The electronic structures and lattice dynamics of pressure-induced complex phase transitions [bcc 3 hR1(110.5°) 3 distortedhR1(108.2°) 3 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 [00] ⌫ 3 H high symmetry direction. The nondegenerate transverse acoustic branches TA 1 on ͗1 10͘ and TA2 on ͗001͘ 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 V0 is experimental volume of bcc-V at ambient conditions), derived by phonon softening that results in phase transition of bcc 3 hR1 (alpha ؍ 110.5°). At compression around 130 GPa (V/V 0 ؍ 0.67), the rhombohedral angle of hR1 phase changed to 108.2°, and the electronic structure changed drastically. At even higher pressure, Ϸ250 GPa (V/V 0 ؍ 0.57), lattice dynamic calculations show that the bcc structure becomes stable again.ab initio calculation ͉ phonon ͉ structure phase transition A vast number of extremely interesting and fundamental physical and chemical changes in solids have been reported in high-pressure experiments. The Kohn anomaly in bcc transition metals is considered to be one of the unsolved problems in the field of high-pressure structural phase transition. Kohn anomaly is characterized by electron-phonon features. Vanadium is an interesting case because this metal is one of the so-called hard superconductors (1) and it has been shown that the application of high pressure increases the superconducting temperature Tc (2, 3). The experimental phonon dispersion curves at ambient conditions in bcc phase using inelastic neutron scattering has been measured and for the longitudinal (111) branch it exhibits a dip near the (2/3 2/3 2/3) position (4). In another experiment by Page (5), a peak in the frequency distribution for vanadium is observed at 2 ϫ 10 12 c/s, and this peak is attributed to Kohn anomalies (5). As far as calculations are concerned, the lattice dynamics study of bcc vanadium at high pressure using a full-potential linear muffin-tin orbital (LMTO) method has been performed by Suzuki and Otani (3), and these calculations show a strong change of phonon density of states with volume at 130 GPa. It has been found that the transverse acoustic phonon mode TA [00] around ϭ 1/4 shows a dramatic softening under pressure and becomes imaginary at pressures Ͼ130 GPa, indicating the possibility of a structural phase transition. Landa et al. (6) have performed the elastic constants calculations for vanadium using exact muffin-tin orbital (EMTO) and shown the trigonal shear elastic constant (C44) softening at Ϸ200 GPa due to the intraband nesting of the Fermi surface (FS).Very recently, Ding et al. (7) performed the high-pressure experiment for bcc vanadium using diamond-anvil cell and synchrotron x-ray...