The Q values of the heavy Cd and In isotopes

Spanier, L.; Aleklett, K.; Ekstrom, Brenda L.; Fogelberg, B.

doi:10.1016/0375-9474(87)90621-x

Cited by 29 publications

(36 citation statements)

References 18 publications

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“…However, the 1 − , 3 + and 1 + states, resulting from the coupling of a proton hole g 9/2 with the neutron holes h 11/2 , d 3/2 or g 7/2 , respectively, are experimentally known [18,19] This variation could be explained by a decrease in the effects of p − n interaction when increasing the number of neutron holes. However, as for the aligned 29/2 + state in 127 In, the decrease is underestimated by the calculation.…”

Section: B Even In Nucleimentioning

confidence: 99%

Neutron-rich In and Cd isotopes close to the doubly magicSn132

et al. 2004

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Section: B Even In Nucleimentioning

confidence: 99%

Neutron-rich In and Cd isotopes close to the doubly magicSn132

et al. 2004

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“…At the same time, the formulas (13), (14), (21) and (26) can be used to obtain expressions for calculating the cumulative yield of the first nuclide, as well as the independent and cumulative yields of the second nuclide:…”

Section: Techniquesmentioning

confidence: 99%

“…The spectra thus processed were combined to form an input file for the SIGMA code. The code plots the intensity of a selected γ-line versus time and, using its energy and simulated half-life, identifies the produced nuclides by the GDISP database and simulates their cross sections by formulas (27)(28)(29)(30) [14].…”

Section: Measurement and Processing Of γ-Ray Spectramentioning

confidence: 99%

Experimental and computer simulation study of the radionuclides produced in thin 209Bi targets by 130 MeV and 1.5 GeV proton-induced reactions

Titarenko¹,

Shvedov²,

Igumnov³

et al. 1998

Nuclear Instruments and Methods in Physics Research Section A:

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The results of experimental and computer simulation studies of the yields of residual product nuclei in 209 Bi thin targets irradiated by 130 MeV and 1.5 GeV protons are presented. The yields were measured by direct high-precision γ-spectrometry. The γ-spectrometer resolution was 1.8 keV in the 1332 keV line. The γ-spectra were processed by the ASPRO code. The γ-lines were identified, and the cross sections defined, by the SIGMA code using the GDISP radioactive database. The process was monitored by the 27 Al(p,x) 24 Na reaction. Results are presented for comparisons between the 209 Bi(p,x) reaction yields obtained experimentally and simulated by the HETC, GNASH, LAHET, INUCL, CEM95, CASCADE, and ALICE codes.

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“…However, the 1 − , 3 + and 1 + states, resulting from the coupling of a proton hole g 9/2 with the neutron holes h 11/2 , d 3/2 or g 7/2 , respectively, are experimentally known [18,19] in 126−130 In. In these three states the neutron and proton are in coplanar orbits and the p − n interaction is expected to become strongly attractive, in particular for the 1 + state.…”

Section: B Even In Nucleimentioning

confidence: 99%