| Pramana | |
| Effect of polarization on population transfer in H2 by stimulated Raman transition with partially overlapping laser pulses | |
| Samir Saha1  S S Bhattacharyya1  Sanjay Sen1  Swaralipi Ghosh1  | |
| [1] Atomic and Molecular Physics Section, Department of Materials Science, Indian Association for the Cultivation of Science, Jadavpur, Calcutta 700 032, India$$ | |
| 关键词: Population transfer; polarization effects; stimulated Raman transition.; | |
| DOI : | |
| 学科分类:物理(综合) | |
| 来源: Indian Academy of Sciences | |
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【 摘 要 】
Polarization effects on population transfer by stimulated Raman transition using overlapping time dependent pump and Stokes laser pulses from the ground ð‘‹1$ð›´^{+}_{g}$(ð‘£g=0,ð½g=1) level of H2 to the ï¬nal ð‘‹1$ð›´^{+}_{g}$(ð‘£f=1,ð½f=1) level via the intermediate ðµ1$ð›´^{+}_{u}(ð‘£i=14,ð½i=0,2), ð¶1$ð›±^{+}_{u}$(ð‘£i=3,ð½i=2) and ð¶1$ð›±^{-}_{u}$(ð‘£i=3,ð½i=1) levels have been theoretically investigated by applying the density matrix formalism. We have studied in detail the dependence of the population transfer on time delay between two pulses for the cases of on-resonance excitations considering linear parallel and same-sense circular polarizations of the ï¬elds. The pump and Stokes ï¬elds are taken as having Gaussian pulse shapes with peak intensities $I^{0}_{P}(I^{0}_{S})$=2 × 106 and 1 × 107 W/cm2. Density matrix equations have been solved for each value of the magnetic quantum number ð‘€g(0,± 1)$ of the initial ground level taking into account the ð‘€g dependence of the Rabi frequencies. ð‘€g – averaged population transfer to the ï¬nal level has also been calculated. For resonance excitations to the ðµ(14, 0) or ð¶(3,1) levels, appreciable population transfer is achieved for intuitive pulse order for some particular values of ð‘€g and ð‘€i (magnetic quantum number of the resonant intermediate level) depending on the nature of polarizations. The calculated values of ð‘€g – averaged population transfer for the two cases of polarizations show that for on-resonance excitation to the ðµ(14, 0) or the ð¶(3, 1) level, linear parallel polarization of the laser ï¬elds yield more transfer efï¬ciency whereas for resonance excitation to the ðµ(14, 2) level, larger population transfer results from the same-sense circular polarizations. For resonance excitation to the ð¶(3, 2) level, ð‘€g – averaged population is found to be almost polarization independent. The calculations for the six-level H2 system reveal some interesting features of polarization effects on the population transfer efï¬ciency
【 授权许可】
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【 预 览 】
| Files | Size | Format | View |
|---|---|---|---|
| RO201912040495621ZK.pdf | 281KB |
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