Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm
Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations an...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bazzacco, D. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1990 |
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| Schlagwörter: |
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| Anmerkung: |
© J.C. Baltzer A.G., Scientific Publishing Company 1990 |
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| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 59(1990), 1-4 vom: Aug., Seite 133-136 |
|---|---|
| Übergeordnetes Werk: |
volume:59 ; year:1990 ; number:1-4 ; month:08 ; pages:133-136 |
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| DOI / URN: |
10.1007/BF02401207 |
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OLC2076363181 |
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| 245 | 1 | 0 | |a Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm |
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| 520 | |a Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) | ||
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| 700 | 1 | |a Brandolini, F. |4 aut | |
| 700 | 1 | |a Löwenich, K. |4 aut | |
| 700 | 1 | |a Pavan, P. |4 aut | |
| 700 | 1 | |a Alvarez, C. Rossi |4 aut | |
| 700 | 1 | |a De Poli, M. |4 aut | |
| 700 | 1 | |a Haque, A. M. I. |4 aut | |
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10.1007/BF02401207 doi (DE-627)OLC2076363181 (DE-He213)BF02401207-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) Thin Film Vibrational State Field Technique Transient Field Octupole Vibrational State Brandolini, F. aut Löwenich, K. aut Pavan, P. aut Alvarez, C. Rossi aut De Poli, M. aut Haque, A. M. I. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 59(1990), 1-4 vom: Aug., Seite 133-136 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:133-136 https://doi.org/10.1007/BF02401207 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 59 1990 1-4 08 133-136 |
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10.1007/BF02401207 doi (DE-627)OLC2076363181 (DE-He213)BF02401207-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) Thin Film Vibrational State Field Technique Transient Field Octupole Vibrational State Brandolini, F. aut Löwenich, K. aut Pavan, P. aut Alvarez, C. Rossi aut De Poli, M. aut Haque, A. M. I. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 59(1990), 1-4 vom: Aug., Seite 133-136 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:133-136 https://doi.org/10.1007/BF02401207 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 59 1990 1-4 08 133-136 |
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10.1007/BF02401207 doi (DE-627)OLC2076363181 (DE-He213)BF02401207-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) Thin Film Vibrational State Field Technique Transient Field Octupole Vibrational State Brandolini, F. aut Löwenich, K. aut Pavan, P. aut Alvarez, C. Rossi aut De Poli, M. aut Haque, A. M. I. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 59(1990), 1-4 vom: Aug., Seite 133-136 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:133-136 https://doi.org/10.1007/BF02401207 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 59 1990 1-4 08 133-136 |
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10.1007/BF02401207 doi (DE-627)OLC2076363181 (DE-He213)BF02401207-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) Thin Film Vibrational State Field Technique Transient Field Octupole Vibrational State Brandolini, F. aut Löwenich, K. aut Pavan, P. aut Alvarez, C. Rossi aut De Poli, M. aut Haque, A. M. I. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 59(1990), 1-4 vom: Aug., Seite 133-136 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:133-136 https://doi.org/10.1007/BF02401207 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 59 1990 1-4 08 133-136 |
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10.1007/BF02401207 doi (DE-627)OLC2076363181 (DE-He213)BF02401207-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) Thin Film Vibrational State Field Technique Transient Field Octupole Vibrational State Brandolini, F. aut Löwenich, K. aut Pavan, P. aut Alvarez, C. Rossi aut De Poli, M. aut Haque, A. M. I. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 59(1990), 1-4 vom: Aug., Seite 133-136 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:133-136 https://doi.org/10.1007/BF02401207 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 59 1990 1-4 08 133-136 |
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transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $sm |
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Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm |
| abstract |
Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) © J.C. Baltzer A.G., Scientific Publishing Company 1990 |
| abstractGer |
Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) © J.C. Baltzer A.G., Scientific Publishing Company 1990 |
| abstract_unstemmed |
Abstract The g-factor of the octupole vibrational state $ 3^{−} $ at 1810 keV $ in^{144} $Sm has been measured to be 0.76(9) by means of the transient field technique. The state has been Coulomb excited by 217 $ MeV^{58} $Ni beam. The obtained value agrees with the predictions of RPA calculations and confirms the dominance of the proton particle-hole configuration π($ 1h_{11/2} $−$ 2d_{5/2} $−1) © J.C. Baltzer A.G., Scientific Publishing Company 1990 |
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| title_short |
Transient fieldg-factor measurement of the first $ 3^{−} $ state $ in^{144} $Sm |
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https://doi.org/10.1007/BF02401207 |
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Brandolini, F. Löwenich, K. Pavan, P. Alvarez, C. Rossi De Poli, M. Haque, A. M. I. |
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Brandolini, F. Löwenich, K. Pavan, P. Alvarez, C. Rossi De Poli, M. Haque, A. M. I. |
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10.1007/BF02401207 |
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2024-07-04T03:11:34.632Z |
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