Department of Physics, Harvard University, Cambridge, MA 02138;
Department of Chemistry and Chemical Biology, Harvard University, Cambridge, MA 02138.
Proc Natl Acad Sci U S A. 2019 Sep 10;116(37):18316-18321. doi: 10.1073/pnas.1908624116. Epub 2019 Aug 23.
Within a tight-binding approximation, we numerically determine the time evolution of graphene electronic states in the presence of classically vibrating nuclei. There is no reliance on the Born-Oppenheimer approximation within the p-orbital tight-binding basis, although our approximation is "atomically adiabatic": the basis p-orbitals are taken to follow nuclear positions. Our calculations show that the strict adiabatic Born-Oppenheimer approximation fails badly. We find that a diabatic (lazy electrons responding weakly to nuclear distortions) Born-Oppenheimer model provides a much more accurate picture and suggests a generalized many-body Bloch orbital-nuclear basis set for describing electron-phonon interactions in graphene.
在紧束缚近似下,我们数值地确定了在经典振动核存在下石墨烯电子态的时间演化。虽然在 p 轨道紧束缚基中不依赖 Born-Oppenheimer 近似,但我们的近似是“原子绝热的”:基 p 轨道被认为跟随核位置。我们的计算表明,严格的绝热 Born-Oppenheimer 近似严重失效。我们发现,非绝热(电子对核变形的响应较弱)Born-Oppenheimer 模型提供了更准确的图像,并提出了广义多体 Bloch 轨道-核基组,用于描述石墨烯中的电子-声子相互作用。