Electron-impact coherence parameters for electron-impact excitation of laser-excited 174Yb (... 6s6p 3P1)
We have measured and calculated the P3 collision Stokes parameter for electron-impact collisional de-excitation to the ytterbium (…6s6p 3P1) level from the higher-lying 1P1, 3D1, 2, 3 and 3S1 levels for 20 eV residual energy. These processes are the time-reverse of the experimentally measured proces...
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| Hauptverfasser: | , , , , , , , , |
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| Dokumenttyp: | Article (Journal) |
| Sprache: | Englisch |
| Veröffentlicht: |
16 March 2011
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| In: |
Journal of physics. B, Atomic, molecular and optical physics
Year: 2011, Jahrgang: 44, Heft: 7, Pages: 1-7 |
| ISSN: | 1361-6455 |
| DOI: | 10.1088/0953-4075/44/7/075201 |
| Online-Zugang: | Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1088/0953-4075/44/7/075201
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| Verfasserangaben: | J.D. Hein, S. Kidwai, P.W. Zetner, C. Bostock, D.V. Fursa, I. Bray, L. Sharma, R. Srivastava and A. Stauffer |
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| 245 | 1 | 0 | |a Electron-impact coherence parameters for electron-impact excitation of laser-excited 174Yb (... 6s6p 3P1) |c J.D. Hein, S. Kidwai, P.W. Zetner, C. Bostock, D.V. Fursa, I. Bray, L. Sharma, R. Srivastava and A. Stauffer |
| 246 | 3 | 3 | |a Electron-impact coherence parameters for electron-impact excitation of laser-excited 174 Yb (... 6s6p 3 P 1) |
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| 520 | |a We have measured and calculated the P3 collision Stokes parameter for electron-impact collisional de-excitation to the ytterbium (…6s6p 3P1) level from the higher-lying 1P1, 3D1, 2, 3 and 3S1 levels for 20 eV residual energy. These processes are the time-reverse of the experimentally measured processes, where an impact energy of 20 eV was used to collisionally excite the 3P1 target, prepared by resonant laser pumping. Measurements were performed using a crossed-beam apparatus, where excited-state atomic targets were produced using resonant laser radiation incident on the electron-atom interaction region. Calculations were performed in the relativistic convergent close-coupling, convergent close-coupling and relativistic distorted-wave approximations. The theoretical calculations show that the h electron-impact coherence parameter (EICP) is equal to 1/2, independent of the scattering angle. We use this result to present the L⊥ EICP for the (…6s7s 3S1)→(…6s6p 3P1) collision process. | ||
| 700 | 1 | |a Kidwai, S. |e VerfasserIn |4 aut | |
| 700 | 1 | |a Zetner, P. W. |e VerfasserIn |4 aut | |
| 700 | 1 | |a Bostock, C. |e VerfasserIn |4 aut | |
| 700 | 1 | |a Fursa, D. V. |e VerfasserIn |4 aut | |
| 700 | 1 | |a Bray, I. |e VerfasserIn |4 aut | |
| 700 | 1 | |a Sharma, Lalita |e VerfasserIn |0 (DE-588)1269427490 |0 (DE-627)1817962914 |4 aut | |
| 700 | 1 | |a Srivastava, R. |e VerfasserIn |4 aut | |
| 700 | 1 | |a Stauffer, A. |e VerfasserIn |4 aut | |
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