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.
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container_volume 961
creator 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.
description 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.
doi_str_mv 10.1063/1.2827262
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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%. 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(ORNL), Oak Ridge, TN (United States)</aucorp><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Fine Structure in Proton Emission from the Deformed 141g.sHo and 141mHo</atitle><date>2007-11-01</date><risdate>2007</risdate><volume>961</volume><issn>0094-243X</issn><eissn>1551-7616</eissn><abstract>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%. 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subjects BRANCHING RATIO
EVAPORATION
EXCITED STATES
FINE STRUCTURE
HOLMIUM ISOTOPES
MASS SPECTROMETERS
NUCLEI
PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
PROCESSING
PROTONS
RESIDUES
title Fine Structure in Proton Emission from the Deformed 141g.sHo and 141mHo
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