Implementation of the projector augmented-wave method in the ABINIT code: Application to the study of iron under pressure
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Xavier Gonze | G. Zerah | F. Jollet | François Bottin | Marc Torrent | X. Gonze | F. Jollet | M. Torrent | F. Bottin | G. Zérah
[1] G. E. Matthews,et al. Comparison of the Projector Augmented-Wave, Pseudopotential, and Linearized Augmented- Plane-Wave Formalisms for Density-Functional Calculations of Solids , 1997 .
[2] Lee,et al. Car-Parrinello molecular dynamics with Vanderbilt ultrasoft pseudopotentials. , 1993, Physical review. B, Condensed matter.
[3] Xavier Gonze,et al. A brief introduction to the ABINIT software package , 2005 .
[4] M. Torrent,et al. Quasihydrostatic equation of state of iron above 2 Mbar. , 2006, Physical review letters.
[5] Cohen,et al. Iron at high pressure: Linearized-augmented-plane-wave computations in the generalized-gradient approximation. , 1994, Physical review. B, Condensed matter.
[6] Stefan Goedecker,et al. An efficient 3-dim FFT for plane wave electronic structure calculations on massively parallel machines composed of multiprocessor nodes , 2003 .
[7] G. Kresse,et al. From ultrasoft pseudopotentials to the projector augmented-wave method , 1999 .
[8] Blöchl,et al. Projector augmented-wave method. , 1994, Physical review. B, Condensed matter.
[9] B. Johansson,et al. Stability of the body-centered-tetragonal phase of fe at high pressure : Ground-state energies, phonon spectra, and molecular dynamics simulations , 2006 .
[10] G. E. Matthews,et al. A Projector Augmented Wave (PAW) code for electronic structure calculations, Part II: Pwpaw for periodic solids in a plane wave basis , 2001 .
[11] H. Mao,et al. Static compression of iron to 300 GPa and Fe(0.8)Ni(0.2) alloy to 260 GPa - Implications for composition of the core , 1990 .
[12] Xavier Gonze,et al. Projector augmented-wave approach to density-functional perturbation theory , 2006 .
[13] G. E. Matthews,et al. A Projector Augmented Wave (PAW) code for electronic structure calculations, Part I: atompaw for generating atom-centered functions , 2001 .
[14] H. Monkhorst,et al. SPECIAL POINTS FOR BRILLOUIN-ZONE INTEGRATIONS , 1976 .
[15] Alessandro Curioni,et al. Dual-level parallelism for ab initio molecular dynamics: Reaching teraflop performance with the CPMD code , 2005, Parallel Comput..
[16] A. Cracknell,et al. The mathematical theory of symmetry in solids;: Representation theory for point groups and space groups, , 1972 .
[17] Peter M. Bell,et al. Static compression of iron to 78 GPa with rare gas solids as pressure-transmitting media , 1986 .
[18] M. A. Blanco,et al. Evaluation of the rotation matrices in the basis of real spherical harmonics , 1997 .
[19] Andrew V. Knyazev,et al. Toward the Optimal Preconditioned Eigensolver: Locally Optimal Block Preconditioned Conjugate Gradient Method , 2001, SIAM J. Sci. Comput..
[20] Paxton,et al. High-precision sampling for Brillouin-zone integration in metals. , 1989, Physical review. B, Condensed matter.
[21] Martin,et al. Quantum-mechanical theory of stress and force. , 1985, Physical review. B, Condensed matter.
[22] Matthieu Verstraete,et al. First-principles computation of material properties: the ABINIT software project , 2002 .
[23] G. Steinle-Neumann,et al. First-principles elastic constants for the hcp transition metals Fe, Co, and Re at high pressure (vol 60, pg 791, 1999) , 1999 .
[24] Burke,et al. Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.
[25] D. Vanderbilt,et al. Soft self-consistent pseudopotentials in a generalized eigenvalue formalism. , 1990, Physical review. B, Condensed matter.