reconstructed missing mass spectrum. In the absence of a signal, limits in the range 2×10−6 to 10−5 have been set on the squared mixing matrix element |Uμ4|2 between muon and heavy neutrino states, for heavy neutrino masses in the range 300–375 MeV/ c2 . The result extends the range of masses for which upper limits have been set on the value of |Uμ4|2 in previous production search experiments.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsMuon010308 nuclear & particles physicsPhysics beyond the Standard ModelHeavy neutrinoNA62 experiment01 natural scienceslcsh:QC1-999Heavy neutrinos; Kaon decays; Nuclear and High Energy PhysicsNuclear physicsKaon decayHeavy neutrinos0103 physical sciencesMass spectrumKaon decaysNeutrinoHeavy neutrino010306 general physicslcsh:PhysicsMixing (physics)
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Identification of excited states in doubly odd63140Eu77by recoil-isomer tagging

2002

The 36Ar + 107Ag fusion-evapn. reaction was used to search for isomeric states in the N = 77 isotope 140Eu near the proton-drip line. The recoiling nuclei were implanted into a Si detector, at the focal plane of a gas-filled separator, where prompt and delayed g-ray transitions were correlated across isomeric states using recoil-isomer tagging. The feeding and decay of a new 299(3) ns isomeric state was established. This measurement represents the first observation of excited high-spin states in 140Eu. The behavior of the new states above the isomer is discussed in terms of theor. calcns. based upon the cranked-shell model and upon the exptl. systematics of other N = 77 isotones. Within thi…

PhysicsNuclear and High Energy PhysicsRecoilExcited stateHadronNuclear structureGamma rayFermionAtomic physicsNucleonRadioactive decayPhysical Review C
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α-decay properties ofPb181

1996

The isotope {sup 181}Pb was produced in {sup 92}Mo bombardments of {sup 90}Zr and, together with other reaction products, was passed through a recoil mass separator and implanted in a double-sided silicon strip detector for {alpha}-particle assay. The half-life and energy of the main {sup 181}Pb {alpha} transition were determined to be 45 (20) ms and 7065 (20) keV, respectively. This {sup 181}Pb {ital E}{sub {alpha}} agrees with one previously measured value [7044 (15) keV], but not with the one [7211 (10) keV] used as input to the 1993 Atomic Mass Evaluation. The 6180-keV {alpha} transition assigned to {sup 181}Tl by Bolshakov {ital et} {ital al}. was observed, but the 6566-keV {alpha} par…

PhysicsNuclear and High Energy PhysicsRecoilSiliconchemistryIsotopeAnalytical chemistrychemistry.chemical_elementAlpha particleAlpha decayAtomic massPhysical Review C
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Nuclear magnetic resonance at millitesla fields using a zero-field spectrometer

2016

We describe new analytical capabilities for nuclear magnetic resonance (NMR) experiments in which signal detection is performed with chemical resolution (via spin-spin J couplings) in the zero to ultra-low magnetic field region, below 1μT. Using magnetic fields in the 100μT to 1mT range, we demonstrate the implementation of conventional NMR pulse sequences with spin-species selectivity.

PhysicsNuclear and High Energy PhysicsRelaxometryZero field NMRBiophysicsMagnetic resonance force microscopy010402 general chemistryCondensed Matter Physics01 natural sciencesBiochemistry0104 chemical sciencesFree induction decayNuclear magnetic resonanceSolid-state nuclear magnetic resonance0103 physical sciencesSpin echoCondensed Matter::Strongly Correlated Electrons010306 general physicsNuclear magnetic resonance decouplingEarth's field NMRJournal of Magnetic Resonance
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Beta-decay of 56Cu

1998

Beta-decay studies of proton-rich isotopes near the doubly closed-shell nucleus 56Ni are of interest as (i) nuclei with a few nucleons outside a doubly-magic core are expected to represent comparatively simple configurations and thus be useful for testing nuclear shell-model predictions, and (ii) the large decay-energy window guarantees that a sizeable fraction of the strength of the allowed β-decay can be reached by the experiment. Moreover, nuclear structure properties of proton-rich N ~ Z isotopes are of astrophysical interest, e.g., concerning the EC cooling of supernovae and the astrophysical rp-process.

PhysicsNuclear and High Energy PhysicsSIMPLE (dark matter experiment)IsotopeNuclear TheorySHELL modelNuclear structureBeta decayNuclear physicsSupernovamedicine.anatomical_structuremedicineNuclear ExperimentNucleonNucleusPhysics Letters B
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Observation of a dramatic hindrance of the nuclear decay of isomeric states for fully ionized atoms

2003

Abstract The half-lives of isomeric states of fully ionized 144Tb, 149Dy and 151Er have been measured. These nuclides were produced via fragmentation of about 900 MeV/u 209Bi projectiles, separated in flight with the fragment separator (FRS) and stored in the cooler ring (ESR). The decay times of the cooled fragments have been measured with time-resolved Schottky spectrometry. We observed for the first time drastic increases of the half-lives of bare isomers by factors of up to 30 compared to their neutral counterparts. This is due to the exclusion of the strong internal conversion and electron-capture channels in the radioactive decay of these bare nuclei. The experimental results are in g…

PhysicsNuclear and High Energy PhysicsSchottky diodeHighly-charged ionsRing (chemistry)Mass spectrometryHalf-livesStorage ringsInternal conversionFragmentation (mass spectrometry)IonizationNuclideAtomic physicsNuclear ExperimentExotic nucleiRadioactive decayPhysics Letters B
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