g-factor of the first excited $ 4^{+} $ states $ in^{156} $Gd $ and^{158} $Gd
Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed v...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bazzacco, D. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1990 |
|---|
| Schlagwörter: |
|---|
| Anmerkung: |
© J.C. Baltzer A.G., Scientific Publishing Company 1990 |
|---|
| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 59(1990), 1-4 vom: Aug., Seite 125-128 |
|---|---|
| Übergeordnetes Werk: |
volume:59 ; year:1990 ; number:1-4 ; month:08 ; pages:125-128 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF02401205 |
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OLC2076363203 |
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| 520 | |a Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. | ||
| 650 | 4 | |a Thin Film | |
| 650 | 4 | |a Gadolinium | |
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| 650 | 4 | |a Field Technique | |
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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/BF02401205 doi (DE-627)OLC2076363203 (DE-He213)BF02401205-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut g-factor of the first excited $ 4^{+} $ states $ in^{156} $Gd $ and^{158} $Gd 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. Thin Film Gadolinium Rotational Model Field Technique Rotational Alignment 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 125-128 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:125-128 https://doi.org/10.1007/BF02401205 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 08 125-128 |
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10.1007/BF02401205 doi (DE-627)OLC2076363203 (DE-He213)BF02401205-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut g-factor of the first excited $ 4^{+} $ states $ in^{156} $Gd $ and^{158} $Gd 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. Thin Film Gadolinium Rotational Model Field Technique Rotational Alignment 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 125-128 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:125-128 https://doi.org/10.1007/BF02401205 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 08 125-128 |
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10.1007/BF02401205 doi (DE-627)OLC2076363203 (DE-He213)BF02401205-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut g-factor of the first excited $ 4^{+} $ states $ in^{156} $Gd $ and^{158} $Gd 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. Thin Film Gadolinium Rotational Model Field Technique Rotational Alignment 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 125-128 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:125-128 https://doi.org/10.1007/BF02401205 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 08 125-128 |
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10.1007/BF02401205 doi (DE-627)OLC2076363203 (DE-He213)BF02401205-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut g-factor of the first excited $ 4^{+} $ states $ in^{156} $Gd $ and^{158} $Gd 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. Thin Film Gadolinium Rotational Model Field Technique Rotational Alignment 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 125-128 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:125-128 https://doi.org/10.1007/BF02401205 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 08 125-128 |
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10.1007/BF02401205 doi (DE-627)OLC2076363203 (DE-He213)BF02401205-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Bazzacco, D. verfasserin aut g-factor of the first excited $ 4^{+} $ states $ in^{156} $Gd $ and^{158} $Gd 1990 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer A.G., Scientific Publishing Company 1990 Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. Thin Film Gadolinium Rotational Model Field Technique Rotational Alignment 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 125-128 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:59 year:1990 number:1-4 month:08 pages:125-128 https://doi.org/10.1007/BF02401205 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 08 125-128 |
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| title_auth |
g-factor of the first excited $ 4^{+} $ states $ in^{156} $Gd $ and^{158} $Gd |
| abstract |
Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. © J.C. Baltzer A.G., Scientific Publishing Company 1990 |
| abstractGer |
Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. © J.C. Baltzer A.G., Scientific Publishing Company 1990 |
| abstract_unstemmed |
Abstract Relative g-factor of the first $ 2^{+} $ and $ 4^{+} $ states have been measured with the transient field technique $ in^{156} $Gd $ and^{158} $Gd. The precession of gamma rays depopulating the levels under study were observed, after passing through thin polarized gadolinium. The observed values agree with the predictions of the rotational model, i.c. g($ 4^{+} $)= g($ 2^{+} $), while contrasting the hypothesis that $ in^{156} $Gd the g-factor of the $ 4^{+} $ is reduced with respect to the $ 2^{+} $, because of rotational alignment. © J.C. Baltzer A.G., Scientific Publishing Company 1990 |
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| container_issue |
1-4 |
| title_short |
g-factor of the first excited $ 4^{+} $ states $ in^{156} $Gd $ and^{158} $Gd |
| url |
https://doi.org/10.1007/BF02401205 |
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| author2 |
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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| doi_str |
10.1007/BF02401205 |
| up_date |
2024-07-04T03:11:34.793Z |
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