Dieter Vollhardt

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Dieter Vollhardt (born September 8, 1951) is a German physicist and Professor of Theoretical Physics at the University of Augsburg.

Scientific work[edit]

Vollhardt is one of the founders of the Dynamical Mean-Field Theory (DMFT) for strongly correlated electronic solids such as transition metals (e.g. iron or vanadium) and their oxides, i.e. materials with electrons in open d- and f-shells. The properties of these systems are determined by the Coulomb repulsion between the electrons which makes these electrons strongly correlated. The repulsion has the tendency to localize electrons. This leads to a multitude of phenomena such as the Mott-Hubbard metal insulator transition. Conventional band theory or density functional theory cannot describe these systems adequately. In 1989 Vollhardt and his doctoral student Walter Metzner introduced electronic models with local interaction (Hubbard model) on a lattice with infinitely many nearest neighbors,[1] which Gabriel Kotliar and Antoine Georges[2] then developed into the DMFT.[3] The DMFT may be viewed as a self-consistent, field-theoretical generalization of a quantum impurity model by Philip W. Anderson, where the mean-field describes the coupling of the impurity to an "electronic bath".

DMFT provides an exact description of the quantum dynamics of correlated lattice systems with local interaction, but neglects spatial correlations. It has provided fundamental insights into the properties of correlated electronic systems. The combination of the DMFT with material-specific approaches, such as the "Local Density Approximation" (LDA) to the density functional theory, led to a new computational scheme, often referred to as LDA+DMFT, for the investigation of strongly correlated materials.[4][5][6]

Selected awards[edit]

Selected publications[edit]

  • Dynamical mean-field theory for correlated electrons (Einstein Lecture), Ann. Phys. (Berlin), 524, 1 (2012) doi:10.1002/andp.201100250
  • with Gabriel Kotliar, Strongly correlated materials: Insights from dynamical mean field theory, Physics Today 57, No. 3 (March), 53 (2004)
  • Strong-coupling approaches to correlated Fermions, in: Enrico Fermi Course 121, Broglia, Schrieffer (ed.), North Holland 1994
  • with Peter Wölfle, Superfluid Phases of Helium 3, Taylor and Francis 1990, corrected reprint by Dover Publications 2013
  • Normal 3He: An Almost Localized Fermi-Liquid, Reviews of Modern Physics 56, 99 (1984) doi:10.1103/RevModPhys.56.99
  • with Peter Wölfle, A Diagrammic, Self-Consistent Treatment of the Anderson Localization Problem in d ≤ 2 Dimensions, Physical Review B 22, 4666 (1980) doi:10.1103/PhysRevB.22.4666

External links[edit]

References[edit]

  1. ^ Metzner, Walter (1989). "Correlated Lattice Fermions in d = ∞ Dimensions". Physical Review Letters. 62 (3): 324–327. Bibcode:1989PhRvL..62..324M. doi:10.1103/PhysRevLett.62.324. PMID 10040203.
  2. ^ Georges, Antoine (1992). "Hubbard model in infinite dimensions". Physical Review B. 45 (12): 6479–6483. doi:10.1103/PhysRevB.45.6479.
  3. ^ Georges, Antoine (1996). "Dynamical mean-field theory of strongly correlated fermion systems and the limit of infinite dimensions". Reviews of Modern Physics. 68 (1): 13–125. Bibcode:1996RvMP...68...13G. doi:10.1103/RevModPhys.68.13.
  4. ^ K. Held, I. A. Nekrasov, G. Keller, V. Eyert, N. Blümer, A. K. McMahan, R. T. Scalettar, T. Pruschke, V. I. Anisimov, D. Vollhardt, Psi-k Newsletter No. 56 (April 2003), p. 65
  5. ^ Georges, Antoine (1996). "Dynamical mean-field theory of strongly correlated fermion systems and the limit of infinite dimensions". Reviews of Modern Physics. 68 (1): 13–125. Bibcode:1996RvMP...68...13G. doi:10.1103/RevModPhys.68.13.
  6. ^ The LDA+DMFT approach to strongly correlated materials, Lecture Notes of the Autumn School 2011 Hands-on LDA+DMFT, Editors: E. Pavarini, E. Koch, D. Vollhardt, A. Lichtenstein, Forschungszentrum Jülich (2011)