0000000000083272

AUTHOR

G. Canchel

showing 15 related works from this author

Precision measurement of the half-life and the decay branches of 62Ga

2005

In an experiment performed at the Accelerator Laboratory of the University of Jyvaskyla, the beta-decay half-life of 62Ga has been studied with high precision using the IGISOL technique. A half-life of T1/2 = 116.09(17)ms was measured. Using beta-gamma coincidences, the gamma intensity of the 954keV transition and an upper limit of the beta-decay feeding of the 0+_2 state have been extracted. The present experimental results are compared to previous measurements and their impact on our understanding of the weak interaction is discussed.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsIGISOL TECHNIQUEHalf-lifeFOS: Physical sciencesState (functional analysis)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Weak interaction01 natural sciencesIntensity (physics)Nuclear physics23.40.-s $\beta$ decay ; double $\beta$ decay ; electron and muon capture - 21.10. Tg Lifetimes - 27.50.+e 59 < A < 890103 physical sciencesLimit (mathematics)Nuclear Experiment (nucl-ex)010306 general physicsNuclear Experiment
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Production of refractory elements close to the Z=N line using the ion-guide technique

1998

Production of neutron-deficient isotopes of refractory elements in the A = 80-88 region was studied using the IGISOL technique and the 165 MeV Si-32 + Ni-nat reaction. Radioactive isotopes of Y through Mo could be produced up to the M-T = + 1 line. New information on the decay of the A = 82 and 85 nuclei, including a more detailed decay scheme and more accurate half-life for Y-82, was obtained. (C) 1998 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsIsotopes of germaniumAnalytical chemistryONLINE[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesY-81Isotopes of oxygenNuclear physicsIsotopes of protactinium0103 physical sciencesNEUTRON-DEFICIENT ISOTOPES010306 general physicsInstrumentationIsotopes of europiumPhysicsDecay schemeIsotope010308 nuclear & particles physicsRefractory metalsIGISOL TECHNIQUEheavy-ion fusion-evaporation reactionsBeta decayrefractory elementsbeta decayDECAY
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A new isomer in 125La

1999

Levels in 125La have been studied via β+/EC decay of on-line mass-separated 125Ce using the HIGISOL technique. A new (390 ± 40) ms isomer is definitely attributed to 125La by conversion electron measurements of the 107 keV E3 isomeric transition.

Nuclear physicsPhysicsNuclear and High Energy PhysicsHadronNuclear fusionElectronAtomic physicsNuclear isomerThe European Physical Journal A
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Erratum to “Beta decay half-lives of neutron rich Ti–Co isotopes around N=40” [Nucl. Phys. A 660 (1999) 3–19]

2000

Abstract The neutron-rich 57−59 Ti, 59−62 V, 61−64 Cr, 63−66 Mn, 65−68 Fe, 67−70 Co have been produced at GANIL via interactions of a 60.4 MeV/u 86 Kr 34+ with a 58 Ni target. They have been separated by the doubly achromatic spectrometer LISE3. Beta-decay half-lives have been determined for all produced nuclei, and subsequent γ -rays have been observed for the most efficiently produced nuclei. The measured half-lives of vanadium and chromium isotopes are compared to QRPA calculations using ground states deformations from the FRDM or ETFSI models. In an astrophysical context, the short half-lives of 58 Ti and 64 Cr indicate that these nuclei are potential r-process progenitors, after β -dec…

Nuclear reactionPhysicsNuclear and High Energy PhysicsIsotopes of chromium010308 nuclear & particles physicsContext (language use)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesBeta decayIsotopes of vanadium0103 physical sciencesNeutronAtomic physics010306 general physicsIsotopes of cobaltRadioactive decayNuclear Physics A
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The $\beta$-delayed one- and two-proton emission of $^{27}$S

2001

In an experiment performed at the GANIL LISE3 facility, radioactive 27S isotopes have been produced by projectile fragmentation of a 95 AMeV 36Ar primary beam. After selection by means of the LISE3 separator, the isotope of interest was implanted in a silicon-detector telescope where its half-life ( T 1/2 = 15.5(15) ms) and its main decay branches were measured.

PhysicsNuclear and High Energy PhysicsDecay schemeIsotopes of germanium010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBeta-decay stable isobarsNuclear physics0103 physical sciencesBeta particleIsotopes of zirconiumIsotopes of siliconProton emission010306 general physicsRadioactive decay
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$Q$-value of the superallowed $\beta$ decay of 62Ga

2006

Masses of the radioactive isotopes 62Ga, 62Zn and 62Cu have been measured at the JYFLTRAP facility with a relative precision of better than 18 ppb. A Q_EC value of (9181.07 +- 0.54) keV for the superallowed decay of 62Ga is obtained from the measured cyclotron frequency ratios of 62Ga-62Zn, 62Ga-62Ni and 62Zn-62Ni ions. The resulting Ft-value supports the validity of the conserved vector current hypothesis (CVC). The mass excess values measured were (-51986.5 +-1.0) keV for 62Ga, (-61167.9 +- 0.9) keV for 62Zn and (-62787.2 +- 0.9) keV for 62Cu.

Nuclear and High Energy PhysicsMass excessQ valuePenning trapCyclotronFOS: Physical sciences27.50.+e; 23.40.-s; 24.80.+g; 21.10.Dr[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyIonlaw.inventionNuclear physicslawDouble beta decayFt value0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsRadionuclide010308 nuclear & particles physicsBeta decayQ-valueAtomic massAtomic mass
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Investigation of a gas catcher/ion guide system at the Warsaw cyclotron

2003

NESTER ACC; The properties of a gas-catcher/ion guide system, connected to a mass separator at the Heavy Ion Laboratory of Warsaw University, were investigated by using the α-decay recoil products 219Rn and 215Po, obtained from a 223Ra source. The “plasma effect” was studied by using a 14N beam with intensities ranging from 7 to 64 particledot operatornA, which correspond to power depositions between 1.6 dot operator 1016 and 7.2 dot operator 1017 eV/s for helium pressures of 75 and 380 hPa, respectively.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsCyclotronSeparator (oil production)chemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesIonlaw.inventionRecoilchemistrylaw0103 physical sciencesHeavy ionPlasma effectAtomic physics010306 general physicsHelium
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Studying exotic nuclides close to the N = Z line at the HIGISOL facility

2003

The ion guide [1, 2] for heavy-ion fusion-evaporation reactions (HIGISOL) which was developed by Beraud et al. [3] has been implemented at the IGISOL facility in Jyvaskyla [4]. This system was modified over the past 5 years. Figure 1 shows the present set-up. The HIGISOL takes advantage of the different angular distributions of primary beam and reaction products: the primary beam is stopped in front of the stopping chamber and the reaction products enter the stopping chamber through a thin foil passing the beam stop. This so called “shadow” method removes the plasma effect since the primary beam is not ionising the stopping gas. In order to improve ion optical properties, mainly to reduce t…

PhysicsNuclear physicsDc voltageIon beamPlasma effectSkimmer (machine)NuclideBeam (structure)Line (formation)Ion
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Beta-decay half-lives at the N = 28 shell closure

2004

Abstract Measurements of the beta-decay half-lives of neutron-rich nuclei (MgAr) in the vicinity of the N =28 shell closure are reported. Some 22 half-lives have been determined, 12 of which for the first time. Particular emphasis is placed on the results for the Si isotopes, the half-lives of which have been extended from N =25 to 28. Comparison with QRPA calculations suggests that 42 Si is strongly deformed. This is discussed in the light of a possible weakening of the spin–orbit potential.

PhysicsNuclear and High Energy Physics21.10.Tg; 23.40.-s; 27.30.+t; 27.30.+zIsotope010308 nuclear & particles physicsNuclear TheoryShell (structure)Closure (topology)Beta decayLifetimes[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBeta decay0103 physical sciencesNeutronIsotopes of siliconAtomic physics010306 general physicsNuclear Experiment
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Beta decay half-lives of neutron rich Ti–Co isotopes around

1999

Abstract The neutron-rich 57 – 59 Ti, 59 – 62 V, 61 – 64 Cr, 63 – 66 Mn, 65 – 68 Fe, 67 – 70 Co have been produced at GANIL via interactions of a 60.4 MeV/u 86 Kr 34+ with a 58 Ni target. They have been separated by the doubly achromatic spectrometer LISE3. Beta-decay half-lives have been determined for all produced nuclei, and subsequent γ -rays have been observed for the most efficiently produced nuclei. The measured half-lives of vanadium and chromium isotopes are compared to QRPA calculations using ground states deformations from the FRDM or ETFSI models. In an astrophysical context, the short half-lives of 58 Ti and 64 Cr indicate that these nuclei are potential r-process progenitors, …

PhysicsNuclear reactionNuclear and High Energy PhysicsIsotopes of chromiumIsotopeIsotopes of vanadiumAnalytical chemistryNeutronContext (language use)Atomic physicsBeta decayRadioactive decayNuclear Physics A
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Status of HIGISOL a new version equipped with SPIG and electric field guidance

2001

A new HIGISOL chamber devoted to the study of short-lived products from heavy-ion-induced fusion-evaporation reactions is proposed. It enables, via the extraction of ions by means of a SPIG (SextuPole rf Ion Guide), to improve the mass resolving power by a factor 2.5 compared to the previous system using a skimmer-ring assembly. The gas cell was also equiped with an electric field for faster transportation of recoiling ions to the nozzle where they are ejected with the gas jet. The first results obtained both with a radioactive α-source and cyclotron beam will be reported.

Jet (fluid)Field (physics)[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]ChemistryNuclear engineeringNozzleCyclotron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energy030218 nuclear medicine & medical imagingIonlaw.inventionNuclear physics03 medical and health sciences0302 clinical medicinePhysics::Plasma PhysicslawElectric field0103 physical sciencesNuclear spectroscopy010306 general physicsBeam (structure)
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Spectroscopic studies of neutron-deficient light nuclei: decay properties of 21Mg, 25Si and 26P

2003

Neutron‐deficient nuclei with Tz equals to −3/2 and −2 have been produced at the GANIL/LISE3 facility in fragmentation reactions of a 95 MeV/u 36Ar primary beam in a 12C target. For the first time, β‐delayed proton and β‐γ emission has been simultaneously observed in the decay of 21Mg, 25Si and 26P. The decay scheme of the latter is proposed and the Gamow‐Teller strength distribution in its β decay is compared to shell‐model calculations based on the USD interaction. The B(GT) values derived from the absolute measurement of the β‐branching ratios are in agreement with the quenching factor of about 60% obtained for allowed Gamow‐Teller transitions in this mass region. A precise half‐life of …

23.50.+z 23.40.-s 23.20.Lv 27.30.+tPhysicsDecay schemeProtonIsotopes of germaniumBranching fractionNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyNuclear physicsDouble beta decayNeutronProton emissionAtomic physicsNuclear ExperimentRadioactive decayAIP Conference Proceedings
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Isomeric state of 80Y and its role in the rp-process

2003

The HIGISOL facility has been used to investigate carefully the isomeric transition 228.5 keV in 80Y. We have measured the electron internal conversion coefficient for this transition αK = 0.50 ± 0.07 which gives the value for half-life of “bare” isomeric state T 1/2 = 6.8 ± 0.5 s. The isomeric state should play an important role in the rp-process calculations.

Materials scienceThermodynamicsElectronState (functional analysis)rp-processNuclear isomerInternal conversion coefficientValue (mathematics)
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Isomeric state of $^{80}$Y and its role in the astrophysical rp-process

2001

5 pages, 7 figures.-- PACS nrs: 21.10.Tg; 23.20.Nx; 27.50.+e.

59 ≤ A ≤ 89 [[PACS] Properties of specific nuclei listed by mass ranges]PhysicsNuclear and High Energy Physics[PACS] Properties of specific nuclei listed by mass ranges: 59 ≤ A ≤ 89Proton[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]010308 nuclear & particles physicsHadronElectron[PACS] Internal conversion and extranuclear effects (including Auger electrons and internal bremsstrahlung)rp-processNuclear isomer[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsExcited state0103 physical sciences[PACS] Lifetimes widthsAtomic physics010306 general physicsInternal conversion coefficientExcitation
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Production of neutron-rich isotopes in fission of uranium induced by neutrons of 20 MeV average energy

2000

In the context of a parameter study conducted by several laboratories for future European radioactive beam facilities based on fast-neutron induced fission, in particular for the SPIRAL-II project at GANIL, we have measured the yields of neutron-rich isotopes in the mass range of 88 to 144. These nuclei were obtained as fission products of natural uranium bombarded by neutrons of 20 MeV average energy emitted by a thick carbon target irradiated by 50 MeV deuterons. Yields have been measured using on-line mass separation with the ion-guide method. Compared with proton-induced fission at 25 MeV the magnitude of cross-sections, except for the symmetric region, is similar. Z-distributions of is…

PhysicsNuclear and High Energy PhysicsCold fissionIsotopes of uranium010308 nuclear & particles physicsNeutron emissionIsotopes of samariumNuclear TheoryFission product yield[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyFast fissionNuclear physicsUranium-2380103 physical sciencesPhysics::Accelerator PhysicsNuclear Experiment010306 general physicsLong-lived fission product
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