Search results for "accelerator-based physics"

showing 10 items of 16 documents

Penning-trap mass measurements on 92, 94-98, 100Mo with JYFLTRAP

2012

Penning-trap measurements on stable 92, 94-98, 100Mo isotopes have been performed with relative accuracy of \ensuremath1⋅10−8\ensuremath1⋅10−8 with the JYFLTRAP Penning-trap mass spectrometer by using 85Rb as a reference. The Mo isotopes have been found to be about 3keV more bound than given in the Atomic Mass Evaluation 2003 (AME03). The results confirm that the discrepancy between the ISOLTRAP and JYFLTRAP data for 101-105Cd isotopes was due to an erroneous value in the AME03 for 96Mo used as a reference at JYFLTRAP. The measured frequency ratios of Mo isotopes have been used to update mass-excess values of 30 neutron-deficient nuclides measured at JYFLTRAP. peerReviewed

nuclear spectroscopyPhysicsNuclear and High Energy PhysicsMass excessIsotopeaccelerator-based physicsPenning trapMass spectrometrykiihdytinpohjainen fysiikkaISOLTRAPAtomic massNuclear physicsydinrakennenuclear structureydinspektroskopiaNuclear fusionNuclideAtomic physicsydinfysiikkaThe European Physical Journal A
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Prompt and delayed spectroscopy of 199At

2010

The neutron-deficient nucleus At199 has been studied through γ-ray and electron spectroscopy, using the recoil-decay tagging technique. Two experiments were conducted, using a gas-filled recoil separator with a focal-plane spectrometer alone and together with a germanium-detector array at the target position. The resulting level scheme for At199 includes a new isomer with a half-life of 0.80(5) μs and a spin and parity of (29/2+). The 13/2+ isomer, which de-excites via an M2 transition to the 9/2− ground state, was measured to have a half-life of 70(20) ns. Our earlier version of the level scheme for At197 has been updated as well. peerReviewed

nuclear spectroscopyydinrakenneaccelerator-based physicsnuclear structureydinspektroskopiaydinfysiikkakiihdytinpohjainen fysiikka
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Precision Mass Measurements beyond $^{132}$Sn: Anomalous behaviour of odd-even staggering of binding energies

2012

Atomic masses of the neutron-rich isotopes $^{121-128}$Cd, $^{129,131}$In, $^{130-135}$Sn, $^{131-136}$Sb, and $^{132-140}$Te have been measured with high precision (10 ppb) using the Penning trap mass spectrometer JYFLTRAP. Among these, the masses of four r-process nuclei $^{135}$Sn, $^{136}$Sb, and $^{139,140}$Te were measured for the first time. The data reveals a strong $N$=82 shell gap at $Z$=50 but indicates the importance of correlations for $Z>50$. An empirical neutron pairing gap expressed as the odd-even staggering of isotopic masses shows a strong quenching across $N$=82 for Sn, with the $Z$-dependence that is unexplainable by the current theoretical models.

nuclear spectroscopyydinrakenneTheoretical nuclear physicsaccelerator-based physicsnuclear structureydinspektroskopiaFOS: Physical sciencesNuclear Experiment (nucl-ex)ydinfysiikkakiihdytinpohjainen fysiikkaNuclear Experiment
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Low-spin excitations in the 109Tc nucleus

2012

Monoisotopic samples of ${}^{109}$Mo nuclei, produced in the deuteron-induced fission of ${}^{238}$U and separated using the IGISOL mass separator coupled to a Penning trap, were used to perform $\ensuremath{\beta}$- and $\ensuremath{\gamma}$-coincidence spectroscopy of ${}^{109}$Tc. Spin and parity 5/2${}^{+}$ for the ground state of ${}^{109}$Mo, proposed earlier, are supported in the present work. Three new low-energy levels observed in ${}^{109}$Tc are interpreted as bandheads of the $\ensuremath{\pi}3/{2}^{\ensuremath{-}}$[301], $\ensuremath{\pi}5/{2}^{\ensuremath{-}}$[303], and $\ensuremath{\pi}1/{2}^{+}$[431] configurations, respectively. A further three levels observed around 0.4 Me…

Nuclear and High Energy PhysicsFissionProlate spheroid[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]kiihdytinpohjainen fysiikka01 natural sciencesydinrakenneDouble beta decay0103 physical sciencesmedicine010306 general physicsSpectroscopynuclear spectroscopyPhysicsta114accelerator-based physics010308 nuclear & particles physicsParity (physics)medicine.anatomical_structurenuclear structureydinspektroskopiaAtomic physicsydinfysiikkaGround stateNucleusExcitation
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Mass measurements of neutron-deficient nuclei and their implications for astrophysics

2012

During the years 2005-2010 the double-Penning-trap mass spectrometer JYFLTRAP has been used to measure the masses of 90 ground and 8 isomeric states of neutron-deficient nuclides with a typical precision of better than 10keV. The masses of 14 nuclides -- 84Zr , 88, 89Tc , 90-92Ru , 92-94Rh , 94, 95Pd , 106, 108, 110Sb -- have been experimentally determined for the first time. This article gives an overview on these measurements and their impact on the modeling of the astrophysical rp -process. peerReviewed

nuclear spectroscopyPhysicsNuclear and High Energy PhysicsMass excessaccelerator-based physicsHadronMeasure (physics)Mass spectrometrykiihdytinpohjainen fysiikkaMass measurementNuclear physicsydinrakennenuclear structureydinspektroskopiaNuclear fusionNeutronNuclideydinfysiikkaThe European Physical Journal A
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Isomer and decay studies for the rp process at IGISOL

2012

This article reviews the decay studies of neutron-deficient nuclei within the mass region \ensuremathA=56--100 performed at the Ion-Guide Isotope Separator On-Line (IGISOL) facility in the University of Jyväskylä over last 25 years. Development from He-jet measurements to on-line mass spectrometry, and eventually to atomic mass measurements and post-trap spectroscopy at IGISOL, has yielded studies of around 100 neutron-deficient nuclei over the years. The studies form a solid foundation to astrophysical rp -process path modelling. The focus is on isomers studied either via spectroscopy or via Penning-trap mass measurements. The review is complemented with recent results on the ground and is…

Physicsnuclear spectroscopyNuclear and High Energy PhysicsIsotopeaccelerator-based physicsrp-processPenning trapMass spectrometrykiihdytinpohjainen fysiikkaAtomic massNuclear physicsydinrakennenuclear structureydinspektroskopiaNuclear fusionAtomic physicsGround stateSpectroscopyydinfysiikka
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Structure of 115Ag studied by β− decays of 115Pd and 115mPd

2012

The excited levels of 115Ag have been studied via the beta decay of 115Pd and 115Pdm. The beta-decay schemes for both states have been considerably extended, especially the scheme following the decay of 115Pdm which was practically unknown before this work. Transition intensities and log10 f t values are reported, which have been missing in the literature. A set of levels around 2 MeV has been found to be strongly populated by the beta decay of the ground state of 115Pd and is suggested to have a three-quasiparticle nature. The properties of excited levels have been compared with the level systematics of lighter neutron-rich silver isotopes, and new spin assignments as well as identificatio…

nuclear spectroscopyydinrakenneaccelerator-based physicsnuclear structureydinspektroskopiaydinfysiikkakiihdytinpohjainen fysiikka
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Candidate superdeformed band in 28Si

2012

Recent antisymmetrized molecular dynamics (AMD) calculations for 28Si suggest the presence of a superdeformed (SD) band with a dominant 24Mg + α clustering for its configuration, with firm predictions for its location and associated moment of inertia. This motivates a review of the experimental results reported in the literature with a particular focus on 24Mg(α,γ ) studies, as well as on α-like heavy-ion transfer reactions such as 12C(20Ne,α) 28Si. Combining this information for the first time leads to a set of candidate SD states whose properties point to their α-cluster structure and strong associated deformation. Analysis of data from Gammasphere allows the electromagnetic decay of thes…

nuclear spectroscopyydinrakenneaccelerator-based physicsnuclear structureydinspektroskopiaydinfysiikkakiihdytinpohjainen fysiikka
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High-accuracy mass spectrometry of fission products with Penning traps

2012

Mass measurements of fission products based on Penning-trap technique are reviewed in this article. More than 300 fission products have been measured with JYFLTRAP, ISOLTRAP, CPT, LEBIT and TITAN Penning traps with a typical precision of δm/m ≈ 10−7 − 10−8. In general, the results agree well with each other. The new data provide a valuable source of information and a challenge for the future development of theoretical mass models as well as for obtaining a deeper insight into microscopic properties of atomic nuclei as measured, for example, via key mass differentials. Shape transitions around N = 60, subshell closure at N = 40 and shell closures at N = 50 and N = 82 have been investigated i…

Nuclear and High Energy PhysicsNuclear TheoryMass spectrometry01 natural sciencesISOLTRAPkiihdytinpohjainen fysiikkaNuclear physicssymbols.namesakeydinrakenne0103 physical sciencesNuclear astrophysics010306 general physicsNuclear ExperimentPhysicsnuclear spectroscopyFission products010308 nuclear & particles physicsaccelerator-based physicsNuclear structure13. Climate actionPairingAtomic nucleusnuclear structuresymbolsydinspektroskopiaAtomic physicsTitan (rocket family)ydinfysiikka
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Precise Determination of the Unperturbed 8B Neutrino Spectrum

2012

The measurement was performed at the Kernfysisch Versneller Instituut (KVI) at the University of Groningen, The Netherlands.; A measurement of the final state distribution of the 8B $\beta$ decay, obtained by implanting a 8B beam in a double-sided silicon strip detector, is reported here. The present spectrum is consistent with a recent independent precise measurement performed by our collaboration at the IGISOL facility, Jyvâskylä [O. S. Kirsebom et al., Phys. Rev. C 83, 065802 (2011)]. It shows discrepancies with previously measured spectra, leading to differences in the derived neutrino spectrum. Thanks to a low detection threshold, the neutrino spectrum is for the first time directly ex…

nuclear spectroscopyneutrino oscillationsPhysics::Instrumentation and Detectorsaccelerator-based physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]kiihdytinpohjainen fysiikkaKVIydinrakenne8Bnuclear structureydinspektroskopiaimplantationydinfysiikka23.40.Bw 26.65.+t 27.20.+nbeta-decay
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