2011
DOI: 10.1103/physrevc.83.034602
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Production and decay properties of the 1.9-s isomeric state inRf261

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Cited by 45 publications
(39 citation statements)
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“…At the GARIS recoil separator of RIKEN, Haba and coworkers [117,124,125] have successfully synthesized and pre-separated the isotope 265 Sg which is available at a rate of about one atom per hour for chemical investigations [79]. This gave access to detailed nuclear decay studies of the ground-state and the isomeric state of 265 Sg [79] and to the complex decay pattern into two states of 261 Rf [126,127]. These experiments confirmed results from an earlier meta-analysis [215].…”
Section: Gas Phase Chemistrysupporting
confidence: 66%
See 1 more Smart Citation
“…At the GARIS recoil separator of RIKEN, Haba and coworkers [117,124,125] have successfully synthesized and pre-separated the isotope 265 Sg which is available at a rate of about one atom per hour for chemical investigations [79]. This gave access to detailed nuclear decay studies of the ground-state and the isomeric state of 265 Sg [79] and to the complex decay pattern into two states of 261 Rf [126,127]. These experiments confirmed results from an earlier meta-analysis [215].…”
Section: Gas Phase Chemistrysupporting
confidence: 66%
“…In this most recent development, which constitutes a breakthrough in SHE chemistry, gasfilled magnetic recoil-separators are applied between the target and the recoil chamber -now commonly termed Recoil Transfer Chamber, RTC [116][117][118]. Pioneering work has been performed at the BGS [113,116,119,120] followed by new developments and experiments at the TASCA [110][111][112][121][122][123], the GARIS [117,[124][125][126][127], which had also been used in combination with an IGISOL system before [128], and the DGFRS [129]. A scheme of such a setup, as used at the GARIS, is shown in Fig.…”
Section: Physical Pre-separatorsmentioning
confidence: 99%
“…Considerable progress in the experimental synthesis of heaviest nuclei has been achieved recently by the Flerov Laboratory in Dubna [1,2,3,4,5,6,7,8,9,10,11] and was partially confirmed in the laboratories at GSI [12,13,14,15,16], LBNL [17] and RIKEN [18]. Nonetheless, the fundamental question of what is the largest possible atomic number of an atomic nucleus is still unanswered.…”
Section: Introductionmentioning
confidence: 99%
“…It was observed as the α-decay daughter of 265 Sg in decay chains passing through these nuclides. Only recently, evidence for the formation of this second state as an EVR in a heavy-ion induced fusion reaction was obtained [67], and the most complete and most precise values for its production and decay properties were obtained in an experiment at GARIS [93] where EVRs of the 248 Cm( 18 O, 5n) 261 Rf reaction were preseparated in GARIS and transported by a gas-jet to MANON. This second state (often referred to as 261b Rf ) decays by α decay (27 ± 6%) with an α-particle energy of 8.52 ± 0.05 MeV and by SF (73 ± 6%) with a half-life of 1.9 ± 0.4 s [93].…”
Section: Garismentioning
confidence: 99%
“…Only recently, evidence for the formation of this second state as an EVR in a heavy-ion induced fusion reaction was obtained [67], and the most complete and most precise values for its production and decay properties were obtained in an experiment at GARIS [93] where EVRs of the 248 Cm( 18 O, 5n) 261 Rf reaction were preseparated in GARIS and transported by a gas-jet to MANON. This second state (often referred to as 261b Rf ) decays by α decay (27 ± 6%) with an α-particle energy of 8.52 ± 0.05 MeV and by SF (73 ± 6%) with a half-life of 1.9 ± 0.4 s [93]. The production of either of the two states in 261 Rf is equally probable in the 248 Cm( 18 O, 5n) reaction, the total cross section (for both states) was measured to be 23 ± 4 nb [93].…”
Section: Garismentioning
confidence: 99%