Nuclear Data Sheets for A = 115

Blachot, J.

doi:10.1016/j.nds.2005.03.003

Cited by 64 publications

(13 citation statements)

References 220 publications

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“…[26] as 0.8994 s. It can also be estimated on the basis of systematics of beta-decay partial half-lives for tellurium isotopes. Figure 7 shows the trend of these values as a function of the mass number A, from 109 Te to 115 Te [27][28][29][30]. With a linear regression on ln(T β ), the beta-decay partial half-life of 107 Te can be estimated to be 1.1 ± 0.1 s. This value, obtained with a simple extrapolation, is in agreement with the value calculated in [26].…”

Section: Resultssupporting

confidence: 85%

Experimental study of the decays of112Cs and111Xe

et al. 2012

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An experiment to search for the alpha decay of 112 Cs has been performed at the Holifield Radioactive Ion Beam Facility (HRIBF) at Oak Ridge National Laboratory. The alpha decay of 112 Cs was not observed, thus setting the upper limit of the alpha branching ratio at 0.26%. The half-life of 112 Cs was measured as 506 ± 55 µs. In the same measurement the decay properties of its proton decay daughter 111 Xe were also reinvestigated. The newly measured alpha branching ratio for 111 Xe is 10.4 ± 1.9 %. The experimental proton separation energies Sp for odd-Z nuclei above 100 Sn were compared to shell model calculations. The calculated proton separation energies for 103 Sb and 102 Sb point to half-lives of the order of 10 ps and 1 ns, respectively.

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Section: Resultssupporting

confidence: 85%

Experimental study of the decays of112Cs and111Xe

et al. 2012

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“…The decay data for the monitor reactions were taken from Refs. [22][23][24][25][26][27] and are given in Table II along with the reaction Q values [28]. The decay data for 240 Am and 241 Am used for the data analysis were taken from Refs.…”

Section: Induced Activity Measurementsmentioning

confidence: 99%

“…β-decay properties of the monitor reactions used for the neutron flux normalization (from Refs. [22][23][24][25][26][27]). …”

Section: Induced Activity Measurementsmentioning

confidence: 99%

High resolution measurements of theAm241(n,2n
Sage
¹
,
Semkova
²
,
Bouland
³

et al. 2010
Phys. Rev. C
26
0
11
0
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Measurements of the 241 Am(n,2n) reaction cross section have been performed at the Joint Research Centre (JRC) Geel in the frame of a collaboration between the European Commission (EC) JRC and French laboratories from CNRS and the Commissariatà L'Energie Atomique (CEA) Cadarache. Raw material coming from the Atalante facility of CEA Marcoule has been transformed by JRC Karlsruhe into suitable 241 AmO 2 samples embedded in Al 2 O 3 matrices specifically designed for these measurements. The irradiations were carried out at the 7-MV Van de Graaff accelerator. The 241 Am(n,2n) reaction cross section was determined relative to the 27 Al(n,α) 24 Na standard cross section. The measurements were performed in four sessions, using quasi-monoenergetic neutrons with energies ranging from 8 to 21 MeV produced via the 2 H(d,n) 3 He and the 3 H(d,n) 4 He reactions. The induced activity was measured by standard γ -ray spectrometry using a high-purity germanium detector. Below 15 MeV, the present results are in agreement with data obtained earlier. Above 15 MeV, these measurements allowed the experimental investigation of the 241 Am(n,2n) reaction cross section for the first time. The present data are in good agreement with predictions obtained with the TALYS code that uses an optical and fission model developed at CEA.

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“…[6,7]. A (5/2 + ) spin assignment for the 115 Pd ground state and (11/2 − ) for the isomeric state have been adopted in the Evaluated Nuclear Structure Data File [8,9] based on systematics. Later on, these assignments were changed to (3/2 + ) and (9/2 − ) [6], and further to (1/2 + ) and (7/2 − ), respectively [7].…”

Section: Introductionmentioning

confidence: 99%

Structure of115Ag studied byβ−decays of115Pd and
Rissanen
¹
,
Kurpeta
²
,
Elomaa
³

et al. 2012
Phys. Rev. C

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The excited levels of 115 Ag have been studied via the beta decay of 115 Pd and 115 Pd m . The beta-decay schemes for both states have been considerably extended, especially the scheme following the decay of 115 Pd m which was practically unknown before this work. Transition intensities and log 10 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 115 Pd 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 identification of Nilsson states in 115 Ag have been made.

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Nuclear Data Sheets for A = 115

Cited by 64 publications

References 220 publications

Experimental study of the decays of112Cs and111Xe

Experimental study of the decays of112Cs and111Xe

High resolution measurements of theAm241(n,2n
Sage
¹
,
Semkova
²
,
Bouland
³

et al. 2010
Phys. Rev. C
26
0
11
0
View full text Add to dashboard Cite

Structure of115Ag studied byβ−decays of115Pd and
Rissanen
¹
,
Kurpeta
²
,
Elomaa
³

et al. 2012
Phys. Rev. C

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Nuclear Data Sheets for A = 115

Cited by 64 publications

References 220 publications

Experimental study of the decays of112Cs and111Xe

Experimental study of the decays of112Cs and111Xe

High resolution measurements of theAm241(n,2nSage1, Semkova2, Bouland3 et al. 2010Phys. Rev. C260110View full textAdd to dashboardCite

Structure of115Ag studied byβ−decays of115Pd andRissanen1, Kurpeta2, Elomaa3 et al. 2012Phys. Rev. C

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About

High resolution measurements of theAm241(n,2n
Sage
¹
,
Semkova
²
,
Bouland
³

et al. 2010
Phys. Rev. C
26
0
11
0
View full text Add to dashboard Cite

Structure of115Ag studied byβ−decays of115Pd and
Rissanen
¹
,
Kurpeta
²
,
Elomaa
³

et al. 2012
Phys. Rev. C