Luo Wei, Ahuja Rajeev, Ding Yang, Mao Ho-kwang
Condensed Matter Theory Group, Department of Physics Box 530, SE-751 21 Uppsala, Sweden.
Proc Natl Acad Sci U S A. 2007 Oct 16;104(42):16428-31. doi: 10.1073/pnas.0707377104. Epub 2007 Oct 9.
The electronic structures and lattice dynamics of pressure-induced complex phase transitions [bcc --> hR1(110.5 degrees) --> distorted-hR1(108.2 degrees) --> bcc] in vanadium as a function of pressure up to 400 GPa have been investigated with an ab initio method using density functional perturbation theory (DFPT). At ambient pressure, the soft transverse acoustic phonon mode corresponding to Kohn anomaly appears at a wave vector q = 2k(F) along [xi00] Gamma --> H high symmetry direction. The nondegenerate transverse acoustic branches TA(1) on (110) and TA(2) on (001) show an exceptionally large split at high symmetry point N (0.5 0.5 0.0). The lattice dynamical instability starts at a pressure of 62 GPa (V/V(0) = 0.78, where V(0) is experimental volume of bcc-V at ambient conditions), derived by phonon softening that results in phase transition of bcc --> hR1 (alpha = 110.5 degrees). At compression around 130 GPa (V/V(0) = 0.67), the rhombohedral angle of hR1 phase changed to 108.2 degrees, and the electronic structure changed drastically. At even higher pressure, approximately 250 GPa (V/V(0) = 0.57), lattice dynamic calculations show that the bcc structure becomes stable again.
利用密度泛函微扰理论(DFPT)的从头算方法,研究了钒中压力诱导的复杂相变 [体心立方(bcc)→六方菱形(hR1,110.5°)→畸变六方菱形(hR1,108.2°)→体心立方] 的电子结构和晶格动力学,压力范围高达400 GPa。在常压下,对应于科恩反常的软横向声子模出现在沿[ξ00] Γ→H高对称方向的波矢q = 2k(F)处。(110)面上的非简并横向声子分支TA(1)和(001)面上的TA(2)在高对称点N(0.5 0.5 0.0)处显示出异常大的分裂。晶格动力学不稳定性始于62 GPa的压力(V/V(0) = 0.78,其中V(0)是常压下体心立方钒的实验体积),这是由声子软化导致的体心立方→六方菱形(α = 110.5°)相变引起的。在约130 GPa的压缩下(V/V(0) = 0.67),六方菱形hR1相的菱面体角变为108.2°,电子结构发生了剧烈变化。在更高的压力下,约250 GPa(V/V(0) = 0.57),晶格动力学计算表明体心立方结构再次变得稳定。