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Published bySophie Mills Modified over 8 years ago
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Claudia Ambrosch-Draxl Institute for Theoretical Physics University Graz claudia.ambrosch@uni-graz.at Forces and Phonons within WIEN2k
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Outline Forces in WIEN2k Atomic Forces Geometry optimization The frozen phonon approach The Hellmann-Feynman theorem Forces within density functional theory Pulay corrections Phonons Computational effort Examples Molecular Dynamics Inputs Limitations
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The Frozen Phonon Approach fit: harmonic case:
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Frozen Phonon Approach atomic forces: 3N degrees of freedom N atoms: i=1,....,N force constants: dynamical martrix: general case:
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The Hellmann-Feynman Force Many particle Schrödinger equation Many particle system electronic coordinatesionic coordinates groundstate wavefunction with respect to fixed ions Hellmann-Feynman theorem
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The Hellmann-Feynman Force Hellmann-Feynman force: total classical Coulomb force acting on the nucleus stemming from all other charges of the system = electrostatic force stemming from all other nuclei + electrostatic force stemming from the electronic charges Many particle system component of the electric field caused by the nuclear charge
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Forces in DFT Atomic force: Pulay corrections Total energy:
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Forces in the LAPW Method
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point mode in Si Example
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Computational Effort
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Example: YBa 2 Cu 3 O 7 yttrium barium copper oxygen Lattice Vibrations
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Raman Active Phonons YBa 2 Cu 3 O 7
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Example: YBa 2 Cu 3 O 7 Lattice Vibrations oxygen modes Ba / Cu modes
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