Internal magnetic hyperfine fields at Hf nuclei in iron, cobalt and nickel hosts
Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Aggarwal, N. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1983 |
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| Schlagwörter: |
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| Anmerkung: |
© J.C. Baltzer Scientific Publishing Company 1983 |
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| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 13(1983), 1-3 vom: Jan., Seite 271-274 |
|---|---|
| Übergeordnetes Werk: |
volume:13 ; year:1983 ; number:1-3 ; month:01 ; pages:271-274 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF01027257 |
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| 520 | |a Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. | ||
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| 700 | 1 | |a Bedi, S. C. |4 aut | |
| 700 | 1 | |a Hans, H. S. |4 aut | |
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10.1007/BF01027257 doi (DE-627)OLC2076337660 (DE-He213)BF01027257-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Aggarwal, N. verfasserin aut Internal magnetic hyperfine fields at Hf nuclei in iron, cobalt and nickel hosts 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer Scientific Publishing Company 1983 Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. Iron Magnetic Field Nickel Thin Film Cobalt Singh, B. aut Bhati, A. K. aut Bala, Renu aut Bedi, S. C. aut Hans, H. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 13(1983), 1-3 vom: Jan., Seite 271-274 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:13 year:1983 number:1-3 month:01 pages:271-274 https://doi.org/10.1007/BF01027257 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_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 13 1983 1-3 01 271-274 |
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10.1007/BF01027257 doi (DE-627)OLC2076337660 (DE-He213)BF01027257-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Aggarwal, N. verfasserin aut Internal magnetic hyperfine fields at Hf nuclei in iron, cobalt and nickel hosts 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer Scientific Publishing Company 1983 Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. Iron Magnetic Field Nickel Thin Film Cobalt Singh, B. aut Bhati, A. K. aut Bala, Renu aut Bedi, S. C. aut Hans, H. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 13(1983), 1-3 vom: Jan., Seite 271-274 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:13 year:1983 number:1-3 month:01 pages:271-274 https://doi.org/10.1007/BF01027257 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_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 13 1983 1-3 01 271-274 |
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10.1007/BF01027257 doi (DE-627)OLC2076337660 (DE-He213)BF01027257-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Aggarwal, N. verfasserin aut Internal magnetic hyperfine fields at Hf nuclei in iron, cobalt and nickel hosts 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer Scientific Publishing Company 1983 Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. Iron Magnetic Field Nickel Thin Film Cobalt Singh, B. aut Bhati, A. K. aut Bala, Renu aut Bedi, S. C. aut Hans, H. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 13(1983), 1-3 vom: Jan., Seite 271-274 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:13 year:1983 number:1-3 month:01 pages:271-274 https://doi.org/10.1007/BF01027257 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_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 13 1983 1-3 01 271-274 |
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10.1007/BF01027257 doi (DE-627)OLC2076337660 (DE-He213)BF01027257-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Aggarwal, N. verfasserin aut Internal magnetic hyperfine fields at Hf nuclei in iron, cobalt and nickel hosts 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer Scientific Publishing Company 1983 Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. Iron Magnetic Field Nickel Thin Film Cobalt Singh, B. aut Bhati, A. K. aut Bala, Renu aut Bedi, S. C. aut Hans, H. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 13(1983), 1-3 vom: Jan., Seite 271-274 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:13 year:1983 number:1-3 month:01 pages:271-274 https://doi.org/10.1007/BF01027257 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_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 13 1983 1-3 01 271-274 |
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10.1007/BF01027257 doi (DE-627)OLC2076337660 (DE-He213)BF01027257-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Aggarwal, N. verfasserin aut Internal magnetic hyperfine fields at Hf nuclei in iron, cobalt and nickel hosts 1983 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © J.C. Baltzer Scientific Publishing Company 1983 Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. Iron Magnetic Field Nickel Thin Film Cobalt Singh, B. aut Bhati, A. K. aut Bala, Renu aut Bedi, S. C. aut Hans, H. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 13(1983), 1-3 vom: Jan., Seite 271-274 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:13 year:1983 number:1-3 month:01 pages:271-274 https://doi.org/10.1007/BF01027257 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_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4323 33.00 VZ AR 13 1983 1-3 01 271-274 |
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internal magnetic hyperfine fields at hf nuclei in iron, cobalt and nickel hosts |
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Internal magnetic hyperfine fields at Hf nuclei in iron, cobalt and nickel hosts |
| abstract |
Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. © J.C. Baltzer Scientific Publishing Company 1983 |
| abstractGer |
Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. © J.C. Baltzer Scientific Publishing Company 1983 |
| abstract_unstemmed |
Abstract Integral perturbed angular correlation technique has been used to measure the internal hyperfine magnetic fields at Hf nuclei in Fe, Co and Ni matrices. These represent a consistent set of measurements with diffused sources. The 9+/2 (208 keV) 9−/2 (113 keV) 7−/2 cascade in the decay $ of^{177} $Lu→177Hf was used for measurements. The results obtained are:$$\begin{gathered} H_{Fe}^{Hf} = - 266 \pm 47 kG, \hfill \\ H_{Co}^{Hf} = - 116 \pm 18 kG, \hfill \\ H_{Ni}^{Hf} = - 118 \pm 26 kG. \hfill \\ \end{gathered} $$ These measurements are compared with previous results and discussed in terms of methods of source preparation. © J.C. Baltzer Scientific Publishing Company 1983 |
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| title_short |
Internal magnetic hyperfine fields at Hf nuclei in iron, cobalt and nickel hosts |
| url |
https://doi.org/10.1007/BF01027257 |
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false |
| author2 |
Singh, B. Bhati, A. K. Bala, Renu Bedi, S. C. Hans, H. S. |
| author2Str |
Singh, B. Bhati, A. K. Bala, Renu Bedi, S. C. Hans, H. S. |
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| doi_str |
10.1007/BF01027257 |
| up_date |
2024-07-04T03:08:25.242Z |
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