Gajewski Grzegorz, Mitev Pavlin D, Hermansson Kersti
Materials Chemistry, The Angstrom Laboratory, Uppsala University, Box 538, S-75121 Uppsala, Sweden.
J Chem Phys. 2008 Aug 14;129(6):064502. doi: 10.1063/1.2913518.
Anharmonic vibrational frequencies for the Raman-active (A(1g)) and the IR-active (A(2u)) modes have been calculated for the LiOH crystal within a plane-wave density functional theory (DFT) framework. We find that a two-dimensional quantum-mechanical vibrational approach, allowing for anharmonic coupling between symmetric and antisymmetric OH stretching modes, produces OH frequencies--both absolute frequencies and gas-to-solid frequency shifts--in good agreement with experiment. Remaining errors in the absolute frequencies are largely a consequence of the DFT model chosen. A one-dimensional normal-mode following vibrational treatment, on the other hand, fails to reproduce both absolute anharmonic frequencies and gas-to-solid frequency shifts.
在平面波密度泛函理论(DFT)框架内,计算了LiOH晶体中拉曼活性(A(1g))和红外活性(A(2u))模式的非谐振动频率。我们发现,二维量子力学振动方法考虑了对称和反对称OH伸缩模式之间的非谐耦合,所产生的OH频率——包括绝对频率和气-固频率偏移——与实验结果吻合良好。绝对频率中存在的剩余误差在很大程度上是所选DFT模型的结果。另一方面,一维简正模式跟踪振动处理无法再现绝对非谐频率和气-固频率偏移。