0000000000083268

AUTHOR

J. Giovinazzo

showing 26 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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New neutron-deficient isotopes from $^{78}$Kr fragmentation

2016

In an experiment with the BigRIPS separator at the RIKEN Nishina Center, the fragmentation of a $^{78}$Kr beam allowed the observation of new neutron-deficient isotopes at the proton drip-line. Clean identification spectra could be produced and $^{63}$Se, $^{67}$Kr, and $^{68}$Kr were identified for the first time. In addition, $^{59}$Ge was also observed. Three of these isotopes, $^{59}$Ge, $^{63}$Se, and $^{67}$Kr, are potential candidates for ground-state two-proton radioactivity. In addition, the isotopes $^{58}$Ge, $^{62}$Se, and $^{66}$Kr were also sought but without success. The present experiment also allowed the determination of production cross sections for some of the most exotic…

PhysicsIsotope010308 nuclear & particles physicsFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesSpectral lineNuclear physicsFragmentation (mass spectrometry)0103 physical sciencesNeutronNuclear Experiment (nucl-ex)Atomic physics010306 general physicsNuclear Experiment
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Relative proton andγwidths of astrophysically important states in30S studied in theβ-delayed decay of31Ar

2013

Resonances just above the proton threshold in S-30 affect the P-29(p, gamma)S-30 reaction under astrophysical conditions. The (p,gamma)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton and gamma partial widths of resonances in S-30. The widths are determined from the beta 2p- and beta p gamma-decay of Ar-31, which is produced at the ISOLDE radioactive ion beam facility at the European research organization CERN. Experimental limits on the ratio between the proton and gamma partial widths for astrophysical relevant levels in S-30 have been found for the first time. A le…

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderProtonIon beam010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaEuropean researchGamma ray01 natural sciencesGamma gamma0103 physical sciencesBeta (velocity)Atomic physics010306 general physicsPhysical Review C
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Observation of the 2+ isomer in Co52

2016

We report the first observation of the ${2}^{+}$ isomer in $^{52}\mathrm{Co}$, produced in the $\ensuremath{\beta}$ decay of the ${0}^{+}$, $^{52}\mathrm{Ni}$ ground state. We have observed three $\ensuremath{\gamma}$ rays at 849, 1910, and 5185 keV characterizing the $\ensuremath{\beta}$ de-excitation of the isomer. We have measured a half-life of 102(6) ms for the isomeric state. The Fermi and Gamow-Teller transition strengths for the $\ensuremath{\beta}$ decay of $^{52m}\mathrm{Co}$ to $^{52}\mathrm{Fe}$ have been determined. We also add new information on the $\ensuremath{\beta}$ decay of the ${6}^{+}$, $^{52}\mathrm{Co}$ ground state, for which we have measured a half-life of 112(3) ms.

Physics010308 nuclear & particles physics0103 physical sciencesAtomic physics010306 general physicsGround state01 natural sciencesPhysical Review C
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Studying the Exotic Decay $^{70}Kr$ $\rightarrow$ $^{70}Br$

2019

Acta physica Polonica / B 51(3), 587 (2020). doi:10.5506/APhysPolB.51.587

Nuclear physicsPhysics010308 nuclear & particles physics0103 physical sciencesGeneral Physics and Astronomyddc:530[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences530
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Super-Allowed β Decay of23Mg Studied with a High-Precision Germanium Detector

2015

Physicsnuclear mirror transitionsta114super-allowed decayAnalytical chemistryquark-mixing matrixSemiconductor detectorProceedings of the Conference on Advances in Radioactive Isotope Science (ARIS2014)
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Multiparticle emission in the decay ofAr31

2014

A multihit capacity setup was used to study the decay of the dripline nucleus Ar-31, produced at the ISOLDE facility at CERN. A spectroscopic analysis of the beta-delayed three-proton decay of Ar-31 is presented for the first time together with a quantitative analysis of the beta-delayed 2p gamma decay. A new method for determination of the spin of low-lying levels in the beta p daughter 30S using proton-proton angular correlations is presented and used to determine that the spin of the 5.2-MeV level is most likely 3(+) with 4(+) also possible. The half-life of Ar-31 is found to be 15.1(3) ms. An improved analysis of the Fermi beta strength including the beta 3p-decay mode gives a total mea…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsBranching fractionGamma ray7. Clean energy01 natural sciencesNuclear physicsmedicine.anatomical_structure0103 physical sciencesmedicineIsobaric processBeta (velocity)Atomic physics010306 general physicsNucleusSpin-½Fermi Gamma-ray Space TelescopePhysical Review C
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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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Nuclear weak response from the combined study of beta-decay and charge-exchange reaction

2009

Studying the weak nuclear response, especially the Gamow-Teller (GT) transitions, of stable as well as unstable pf-shell nuclei, is one of the key issues in nuclear and astro-nuclear physics. We study the decay half-lives and the GT transitions starting from Tz = ±1 and ±2 mirror nuclei, respectively, by means of β decays and complementary hadronic (3 He , t) charge-exchange reactions. Under the assumption that isospin is a good quantum number, symmetry is expected for mirror nuclei and the GT transitions starting from the mirror nuclei. The half-lives and branching ratios and the measured strength distributions of GT transitions are compared and also combined for the understanding of the …

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsHadronNuclear TheoryNuclear structureGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Key issues01 natural sciencesGood quantum numberNuclear physicsIsospin0103 physical sciencesMirror nucleiAtomic physics010306 general physicsNuclear ExperimentCharge exchange
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Precise half-life measurement of the Si-26 ground state

2008

The beta-decay half-life of 26Si was measured with a relative precision of 1.4*10e3. The measurement yields a value of 2.2283(27) s which is in good agreement with previous measurements but has a precision that is better by a factor of 4. In the same experiment, we have also measured the non-analogue branching ratios and could determine the super-allowed one with a precision similar to the previously reported measurements. The experiment was done at the Accelerator Laboratory of the University of Jyvaskyla where we used the IGISOL technique with the JYFLTRAP facility to separate pure samples of 26Si.

PhysicsNuclear and High Energy PhysicsBranching fraction010308 nuclear & particles physicsFOS: Physical sciencesHalf-life01 natural sciencesNuclear physics0103 physical sciencesRelative precisionNuclear Experiment (nucl-ex)010306 general physicsGround stateNuclear ExperimentNuclear Physics
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Half-life, branching-ratio, andQ-value measurement for the superallowed0+→0+β+emitterTi42

2009

The half-life, the branching ratio, and the decay $Q$ value of the superallowed $\ensuremath{\beta}$ emitter $^{42}\mathrm{Ti}$ were measured in an experiment performed at the JYFLTRAP facility of the Accelerator Laboratory of the University of Jyv\"askyl\"a. $^{42}\mathrm{Ti}$ is the heaviest ${T}_{z}=\ensuremath{-}1$ nucleus for which high-precision measurements of these quantities have been tried. The half-life (${T}_{1/2}=208.14\ifmmode\pm\else\textpm\fi{}0.45$ ms) and the $Q$ value [${Q}_{\mathrm{EC}}=7016.83(25)$ keV] are close to or reach the required precision of about 0.1%. The branching ratio for the superallowed decay branch [$\mathrm{BR}=47.7(12)%$], a by-product of the half-lif…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsQ valueBranching fraction0103 physical sciencesHalf-lifeAtomic physics010306 general physics01 natural sciencesCommon emitterPhysical Review C
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Sizeable beta-strength in $^{31}$Ar (β3p) decay

2014

5 pags. ; 7 figs. ; Open Access funded by SCOAP3 - Sponsoring Consortium for Open Access Publishing in Particle Physics

Nuclear and High Energy PhysicsFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex01 natural sciencesNuclear physicsESPECTROSCOPÍA0103 physical sciencesNuclear Physics - ExperimentBeta (velocity)Nuclear Experiment (nucl-ex)010306 general physicsFÍSICA NUCLEARNuclear ExperimentPhysicsta114Isotope010308 nuclear & particles physicsIsotopes of chlorineIsotopes of argonSPECTROSCOPICBeta decaylcsh:QC1-999DESINTEGRATION3. Good healthFísica nuclearHigh Energy Physics::ExperimentAtomic physicsEMISSIONlcsh:PhysicsFÍSICAEnergy (signal processing)ExcitationRadioactive decay
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Beta decay of the exotic Tz = - 2, $^{56}$Zn nucleus and half-life of various proton-rich Tz = -1 nuclei

2014

Expérience GANIL/LISE3/EXOGAM; International audience; Preliminary results of an experimental study of the beta -decay of the exotic T$_z$ = - 2, $^{56}$Zn nucleus and other proton-rich T$_z$ = -1 nuclei are presented. The ions were produced at GANIL using fragmentation reactions, separated by the LISE3 spectrometer and implanted in a double-sided silicon strip detector surrounded by Ge detectors. The half-lives of $^{56}$Zn and four T$_z$ = -1 nuclei in the fp-shell have been measured. While the decay of the T$_z$ = -1 nuclei proceeds essentially by -delayed gamma emission, in the case of $^{56}$Zn -delayed proton emission is also observed. Moreover, the exotic -delayed gamma-proton decay …

PhysicsNuclear physics23.40.-s 23.50.+z 21.10.-k 27.40.+zmedicine.anatomical_structureProtonmedicineGeneral Physics and AstronomyHalf-life[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyBeta decayNucleus
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Two-Proton Radioactivity ofKr67

2016

In an experiment with the BigRIPS separator at the RIKEN Nishina Center, we observed two-proton (2p) emission from 67Kr. At the same time, no evidence for 2p emission of 59Ge and 63Se, two other potential candidates for this exotic radioactivity, could be observed. This observation is in line with Q value predictions which pointed to 67Kr as being the best new candidate among the three for two-proton radioactivity. 67Kr is only the fourth 2p ground-state emitter to be observed with a half-life of the order of a few milliseconds. The decay energy was determined to be 1690(17) keV, the 2p emission branching ratio is 37(14)%, and the half-life of 67Kr is 7.4(30) ms.

PhysicsProton010308 nuclear & particles physicsBranching fractionQ valueGeneral Physics and Astronomy01 natural sciences7. Clean energyNuclear physicsDecay energy0103 physical sciencesAtomic physics010306 general physicsCommon emitterLine (formation)Physical Review Letters
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β decay of the very neutron-deficient Ge60 and Ge62 nuclei

2021

We report here the results of a study of the $\beta$ decay of the proton-rich Ge isotopes, $^{60}$Ge and $^{62}$Ge, produced in an experiment at the RIKEN Nishina Center. We have improved our knowledge of the half-lives of $^{62}$Ge (73.5(1) ms), $^{60}$Ge (25.0(3) ms) and its daughter nucleus, $^{60}$Ga (69.4(2) ms). We measured individual $\beta$-delayed proton and $\gamma$ emissions and their related branching ratios. Decay schemes and absolute Fermi and Gamow-Teller transition strengths have been determined. The mass excesses of the nuclei under study have been deduced. A total $\beta$-delayed proton-emission branching ratio of 67(3)% has been obtained for $^{60}$Ge. New information has…

PhysicsIsotope010308 nuclear & particles physicsBranching fractionExcited state0103 physical sciencesNeutronAtomic physics010306 general physicsGround state7. Clean energy01 natural sciencesFermi Gamma-ray Space TelescopePhysical Review C
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$\beta $-delayed $\gamma $-proton Decay in $^{56}$Zn: Analysis of the Charged-particle Spectrum

2014

A study of the $\beta$ decay of the proton-rich $T_{z}$ = -2 nucleus $^{56}$Zn has been reported in a recent publication. A rare and exotic decay mode, $\beta$-delayed $\gamma$-proton decay, has been observed there for the first time in the $fp$ shell. Here we expand on some of the details of the data analysis, focussing on the charged particle spectrum.

Physics010308 nuclear & particles physicsProton decaySpectrum (functional analysis)Nuclear TheoryGeneral Physics and AstronomyFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCharged particle23.40.–s 23.50.+z 21.10.–k 27.40.+zNuclear physicsmedicine.anatomical_structureBeta (plasma physics)0103 physical sciencesmedicineHigh Energy Physics::ExperimentFísica nuclearNuclear Experiment (nucl-ex)Nuclear ExperimentNucleusNuclear Experiment
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Simultaneous investigation of the T=1(Jπ=0+) and T=0(Jπ=9+) β decays in Br70

2017

The $\beta$ decay of the odd-odd nucleus $^{70}$Br has been investigated with the BigRIPS and EURICA setups at the Radioactive Ion Beam Factory (RIBF) of the RIKEN Nishina Center. The $T=0$ ($J^{\pi}=9^+$) and $T=1$ ($J^{\pi}=0^+$) isomers have both been produced in in-flight fragmentation of $^{78}$Kr with ratios of 41.6(8)\% and 58.4(8)\%, respectively. A half-life of $t_{1/2}=2157^{+53}_{-49}$ ms has been measured for the $J^{\pi}=9^+$ isomer from $\gamma$-ray time decay analysis. Based on this result, we provide a new value of the half-life for the $J^{\pi}=0^+$ ground state of $^{70}$Br, $t_{1/2}=78.42\pm0.51$ ms, which is slightly more precise, and in excellent agreement, with the bes…

PhysicsSpins010308 nuclear & particles physicsBranching fractionTime decayProlate spheroid01 natural sciencesNuclear physicsExcited state0103 physical sciencesPiAtomic physics010306 general physicsGround stateExcitationPhysical Review C
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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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Observation of theβ-Delayedγ-Proton Decay ofZn56and its Impact on the Gamow-Teller Strength Evaluation

2014

We report the observation of a very exotic decay mode at the proton drip line, the $\ensuremath{\beta}$-delayed $\ensuremath{\gamma}$-proton decay, clearly seen in the $\ensuremath{\beta}$ decay of the ${T}_{z}=\ensuremath{-}2$ nucleus $^{56}\mathrm{Zn}$. Three $\ensuremath{\gamma}$-proton sequences have been observed after the $\ensuremath{\beta}$ decay. Here this decay mode, already observed in the $sd$ shell, is seen for the first time in the $fp$ shell. Both $\ensuremath{\gamma}$ and proton decays have been taken into account in the estimation of the Fermi and Gamow-Teller strengths. Evidence for fragmentation of the Fermi strength due to strong isospin mixing is found.

Nuclear physicsPhysicsProton decayIsospinDouble beta decayNuclear TheoryGeneral Physics and AstronomyHigh Energy Physics::ExperimentNuclear ExperimentNuclear theoryBeta decayFermi Gamma-ray Space TelescopePhysical Review Letters
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Beta Decay Study of the Tz=−2 56Zn Nucleus and the Determination of the Half-Lives of a Few fp-shell Nuclei

2014

Abstract This paper concerns the experimental study of the β decay properties of few proton-rich fp -shell nuclei. The nuclei were produced at GANIL in fragmentation reactions, separated with the LISE spectrometer and stopped in an implantation detector surrounded by Ge detectors. The β -delayed gammas, β -delayed protons and the exotic β -delayed gamma-proton emission have been studied. Preliminary results are presented. The decay of the T z = − 2 nucleus 56 Zn has been studied in detail. Information from the β -delayed protons and β -delayed gammas has been used to deduce the decay scheme. The exotic beta-delayed gamma-proton decay has been observed for the first time in the fp -shell. Th…

PhysicsNuclear and High Energy PhysicsDecay schemeNuclear TheoryNuclear dataHalf-lifeBeta decayNuclear physicsmedicine.anatomical_structureFragmentation (mass spectrometry)Double beta decaymedicineMirror nucleiAtomic physicsNuclear ExperimentNucleusNuclear Data Sheets
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Precise measurements of half-lives and branching ratios for the ββ mirror transitions in the decay of 23Mg and 27Si

2017

Half-lives and branching ratios for the two mirror ββ decays of 23Mg and 27Si have been measured at the University of Jyväskylä with the IGISOL facility. The results obtained, T1/2=11.303(3)T1/2=11.303(3) s and T1/2=4.112(2)T1/2=4.112(2) s for the half-lives of 23Mg and 27Si , respectively, are 7 and 8 times more precise than the averages of previous measurements. The values obtained for the super-allowed branching ratios of 23Mg and 27Si are B.R.=92.18(8)%B.R.=92.18(8)% and B.R.=99.74(2)%B.R.=99.74(2)% , respectively. The result for 23Mg is three times more precise than the average of the previous measurements, while for 27Si the precision has not been improved, the average of the previous…

branching ratioshalf-livesmirror transitions
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Relative proton and γ widths of astrophysically important states in 30S studied in the β-delayed decay of 31Ar

2013

Resonances just above the proton threshold in 30S affect the 29P(p,gamma)30S reaction under astrophysical conditions. The (p,gamma)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton and gamma partial widths of resonances in 30S. The widths are determined from the beta-2p and beta-p-gamma decay of 31Ar, which is produced at the ISOLDE facility at the European research organization CERN. Experimental limits on the ratio between the proton and gamma partial widths for astrophysical relevant levels in 30S have been found for the first time. A level at 4688(5) keV is identif…

26.30.−k 23.40.Hc 27.30.+tAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesddc:530Experimental nuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment
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Multiparticle emission in the decay of Ar 31

2014

A multihit capacity setup was used to study the decay of the dripline nucleus 31Ar, produced at the ISOLDE facility at CERN. A spectroscopic analysis of the β-delayed three-proton decay of 31Ar is presented for the first time together with a quantitative analysis of the β-delayed 2pγ decay. A new method for determination of the spin of low-lying levels in the βp daughter 30S using proton-proton angular correlations is presented and used to determine that the spin of the 5.2-MeV level is most likely 3+ with 4+ also possible. The half-life of 31Ar is found to be 15.1(3) ms. An improved analysis of the Fermi β strength including the β3p-decay mode gives a total measured branching ratio of 3.60…

NUCLEAR EXPERIMENTmultiparticle emissionCIENCIAANÁLISIS ESPECTROSCÓPICOBETA DESINTEGRATIONPROTONFÍSICA NUCLEARFÍSICA
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Multi-particle emission in the decay of $^{31}$Ar

2014

A multi-hit capacity setup was used to study the decay of the dripline nucleus 31Ar, produced at the ISOLDE facility at CERN. A spectroscopic analysis of the beta-delayed three-proton decay of 31Ar is presented for the first time together with a quantitative analysis of the beta-delayed two-proton-gamma-decay. A new method for determination of the spin of low-lying levels in the beta-proton-daughter 30S using proton-proton angular correlations is presented and used for the level at 5.2 MeV, which is found to be either a 3+ or 4+ level, with the data pointing towards the 3+. The half-life of 31Ar is found to be 15.1(3) ms. An improved analysis of the Fermi beta-strength gives a total measure…

Physics::Accelerator PhysicsFOS: Physical sciencesNuclear Physics - Experiment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment23.40.Hc 27.30.+t
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Observation of the beta-Delayed gamma-Proton Decay of Zn-56 and its Impact on the Gamow-Teller Strength Evaluation

2014

We report the observation of a very exotic decay mode at the proton drip line, the beta-delayed gamma-proton decay, clearly seen in the beta decay of the T-z = -2 nucleus Zn-56. Three gamma-proton sequences have been observed after the beta decay. Here this decay mode, already observed in the sd shell, is seen for the first time in the f p shell. Both. and proton decays have been taken into account in the estimation of the Fermi and Gamow-Teller strengths. Evidence for fragmentation of the Fermi strength due to strong isospin mixing is found.

Nuclear TheoryHigh Energy Physics::ExperimentFísica nuclearNuclear Experiment
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