Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions
Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Little, A. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1980 |
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| Schlagwörter: |
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| Anmerkung: |
© North-Holland Publishing Company 1980 |
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| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 8(1980), 1-3 vom: Apr., Seite 3-18 |
|---|---|
| Übergeordnetes Werk: |
volume:8 ; year:1980 ; number:1-3 ; month:04 ; pages:3-18 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF01026853 |
|---|
| Katalog-ID: |
OLC2076334238 |
|---|
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| 245 | 1 | 0 | |a Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions |
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| 520 | |a Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. | ||
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| 700 | 1 | |a Hanna, S. S. |4 aut | |
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10.1007/BF01026853 doi (DE-627)OLC2076334238 (DE-He213)BF01026853-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Little, A. verfasserin aut Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © North-Holland Publishing Company 1980 Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. Excited State Charge State External Field Small Contribution Hyperfine Interaction Jain, H. C. aut Lazarus, S. M. aut Saylor, T. K. aut Triplett, B. B. aut Hanna, S. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 8(1980), 1-3 vom: Apr., Seite 3-18 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:8 year:1980 number:1-3 month:04 pages:3-18 https://doi.org/10.1007/BF01026853 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_2015 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 33.00 VZ AR 8 1980 1-3 04 3-18 |
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10.1007/BF01026853 doi (DE-627)OLC2076334238 (DE-He213)BF01026853-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Little, A. verfasserin aut Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © North-Holland Publishing Company 1980 Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. Excited State Charge State External Field Small Contribution Hyperfine Interaction Jain, H. C. aut Lazarus, S. M. aut Saylor, T. K. aut Triplett, B. B. aut Hanna, S. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 8(1980), 1-3 vom: Apr., Seite 3-18 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:8 year:1980 number:1-3 month:04 pages:3-18 https://doi.org/10.1007/BF01026853 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_2015 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 33.00 VZ AR 8 1980 1-3 04 3-18 |
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10.1007/BF01026853 doi (DE-627)OLC2076334238 (DE-He213)BF01026853-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Little, A. verfasserin aut Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © North-Holland Publishing Company 1980 Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. Excited State Charge State External Field Small Contribution Hyperfine Interaction Jain, H. C. aut Lazarus, S. M. aut Saylor, T. K. aut Triplett, B. B. aut Hanna, S. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 8(1980), 1-3 vom: Apr., Seite 3-18 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:8 year:1980 number:1-3 month:04 pages:3-18 https://doi.org/10.1007/BF01026853 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_2015 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 33.00 VZ AR 8 1980 1-3 04 3-18 |
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10.1007/BF01026853 doi (DE-627)OLC2076334238 (DE-He213)BF01026853-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Little, A. verfasserin aut Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © North-Holland Publishing Company 1980 Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. Excited State Charge State External Field Small Contribution Hyperfine Interaction Jain, H. C. aut Lazarus, S. M. aut Saylor, T. K. aut Triplett, B. B. aut Hanna, S. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 8(1980), 1-3 vom: Apr., Seite 3-18 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:8 year:1980 number:1-3 month:04 pages:3-18 https://doi.org/10.1007/BF01026853 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_2015 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 33.00 VZ AR 8 1980 1-3 04 3-18 |
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10.1007/BF01026853 doi (DE-627)OLC2076334238 (DE-He213)BF01026853-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Little, A. verfasserin aut Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © North-Holland Publishing Company 1980 Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. Excited State Charge State External Field Small Contribution Hyperfine Interaction Jain, H. C. aut Lazarus, S. M. aut Saylor, T. K. aut Triplett, B. B. aut Hanna, S. S. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 8(1980), 1-3 vom: Apr., Seite 3-18 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:8 year:1980 number:1-3 month:04 pages:3-18 https://doi.org/10.1007/BF01026853 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_2015 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4305 GBV_ILN_4323 33.00 VZ AR 8 1980 1-3 04 3-18 |
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530 VZ 33.00 bkl Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions Excited State Charge State External Field Small Contribution Hyperfine Interaction |
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Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions |
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Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions |
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Little, A. |
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Hyperfine interactions |
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Hyperfine interactions |
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1980 |
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Little, A. Jain, H. C. Lazarus, S. M. Saylor, T. K. Triplett, B. B. Hanna, S. S. |
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calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions |
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Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions |
| abstract |
Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. © North-Holland Publishing Company 1980 |
| abstractGer |
Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. © North-Holland Publishing Company 1980 |
| abstract_unstemmed |
Abstract Magnetic hyperfine interactions in highly stripped oxygen ions recoiling in vacuum have been measured with perturbed angular correlations. The second excited state $ of^{16} $O(Iπ=$ 3^{−} $,EX=6.13 MeV, τ=26.6 psec, |g|=0.55) was produced with the nuclear $ reactions^{19} $F(p,α)16O $ and^{16} $O(α,α′)16O and the angular correlation of the γ-rays observed in coincidence with α particles emitted at 180°. Five recoil velocities between 1.0 and 3.3% c produced average ion charge states from 2.1 to 5.5. The perturbation of the angular correlation and hence the decoupling of the hyperfine interactions was observed as a function of an external axial magnetic field varied between 0 and 33 kG. The perturbation is expected to arise primarily from hyperfine interactions of unpaired 1s electrons with smaller contributions from 2s electrons and other configurations. The maximum external field was strong enough to decouple all hyperfine interactions except that of the 1s electrons. The decoupling curves obtained were successfully fitted by calculations using the hyperfine interactions of the pertinent atomic Hartree-Fock-Slater orbitals. © North-Holland Publishing Company 1980 |
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Calculation of hyperfine interactions measured by magnetic decoupling in oxygen ions |
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