0000000000043177

AUTHOR

C. Petitjean

showing 6 related works from this author

Ordinary muon capture studies for the matrix elements in ββ decay

2018

Precise measurement of $\gamma$-rays following ordinary (non-radiative) capture of negative muons by natural Se, Kr, Cd and Sm, as well as isotopically enriched $^{48}$Ti, $^{76}$Se, $^{82}$Kr, $^{106}$Cd and $^{150}$Sm targets was performed by means of HPGe detectors. Energy and time distributions were investigated and total life time of negative muon in different isotopes was deduced. Detailed analysis of $\gamma$-lines intensity allows to extract relative yield of several daughter nuclei and partial rates of ($\mu$,$\nu$) capture to numerous excited levels of the $^{48}$Sc, $^{76}$As, $^{82}$Br, $^{106}$Ag and $^{150}$Tc isotopes which are considered to be virtual states of an intermedia…

PhysicsMuonta114010308 nuclear & particles physicsenergy levels and level densitieschemistry.chemical_elementdouble beta decayGermaniumhiukkasfysiikka01 natural sciencesnuclear structure and decaysMuon captureelectron and muon captureMatrix (mathematics)chemistryExcited state0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsydinfysiikkaNuclear ExperimentEnergy (signal processing)Intensity (heat transfer)Physical Review C
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The Study of Prompt and Delayed Muon Induced Fission; II. Mean life times of negative muons bound to 237Np, 242Pu and 244Pu

1988

The mean life times of negative muons bound to actinide nuclei have been measured by detecting the time difference between a stopped muon and the arrival of fragments from delayed fission after muon capture. The deduced capture rates c are 1.392(4)·107/s for237Np, 1.290(7)·107/s for242Pu and 1.240(7)·107/s for244Pu. The results are compared with published data for the fission and the neutron decay channels and for the electron decay of the bound muon. Including a former measurement of c for239Pu, an isotopic dependence of the muon capture rates in the Pu isotopes is clearly observed.

Nuclear reactionPhysicsNuclear and High Energy PhysicsMuonIsotopeFissionPhysics::Instrumentation and DetectorsNuclear TheoryElectronMuon captureNuclear physicsNuclear fusionNeutronHigh Energy Physics::ExperimentNuclear Experiment
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Measurement of trace impurities in ultra pure hydrogen and deuterium at the parts-per-billion level using gas chromatography

2018

Abstract A series of muon experiments at the Paul Scherrer Institute in Switzerland deploy ultra-pure hydrogen active targets. A new gas impurity analysis technique was developed, based on conventional gas chromatography, with the capability to measure part-per-billion (ppb) traces of nitrogen and oxygen in hydrogen and deuterium. Key ingredients are a cryogenic admixture accumulation, a directly connected sampling system and a dedicated calibration setup. The dependence of the measured concentration on the sample volume was investigated, confirming that all impurities from the sample gas are collected in the accumulation column and measured with the gas chromatograph. The system was calibr…

PhysicsNuclear and High Energy PhysicsHydrogenAnalytical chemistryParts-per notationchemistry.chemical_element02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesNitrogenDilutionchemistryDeuteriumImpurity0103 physical sciencesGas chromatography010306 general physics0210 nano-technologyInstrumentationGas chromatography ion detectorNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The probability of prompt and delayed fission of muonic237Np

1991

Fission fragments from the reaction237Np(μ−,γ,f) have been measured in coincidence with muonic X-rays. The efficiency of the fission fragment detector is determined from (μ−,γ,f)-data of the same experiment. The total fission probability perμ-stopPt has been measured as well as the fission probabilities Pf of the non-radiative muonic (3d→1s)- and (2p→1s)-transitions; the latter has been divided into two parts leading to different mean excitation energiesE:P t =(54±17)%,P f (3d→1s)=(41±21)%,P f (2p→1s,E=6.218 MeV)=(61±19)%, andP f (2p→1s,E=6.525 MeV)=(57±18)%. The influence of the muon on the fission barrier is discussed. The fission probability after muon capture is compared with a calculat…

PhysicsNuclear physicsNuclear reactionNuclear and High Energy PhysicsMuonCluster decayFissionBranching fractionNuclear fusionElementary particleAtomic physicsMuon captureZeitschrift für Physik A Hadrons and Nuclei
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Ordinary muon capture studies for the matrix elements in ββ decay

2019

High-purity germanium (HPGe) detectors were used to make a precise measurement of the γ-ray spectrum produced following ordinary (nonradiative) capture of negative muons by natural Se, Kr, Cd, and Sm. The measurement was repeated for isotopically enriched 48Ti, 76Se, 82Kr, 106Cd, and 150Smtargets. By investigating energy and time distributions, the lifetime of negative muons in the different isotopes was deduced. A detailed analysis of the intensity of the γ lines enabled the extraction of the relative yields of several daughter nuclei. The partial rates of (μ−,ν) capture to numerous excited levels of the 48Sc, 76As, 82Br, 106Ag, and 150Tc isotopes (considered to be virtual states of the in…

electron and muon captureenergy levels and level densitiesdouble beta decayhiukkasfysiikkaydinfysiikkanuclear structure and decays
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Doppler-broadening of gamma rays following muon capture: search for scalar coupling

2002

Abstract A precision measurement of the 277 keV γ ray produced by capturing muons in gaseous oxygen was performed using high-resolution HPGe detectors. The Doppler-broadened shape of this line is sensitive to the possible admixture into muon capture of genuine scalar interaction. This experiment complements, in the muon sector, in principle, similar ones undertaken recently in nuclear β decay. Using a procedure discussed in earlier papers, a fit to the experimental line-shape allowed us to obtain for the recoil–gamma correlation coefficient the value of a 1 2 =0.096±0.041 (95% CL). The available evaluations of the contributing nuclear matrix elements, performed in the impulse approximation …

Nuclear reactionPhysicsNuclear and High Energy PhysicsMuonCorrelation coefficient[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]010308 nuclear & particles physicsGamma ray[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Impulse (physics)01 natural sciencesMuon captureNuclear physicsPseudoscalar0103 physical sciences010306 general physicsDoppler broadeningNuclear Physics A
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