Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu
Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0...
Ausführliche Beschreibung
Autor*in: |
Bizzeti-Sona, A. M. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
1993 |
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Anmerkung: |
© Springer-Verlag 1993 |
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Übergeordnetes Werk: |
Enthalten in: Zeitschrift für Physik. A, Hadrons and nuclei - Springer-Verlag, 1975, 346(1993), 3 vom: Sept., Seite 181-182 |
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Übergeordnetes Werk: |
volume:346 ; year:1993 ; number:3 ; month:09 ; pages:181-182 |
Links: |
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DOI / URN: |
10.1007/BF01306076 |
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Katalog-ID: |
OLC2029736031 |
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245 | 1 | 0 | |a Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu |
264 | 1 | |c 1993 | |
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520 | |a Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. | ||
700 | 1 | |a Stefanini, A. A. |4 aut | |
700 | 1 | |a Brandolini, F. |4 aut | |
700 | 1 | |a Pavan, P. |4 aut | |
700 | 1 | |a Haque, A. M. I. |4 aut | |
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10.1007/BF01306076 doi (DE-627)OLC2029736031 (DE-He213)BF01306076-p DE-627 ger DE-627 rakwb eng 530 VZ Bizzeti-Sona, A. M. verfasserin aut Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1993 Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. Stefanini, A. A. aut Brandolini, F. aut Pavan, P. aut Haque, A. M. I. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 346(1993), 3 vom: Sept., Seite 181-182 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:346 year:1993 number:3 month:09 pages:181-182 https://doi.org/10.1007/BF01306076 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4193 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4336 GBV_ILN_4700 AR 346 1993 3 09 181-182 |
spelling |
10.1007/BF01306076 doi (DE-627)OLC2029736031 (DE-He213)BF01306076-p DE-627 ger DE-627 rakwb eng 530 VZ Bizzeti-Sona, A. M. verfasserin aut Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1993 Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. Stefanini, A. A. aut Brandolini, F. aut Pavan, P. aut Haque, A. M. I. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 346(1993), 3 vom: Sept., Seite 181-182 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:346 year:1993 number:3 month:09 pages:181-182 https://doi.org/10.1007/BF01306076 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4193 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4336 GBV_ILN_4700 AR 346 1993 3 09 181-182 |
allfields_unstemmed |
10.1007/BF01306076 doi (DE-627)OLC2029736031 (DE-He213)BF01306076-p DE-627 ger DE-627 rakwb eng 530 VZ Bizzeti-Sona, A. M. verfasserin aut Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1993 Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. Stefanini, A. A. aut Brandolini, F. aut Pavan, P. aut Haque, A. M. I. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 346(1993), 3 vom: Sept., Seite 181-182 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:346 year:1993 number:3 month:09 pages:181-182 https://doi.org/10.1007/BF01306076 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4193 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4336 GBV_ILN_4700 AR 346 1993 3 09 181-182 |
allfieldsGer |
10.1007/BF01306076 doi (DE-627)OLC2029736031 (DE-He213)BF01306076-p DE-627 ger DE-627 rakwb eng 530 VZ Bizzeti-Sona, A. M. verfasserin aut Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1993 Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. Stefanini, A. A. aut Brandolini, F. aut Pavan, P. aut Haque, A. M. I. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 346(1993), 3 vom: Sept., Seite 181-182 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:346 year:1993 number:3 month:09 pages:181-182 https://doi.org/10.1007/BF01306076 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4193 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4336 GBV_ILN_4700 AR 346 1993 3 09 181-182 |
allfieldsSound |
10.1007/BF01306076 doi (DE-627)OLC2029736031 (DE-He213)BF01306076-p DE-627 ger DE-627 rakwb eng 530 VZ Bizzeti-Sona, A. M. verfasserin aut Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1993 Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. Stefanini, A. A. aut Brandolini, F. aut Pavan, P. aut Haque, A. M. I. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 346(1993), 3 vom: Sept., Seite 181-182 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:346 year:1993 number:3 month:09 pages:181-182 https://doi.org/10.1007/BF01306076 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4193 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4336 GBV_ILN_4700 AR 346 1993 3 09 181-182 |
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Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei 346(1993), 3 vom: Sept., Seite 181-182 volume:346 year:1993 number:3 month:09 pages:181-182 |
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Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei 346(1993), 3 vom: Sept., Seite 181-182 volume:346 year:1993 number:3 month:09 pages:181-182 |
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Bizzeti-Sona, A. M. @@aut@@ Stefanini, A. A. @@aut@@ Brandolini, F. @@aut@@ Pavan, P. @@aut@@ Haque, A. M. I. @@aut@@ |
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theg-factor of the $ 8^{+} $ isomer $ of^{142} $eu |
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Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu |
abstract |
Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. © Springer-Verlag 1993 |
abstractGer |
Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. © Springer-Verlag 1993 |
abstract_unstemmed |
Abstract Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu with mean lifeτ=9 ns, has been measured by the time-differential perturbedγ ray angular distribution (TDPAD) method. The $ 8^{+} $ isomer was populated with the $ reaction^{114} $Cd(32S,p3n)142Eu at 155 MeV. The obtained valueg($ 8^{+} $)=0.51(3) agrees with shell model calculations using effective single-particle moments taken from neighbouring nuclei. A main configurationπ$ h_{11/2} $⊗(vh11/2)−1 has been confirmed for the $ 8^{+} $ isomer. © Springer-Verlag 1993 |
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Theg-factor of the $ 8^{+} $ isomer $ of^{142} $Eu |
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