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ELECTRON-PHONON INTERACTIONS IN CSCDBR3-YB3+

机译:CSCDBR3-YB3 +中的电子声子相互作用

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Pronounced electron-phonon coupling is observed for the F-2(7/2)<->F-2(5/2) 4f transitions of Yb3+ doped into CsCdBr3. A comparison of the Raman spectrum and the luminescence excitation sideband accompanying the F-2(7/2)(0)-->F-2(5/2)(2') crystal-field transition reveals vibrational properties of the [YbBr6] coordination unit that differ markedly from those of the CsCdBr3 host. In particular, the vibronic transition associated with the totally symmetric [YbBr6] stretching mode appears as a very weak feature at 191 cm(-1) in the Raman spectrum, whereas the totally symmetric [CdBr6] stretching mode of the CsCdBr3 bulk, which appears as a strong feature at 162.5 cm(-1) in the Raman spectrum, is only weakly discernible In the sideband. This is direct evidence for a large contribution from [YbBr6] local modes and a small contribution from bulk modes to the vibronic intensity. The intensity of the local mode is enhanced by approximately a factor of 2 in the Raman spectrum when the laser is tuned into resonance with the F-2(7/2)(0)-->F-2(5/2)(2') absorption of Yb3+, providing direct confirmation of its assignment. The observation of the first and second members of a Franck-Condon progression for both the local and the bulk totally symmetric modes indicates that a Delta process, rather than an M process, induces the vibronic intensity. Huang-Rhys factors of S-local=0.010+/-0.002 and S-bulk=0.15+/-0.03 were determined from the data, and reflect quite different electron-phonon coupling strengths. These results suggest that multiphonon relaxation of excited electronic states proceeds by the excitation of local modes of [YbBr6] followed by energy transfer to bulk modes of the lattice, possibly through a nonlinear coupling mechanism which is discussed briefly. (C) 1997 American Institute of Physics. [References: 39]
机译:对于掺杂到CsCdBr3中的Yb3 +的F-2(7/2)→F-2(5/2)4f跃迁,观察到明显的电子-声子耦合。拉曼光谱和伴随F-2(7/2)(0)-> F-2(5/2)(2')晶体场跃迁的发光激发边带的比较揭示了[YbBr6 ]协调单元,与CsCdBr3宿主的协调单元明显不同。特别是,与完全对称[YbBr6]拉伸模式相关的振动跃迁在拉曼光谱中的191 cm(-1)处显示为非常弱的特征,而CsCdBr3本体的完全对称[CdBr6]拉伸模式出现了作为拉曼光谱在162.5 cm(-1)的强特征,仅在边带中很难辨别。这直接证明了[YbBr6]局部模式的贡献很大,而体模对振动强度的贡献很小。当激光器被调谐到F-2(7/2)(0)-> F-2(5/2)()时,局部模式的强度在拉曼光谱中提高大约2倍。 2')吸收Yb3 +,直接确认其分配。对局部和整体完全对称模式的弗兰克-康登级数的第一和第二个成员的观察表明,Delta过程而不是M过程会诱发振动强度。由数据确定了S-local = 0.010 +/- 0.002和S-bulk = 0.15 +/- 0.03的Huang-Rhys因子,它们反映了截然不同的电子-声子耦合强度。这些结果表明,激发的电子态的多声子弛豫是通过激发[YbBr6]的局部模式,然后将能量转移到晶格的体模式而进行的,可能是通过简要讨论的非线性耦合机制进行的。 (C)1997美国物理研究所。 [参考:39]

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