J. Sarén
University of Jyväskylä
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Featured researches published by J. Sarén.
Nature | 2006
R.-D. Herzberg; P. T. Greenlees; P. A. Butler; G. D. Jones; M. Venhart; I. G. Darby; S. Eeckhaudt; Kari J. Eskola; T. Grahn; C. Gray-Jones; F. P. Hessberger; P. M. Jones; R. Julin; S. Juutinen; S. Ketelhut; W. Korten; M. Leino; A.-P. Leppänen; S. Moon; M. Nyman; R. D. Page; J. Pakarinen; A. Pritchard; P. Rahkila; J. Sarén; C. Scholey; A. Steer; Y. Sun; Ch. Theisen; J. Uusitalo
A long-standing prediction of nuclear models is the emergence of a region of long-lived, or even stable, superheavy elements beyond the actinides. These nuclei owe their enhanced stability to closed shells in the structure of both protons and neutrons. However, theoretical approaches to date do not yield consistent predictions of the precise limits of the ‘island of stability’; experimental studies are therefore crucial. The bulk of experimental effort so far has been focused on the direct creation of superheavy elements in heavy ion fusion reactions, leading to the production of elements up to proton number Z = 118 (refs 4, 5). Recently, it has become possible to make detailed spectroscopic studies of nuclei beyond fermium (Z = 100), with the aim of understanding the underlying single-particle structure of superheavy elements. Here we report such a study of the nobelium isotope 254No, with 102 protons and 152 neutrons—the heaviest nucleus studied in this manner to date. We find three excited structures, two of which are isomeric (metastable). One of these structures is firmly assigned to a two-proton excitation. These states are highly significant as their location is sensitive to single-particle levels above the gap in shell energies predicted at Z = 114, and thus provide a microscopic benchmark for nuclear models of the superheavy elements.
Physics Letters B | 2010
L. Bianco; R. D. Page; I. G. Darby; D. T. Joss; J. Simpson; J. S. Al-Khalili; A. J. Cannon; B. Cederwall; S. Eeckhaudt; S. Ertürk; B. J. P. Gall; M. B. Gomez Hornillos; T. Grahn; P. T. Greenlees; B. Hadinia; K. Heyde; U. Jakobsson; P. M. Jones; R. Julin; S. Juutinen; S. Ketelhut; M. Labiche; M. Leino; A.-P. Leppänen; M. Nyman; D. O'Donnell; E. S. Paul; M. Petri; P. Peura; A. Puurunen
The nuclides 157W and 161Os have been discovered in reactions of 58Ni ion beams with a 106Cd target. The 161Os α-decay energy and half-life were 6890±12 keV and 640±60 μs. The daughter 157W nuclei β-decayed with a half-life of 275±40 ms, populating both low-lying α-decaying states in 157Ta, which is consistent with a 7/2− ground state in 157W. Fine structure observed in the α decay of 161Os places the lowest excited state in 157W with Iπ =9/2− at 318±30 keV. The branching ratio of 5.5+3.1 −2.2% indicates that 161Os also has a 7/2− ground state. Shell-model calculations analysing the effects of monopole shifts and a tensor force on the relative energies of 2f7/2 and 1h9/2 neutron states in N=83 isotones are presented.
Physics Letters B | 2010
L. Bianco; R. D. Page; I. G. Darby; D. T. Joss; J. Simpson; J. J. Al-Khalili; A. J. Cannon; B. Cederwall; S. Eeckhaudt; S Erturk; B. J. P. Gall; M. B. Gomez Hornillos; T. Grahn; P. T. Greenlees; B. Hadinia; K. Heyde; U. Jakobsson; P. M. Jones; R. Julin; S. Juutinen; S. Ketelhut; M. Labiche; M. Leino; A.-P. Leppänen; M. Nyman; D. O'Donnell; E. S. Paul; M. Petri; P. Peura; A. Puurunen
The nuclides 157W and 161Os have been discovered in reactions of 58Ni ion beams with a 106Cd target. The 161Os α-decay energy and half-life were 6890±12 keV and 640±60 μs. The daughter 157W nuclei β-decayed with a half-life of 275±40 ms, populating both low-lying α-decaying states in 157Ta, which is consistent with a 7/2− ground state in 157W. Fine structure observed in the α decay of 161Os places the lowest excited state in 157W with Iπ =9/2− at 318±30 keV. The branching ratio of 5.5+3.1 −2.2% indicates that 161Os also has a 7/2− ground state. Shell-model calculations analysing the effects of monopole shifts and a tensor force on the relative energies of 2f7/2 and 1h9/2 neutron states in N=83 isotones are presented.
Physical Review C | 2007
B. S. Nara Singh; A. N. Steer; D. G. Jenkins; R. Wadsworth; M. A. Bentley; P. J. Davies; R. Glover; N. S. Pattabiraman; C. J. Lister; T. Grahn; P. T. Greenlees; Peter J. H. Jones; R. Julin; S. Juutinen; M. Leino; M. Nyman; J. Pakarinen; P. Rahkila; J. Sarén; C. Scholey; J. Sorri; J. Uusitalo; P. A. Butler; M. R. Dimmock; D. T. Joss; J. Thomson; B. Cederwall; B. Hadinia; M. Sandzelius
The technique of recoil {beta} tagging has been developed which allows prompt {gamma} decays in nuclei from excited states to be correlated with electrons from their subsequent short-lived {beta} decay. This technique is ideal for studying nuclei very far from stability and improves in sensitivity for very short-lived decays and for high decay Q-values. The method has allowed excited states in {sup 78}Y to be observed for the first time, as well as an extension in the knowledge of T=1 states in {sup 74}Rb. From this new information it has been possible to compare Coulomb energy differences (CED) between T=1 states in {sup 70}Br/{sup 70}Se, {sup 74}Rb/{sup 74}Kr, and {sup 78}Y/{sup 78}Sr. The A=70 CED exhibit an anomalous behavior which is inconsistent with all other known CED. This behavior may be accounted for qualitatively in terms of small variations in the Coulomb energy arising from shape changes.
Physical Review C | 2010
P. Rahkila; D. G. Jenkins; J. Pakarinen; C. Gray-Jones; P. T. Greenlees; U. Jakobsson; P. M. Jones; R. Julin; S. Juutinen; S. Ketelhut; H. Koivisto; M. Leino; P. Nieminen; M. Nyman; P. Papadakis; S. Paschalis; M. Petri; P. Peura; O. Roberts; T. Ropponen; P. Ruotsalainen; J. Sarén; C. Scholey; J. Sorri; A. G. Tuff; J. Uusitalo; R. Wadsworth; M. Bender; P.-H. Heenen
Excited states in the extremely neutron-deficient nucleus {sup 180}Pb have been identified for the first time using the JUROGAM II array in conjunction with the RITU recoil separator at the Accelerator Laboratory of the University of Jyvaeskylae. This study lies at the limit of what is presently achievable with in-beam spectroscopy, with an estimated cross section of only 10 nb for the {sup 92}Mo({sup 90}Zr,2n){sup 180}Pb reaction. A continuation of the trend observed in {sup 182}Pb and {sup 184}Pb is seen, where the prolate minimum continues to rise beyond the N=104 midshell with respect to the spherical ground state. Beyond-mean-field calculations are in reasonable correspondence with the trends deduced from experiment.
Physics Letters B | 2017
F. Wang; B. Sun; Zhenan Liu; R. D. Page; Chong Qi; C. Scholey; S. F. Ashley; L. Bianco; I. J. Cullen; I.G. Darby; Sarah Eeckhaudt; A. B. Garnsworthy; W. Gelletly; M.B. Gómez-Hornillos; T. Grahn; P. T. Greenlees; D. G. Jenkins; G. A. Jones; Peter W. Jones; D. T. Joss; R. Julin; S. Juutinen; S. Ketelhut; S. Khan; A. M. Kishada; M. Leino; M. Niikura; M. Nyman; J. Pakarinen; S. Pietri
Abstract The quenching of the experimental spectroscopic factor for proton emission from the short-lived d 3 / 2 isomeric state in 151mLu was a long-standing problem. In the present work, proton emission from this isomer has been reinvestigated in an experiment at the Accelerator Laboratory of the University of Jyvaskyla. The proton-decay energy and half-life of this isomer were measured to be 1295(5) keV and 15.4(8) μs, respectively, in agreement with another recent study. These new experimental data can resolve the discrepancy in the spectroscopic factor calculated using the spherical WKB approximation. Using the R-matrix approach it is found that the proton formation probability indicates no significant hindrance for the proton decay of 151mLu.
Physical Review C | 2013
P. Ruotsalainen; D. G. Jenkins; M. A. Bentley; K. Auranen; P. J. Davies; T. Grahn; P. T. Greenlees; J. Henderson; A. Herzáň; U. Jakobsson; P. Joshi; R. Julin; S. Juutinen; J. Konki; M. Leino; G. Lotay; A. J. Nichols; A. Obertelli; J. Pakarinen; J. Partanen; P. Peura; P. Rahkila; M. Sandzelius; J. Sarén; C. Scholey; J. Sorri; S. Stolze; J. Uusitalo; R. Wadsworth
Candidates for three excited states in the 66^Se have been identified using the recoil-{\beta} tagging method together with a veto detector for charged-particle evaporation channels. These results allow a comparison of mirror and triplet energy differences between analogue states across the A = 66 triplet as a function of angular momentum. The extracted triplet energy differences follow the negative trend observed in the f_7/2 shell. Shell-model calculations indicate a continued need for an additional isospin non-conserving interaction in addition to the Coulomb isotensor part as a function of mass.
Applied Radiation and Isotopes | 2012
J. Konki; P. T. Greenlees; U. Jakobsson; P. M. Jones; R. Julin; S. Juutinen; S. Ketelhut; K. Hauschild; R. Kontro; A.-P. Leppänen; A. Lopez-Martens; A. Mattila; P. Nieminen; M. Nyman; K. Peräjärvi; P. Peura; P. Rahkila; P. Ruotsalainen; J. Sarén; C. Scholey; J. Sorri; Harri Toivonen; J. Turunen; J. Uusitalo
Aerosol samples have been studied under different background conditions using gamma-ray coincidence and low-background gamma-ray singles spectrometric techniques with High-Purity Germanium detectors. Conventional low-background gamma-ray singles counting is a competitive technique when compared to the gamma-gamma coincidence approach in elevated background conditions. However, measurement of gamma-gamma coincidences can clearly make the identification of different nuclides more reliable and efficient than using singles spectrometry alone. The optimum solution would be a low-background counting station capable of both singles and gamma-gamma coincidence spectrometry.
Physica Scripta | 2006
R-D Herzberg; P. T. Greenlees; P. A. Butler; G. D. Jones; I. G. Darby; S. Eeckhaudt; T. Grahn; C. Gray-Jones; F. P. Hessberger; P. M. Jones; R. Julin; S. Juutinen; S. Ketelhut; M. Leino; A-P. Leppänen; S. Moon; M. Nyman; R. D. Page; J. Pakarinen; A. Pritchard; P. Rahkila; M. Sandzelius; J. Sarén; C. Scholey; A. N. Steer; J. Uusitalo; M. Venhart
Isomeric states in No-254 were investigated using a calorimetric method. Two different isomers were found with half-lives of T-1/2 = 266 +/- 2 ms and T-1/2 = 184 +/- 3 mu s, respectively. The domin ...
Hyperfine Interactions | 2016
P. Papadakis; I. D. Moore; I. Pohjalainen; J. Sarén; J. Uusitalo
A low-energy radioactive ion beam facility for the production and study of nuclei produced close to the proton drip line is under development at the Accelerator Laboratory of the University of Jyväskylä, Finland. The facility will take advantage of the mass selectivity of the recently commissioned MARA vacuum-mode mass separator. The ions selected by MARA will be stopped and thermalised in a small-volume gas cell prior to extraction and further mass separation. The gas cell design allows for resonance laser ionisation/spectroscopy both in-gas-cell and in-gas-jet. The facility will include experimental setups allowing ion counting, mass measurement and decay spectroscopy.