首页> 外文期刊>Journal of Physics. Condensed Matter >Analysis of (F-7(0))Gamma(1g) -> (D-5(2))Gamma(5g), Gamma(3g) and (F-7(0))Gamma(1g) -> (L-5(6))Gamma(1g), a Gamma(5g) two-photon absorption spectra of Cs2NaYF6 : Eu3+
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Analysis of (F-7(0))Gamma(1g) -> (D-5(2))Gamma(5g), Gamma(3g) and (F-7(0))Gamma(1g) -> (L-5(6))Gamma(1g), a Gamma(5g) two-photon absorption spectra of Cs2NaYF6 : Eu3+

机译:分析(F-7(0))Gamma(1g)->(D-5(2))Gamma(5g),Gamma(3g)和(F-7(0))Gamma(1g)->(L -5(6))Gamma(1g),Cs2NaYF6:Eu3 +的Gamma(5g)双光子吸收光谱

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摘要

The direct calculation of transition line strengths and relative intensities is presented for two intraconfigurational two-photon absorption (TPA) transitions of Eu3+ in the cubic Cs2NaYF6 host. Crystal field wavefunctions were utilized for the initial and final f(N)-clectron states and various approaches were used in constructing all the 4f(N-1) 5d(1) intermediate-state wavefunctions. The calculated relative intensities of the (F-7(0)) Gamma(1g) --> (D-5(2))Gamma(5g), Gamma(3g) TPA transitions are in reasonable agreement with experiment. The neglect of J-mixing in the initial state has only a small effect upon the calculation, whereas the neglect of spin-orbit couplings within the initial and terminal states drastically reduces the calculated transition linestrengths, but does not markedly change the intensity ratios. In the case of the (F-7(0))Gamma(1g) --> (F-5(6))Gamma(1g), aGamma(5g) transitions, serious discrepancies between experiment and theory are found if the intermediate states are constructed from a 4f(5) core comprising free ion states and the 5d(1) crystal field states. Satisfactory agreement is, however, found when the 4f(5) crystal field states are utilized in constructing the intermediate states. The contributions to the transition moment have been evaluated for various Hamiltonian terms and the results are discussed. [References: 23]
机译:给出了立方Cs2NaYF6主体中Eu3 +的两个构内双光子吸收(TPA)跃迁的跃迁线强度和相对强度的直接计算。晶体场波函数被用于初始和最终f(N)-电子态,并使用各种方法来构建所有4f(N-1)5d(1)中间态波函数。 (F-7(0))Gamma(1g)->(D-5(2))Gamma(5g),Gamma(3g)TPA跃迁的计算相对强度与实验合理吻合。忽略初始状态下的J混合对计算的影响很小,而忽略初始状态和末端状态内的自旋轨道耦合会大大降低计算出的过渡线强度,但不会明显改变强度比。在[F-7(0))Gamma(1g)->(F-5(6))Gamma(1g),aGamma(5g)跃迁的情况下,如果中间产物被发现存在实验与理论之间的严重差异由包含自由离子态和5d(1)晶场态的4f(5)核构造态。但是,当利用4f(5)晶体场态构建中间态时,发现令人满意的一致性。已经评估了各种哈密顿量项对过渡力矩的贡献,并讨论了结果。 [参考:23]

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