Fine Structure in Proton Emission from the Deformed 141g.sHo and 141mHo

Fine structure in proton emission from the deformed states {sup 141g.s}Ho (T{sub 1/2} = 4.1 ms) and {sup 141}mHo (T{sub 1/2} = 7.4 {micro}s) has been discovered at Oak Ridge by detecting fusion evaporation residues with the Recoil Mass Spectrometer, Si-detectors and digital signal processing electro...

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Hauptverfasser: Karny, M., Rykaczewski, Krzysztof, Grzywacz, R., Batchelder, J. C., Bingham, C. R., Goodin, C., Gross, Carl, Hamilton, J. H., Korgul, A., Krolas, W., Liddick, S. N., Li, K., Maier, Karl, Mazzocchi, C., Piechaczek, A., Shapira, Dan, Simpson, D., Tantawy, M. N., Winger, J. A., Yu, Chang-Hong, Zganjar, E. F.
Format: Tagungsbericht
Sprache:eng
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Zusammenfassung:Fine structure in proton emission from the deformed states {sup 141g.s}Ho (T{sub 1/2} = 4.1 ms) and {sup 141}mHo (T{sub 1/2} = 7.4 {micro}s) has been discovered at Oak Ridge by detecting fusion evaporation residues with the Recoil Mass Spectrometer, Si-detectors and digital signal processing electronics. The branching ratios to the first 2{sup +} excited state in {sup 140}Dy were measured to be I{sub p}{sup g.s.}(2{sup +}) = 0.9{+-}0.1% and I{sub p}{sup m}(2{sup +}) = 1.7{+-}0.5%. A comparison of the available calculations to the experimental values calls for further development of the theoretical models.
ISSN:0094-243X
1551-7616
DOI:10.1063/1.2827262