谷歌浏览器插件
订阅小程序
在清言上使用

Dynamic Jahn-Teller Interaction Withγ5phonons in the Ground State Ofcu2+

Physical review B, Condensed matter(1998)

引用 3|浏览0
暂无评分
摘要
Optical absorption and emission measurements of ${\mathrm{Cu}}^{2+}$ as a substitutional impurity in cubic ZnS and ZnTe are analyzed by means of an electron-phonon coupling model. The ${}^{2}D$ term of ${\mathrm{Cu}}^{2+}$ is split by a crystal field of tetrahedral symmetry into a ${}^{2}{\ensuremath{\Gamma}}_{5}$ orbital triplet and a ${}^{2}{\ensuremath{\Gamma}}_{3}$ orbital doublet. Optical transitions have been observed between these two multiplets in $\mathrm{ZnS}:{\mathrm{Cu}}^{2+}$ and within the ${}^{2}{\ensuremath{\Gamma}}_{5}$ ground state in $\mathrm{ZnTe}:{\mathrm{Cu}}^{2+}$. The theoretical model is based on crystal-field theory and includes the spin-orbit interaction and a dynamic Jahn-Teller interaction between the electronic ${}^{2}{\ensuremath{\Gamma}}_{5}$ states and a transverse acoustic phonon of ${\ensuremath{\Gamma}}_{5}$ symmetry. Starting from the ten spin-orbit wave functions appropriate to the orbital triplet and doublet manifolds, the symmetry-adapted vibronic basis is constructed and used to diagonalize the Hamiltonian matrix. Phonon overtones up to $n=14$ are included to ensure convergence of the energy eigenvalues. The measured positions and relative intensities of the spectral lines are described with good accuracy by the theoretical model, including covalency effects. In ZnS, comparison between theory and experiment yields the following values of the physical parameters: the crystal-field splitting $\ensuremath{\Delta}=5990.6$ ${\mathrm{cm}}^{\ensuremath{-}1}$, the spin-orbit coupling constants ${\ensuremath{\lambda}}_{1}=\ensuremath{-}667$ ${\mathrm{cm}}^{\ensuremath{-}1}$ and ${\ensuremath{\lambda}}_{2}=\ensuremath{-}830$ ${\mathrm{cm}}^{\ensuremath{-}1}$, the phonon energy $\ensuremath{\Elzxh}\ensuremath{\omega}=73.5$ ${\mathrm{cm}}^{\ensuremath{-}1}$, and the Jahn-Teller stabilization energy ${E}_{\mathrm{JT}}=474.5$ ${\mathrm{cm}}^{\ensuremath{-}1}$. The corresponding parameters in ZnTe are $\ensuremath{\Delta}=6000$ ${\mathrm{cm}}^{\ensuremath{-}1}$, ${\ensuremath{\lambda}}_{1}=\ensuremath{-}888$ ${\mathrm{cm}}^{\ensuremath{-}1}$, ${\ensuremath{\lambda}}_{2}=\ensuremath{-}830$ ${\mathrm{cm}}^{\ensuremath{-}1}$, $\ensuremath{\Elzxh}\ensuremath{\omega}=38.8$ ${\mathrm{cm}}^{\ensuremath{-}1}$, and ${E}_{\mathrm{JT}}=468.5$ ${\mathrm{cm}}^{\ensuremath{-}1}$.
更多
查看译文
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要