How many‐body perturbation theory (MBPT) has changed quantum chemistry

The history of many-body perturbation theory (MBPT) and its impact on Quantum Chemistry is reviewed, starting with Brueckner's conjecture of a linked-cluster expansion and the time-dependent derivation by Goldstone of such an expansion. A central part of this article is the time-independent formulation of quantum chemistry in Fock space and its diagrammatic representation including the particle-hole picture and the inversion of a commutator. The results of the time-independent derivation of MBPT are compared with those of Goldstone. It is analyzed which ingredients of Goldstone's approach are decisive. The connected diagram theorem is derived both in a constructive way based on a Lie-algebraic formulation and a nonconstructive way making use of the separation theorem. It is discussed why the Goldstone derivation starting from a unitary time-evolution operator, ends up with a wave operator in intermediate normalization. The Moller–Plesset perturbation expansions of Bartlett and Pople are compared. Examples of complete summations of certain classes of diagrams are discussed, for example, that which leads to the Bethe-Goldstone expansion. MBPT for energy differences is analyzed. The paper ends with recent developments and challenges, such as the generalization of normal ordering to arbitrary reference states, contracted Schrodinger k-particle equations and Brillouin conditions, and finally the Nakatsuji theorem and the Nooijen conjecture. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2009

[1]  D. Mukherjee,et al.  Use of a convenient size-extensive normalization in multi-reference coupled cluster (MRCC) theory with incomplete model space: A novel valence universal MRCC formulation , 2009 .

[2]  W. Kutzelnigg,et al.  Generalized Normal Ordering, Irreducible Brillouin Conditions, and Contracted Schrödinger Equations , 2007 .

[3]  Werner Kutzelnigg,et al.  Density-cumulant functional theory. , 2006, The Journal of chemical physics.

[4]  Piotr Piecuch,et al.  Intriguing accuracies of the exponential wave function expansions exploiting finite two-body correlation operators in calculations for many-electron systems , 2006 .

[5]  W. Kutzelnigg,et al.  Minimal parametrization of an n-electron state , 2005 .

[6]  W. Kutzelnigg,et al.  Irreducible Brillouin conditions and contracted Schrödinger equations for n-electron systems. IV. Perturbative analysis. , 2004, The Journal of chemical physics.

[7]  Debashis Mukherjee,et al.  Irreducible Brillouin conditions and contracted Schrödinger equations for n-electron systems. I. The equations satisfied by the density cumulants , 2001 .

[8]  Nooijen Can the eigenstates of a many-body hamiltonian Be represented exactly using a general two-body cluster expansion? , 2000, Physical review letters.

[9]  Koji Yasuda Direct determination of the quantum-mechanical density matrix: Parquet theory , 1999 .

[10]  Debashis Mukherjee,et al.  Cumulant expansion of the reduced density matrices , 1999 .

[11]  Werner Kutzelnigg,et al.  RELATIVISTIC ONE-ELECTRON HAMILTONIANS 'FOR ELECTRONS ONLY' AND THE VARIATIONAL TREATMENT OF THE DIRAC EQUATION , 1997 .

[12]  Debashis Mukherjee,et al.  Normal order and extended Wick theorem for a multiconfiguration reference wave function , 1997 .

[13]  Jeppe Olsen,et al.  Surprising cases of divergent behavior in Mo/ller–Plesset perturbation theory , 1996 .

[14]  Yasuda,et al.  Direct determination of the quantum-mechanical density matrix using the density equation. , 1996, Physical review letters.

[15]  Werner Kutzelnigg,et al.  Error analysis and improvements of coupled-cluster theory , 1991 .

[16]  W. Kutzelnigg,et al.  Time‐independent theory of one‐particle Green’s functions , 1989 .

[17]  R. Bartlett Coupled-cluster approach to molecular structure and spectra: a step toward predictive quantum chemistry , 1989 .

[18]  W. Kutzelnigg,et al.  Connected‐diagram expansions of effective Hamiltonians in incomplete model spaces. I. Quasicomplete and isolated incomplete model spaces , 1987 .

[19]  W. Kutzelnigg,et al.  Connected‐diagram expansions of effective Hamiltonians in incomplete model spaces. II. The general incomplete model space , 1987 .

[20]  W. Kutzelnigg Quantum chemistry in Fock space. IV. The treatment of permutational symmetry. Spin‐free diagrams with symmetrized vertices , 1985 .

[21]  Valdemoro Spin-adapted reduced Hamiltonian. I. Elementary excitations. , 1985, Physical review. A, General physics.

[22]  Werner Kutzelnigg,et al.  Quantum chemistry in Fock space. III. Particle‐hole formalism , 1984 .

[23]  W. Kutzelnigg,et al.  Quantum chemistry in Fock space. II. Effective Hamiltonians in Fock space , 1983 .

[24]  Werner Kutzelnigg,et al.  Quantum chemistry in Fock space. I. The universal wave and energy operators , 1982 .

[25]  W. Kutzelnigg Fock space perturbation theory , 1981 .

[26]  H. Monkhorst,et al.  Recursive scheme for order-by-order many-body perturbation theory , 1981 .

[27]  Werner Kutzelnigg,et al.  Generalized k-particle brillouin conditions and their use for the construction of correlated electronic wavefunctions , 1979 .

[28]  W. A. Bingel,et al.  Completeness and linear independence of basis sets used in quantum chemistry , 1977 .

[29]  H. Nakatsuji Equation for the direct determination of the density matrix , 1976 .

[30]  R. Bartlett,et al.  Many‐body perturbation theory applied to electron pair correlation energies. I. Closed‐shell first‐row diatomic hydrides , 1976 .

[31]  J. Pople,et al.  Møller–Plesset theory for atomic ground state energies , 1975 .

[32]  Ingvar Lindgren,et al.  The Rayleigh-Schrodinger perturbation and the linked-diagram theorem for a multi-configurational model space , 1974 .

[33]  M. Robb Application of many-body perturbation methods in a discrete orbital basis , 1973 .

[34]  P. W. Langhoff,et al.  Aspects of Time-Dependent Perturbation Theory , 1972 .

[35]  R. Ahlrichs Convergence of the 1 Z Expansion , 1972 .

[36]  Werner Kutzelnigg,et al.  Direct Calculation of Approximate Natural Orbitals and Natural Expansion Coefficients of Atomic and Molecular Electronic Wavefunctions. II. Decoupling of the Pair Equations and Calculation of the Pair Correlation Energies for the Be and LiH Ground States , 1968 .

[37]  P. Claverie,et al.  The Use of Perturbation Methods for the Study of the Effects of Configuration Interaction: I. Choice of the Zeroth-Order Hamiltonian , 1967 .

[38]  J. Cizek On the Correlation Problem in Atomic and Molecular Systems. Calculation of Wavefunction Components in Ursell-Type Expansion Using Quantum-Field Theoretical Methods , 1966 .

[39]  H. P. Kelly Many-Body Perturbation Theory Applied to Open-Shell Atoms , 1966 .

[40]  H. P. Kelly CORRELATION EFFECTS IN MANY FERMION SYSTEMS. II. LINKED CLUSTERS , 1964 .

[41]  H. P. Kelly Correlation Effects in Atoms , 1963 .

[42]  O. Sǐnanoğlu,et al.  MANY-ELECTRON THEORY OF ATOMS AND MOLECULES. I. SHELLS, ELECTRON PAIRS VS MANY-ELECTRON CORRELATIONS , 1962 .

[43]  R. L. Mills,et al.  MANY-BODY BASIS FOR THE OPTICAL MODEL , 1960 .

[44]  D. Layzer On a screening theory of atomic spectra , 1959 .

[45]  F. Coester,et al.  Bound states of a many-particle system , 1958 .

[46]  R. Nesbet Brueckner's Theory and the Method of Superposition of Configurations , 1958 .

[47]  J. Hubbard The description of collective motions in terms of many-body perturbation theory , 1957, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[48]  Jeffrey Goldstone,et al.  Derivation of the Brueckner many-body theory , 1957, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[49]  H. Bethe,et al.  Effect of a repulsive core in the theory of complex nuclei , 1957, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[50]  W. Wada,et al.  Nuclear Saturation and Two-Body Forces: Self-Consistent Solutions and the Effects of the Exclusion Principle , 1956 .

[51]  K. Brueckner,et al.  Many-Body Problem for Strongly Interacting Particles. II. Linked Cluster Expansion , 1955 .

[52]  R. Nesbet Configuration interaction in orbital theories , 1955, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[53]  P. Löwdin Quantum Theory of Many-Particle Systems. I. Physical Interpretations by Means of Density Matrices, Natural Spin-Orbitals, and Convergence Problems in the Method of Configurational Interaction , 1955 .

[54]  K. Brueckner,et al.  TWO-BODY FORCES AND NUCLEAR SATURATION. III. DETAILS OF THE STRUCTURE OF THE NUCLEUS , 1955 .

[55]  M. Gell-Mann,et al.  Bound States in Quantum Field Theory , 1951 .

[56]  G. C. Wick The Evaluation of the Collision Matrix , 1950 .

[57]  R. Feynman The Theory of Positrons , 1949 .

[58]  F. Dyson The Radiation Theories of Tomonaga, Schwinger, and Feynman , 1949 .

[59]  M. Plesset,et al.  Note on an Approximation Treatment for Many-Electron Systems , 1934 .

[60]  John C. Slater,et al.  The Theory of Complex Spectra , 1929 .

[61]  E. Hylleraas,et al.  Neue Berechnung der Energie des Heliums im Grundzustande, sowie des tiefsten Terms von Ortho-Helium , 1929 .

[62]  P. Dirac The Quantum Theory of the Emission and Absorption of Radiation , 1927 .

[63]  P. S. Epstein,et al.  The Stark effect from the point of view of Schroedinger's quantum theory , 1926 .

[64]  W. Kutzelnigg n‐Electron problem and its formulation in terms of k‐particle density cumulants , 2003 .

[65]  David A. Mazziotti,et al.  3,5-CONTRACTED SCHRODINGER EQUATION : DETERMINING QUANTUM ENERGIES AND REDUCED DENSITY MATRICES WITHOUT WAVE FUNCTIONS , 1998 .

[66]  Josef Paldus,et al.  Time-Independent Diagrammatic Approach to Perturbation Theory of Fermion Systems , 1975 .

[67]  K. Freed Many-Body Theories of the Electronic Structure of Atoms and Molecules , 1971 .

[68]  K. Freed Many-Body Approach to Electron Correlation in Atoms and Molecules , 1968 .

[69]  B. Brandow Linked-Cluster Expansions for the Nuclear Many-Body Problem , 1967 .

[70]  N. M. Hugenholtz Perturbation theory of large quantum systems , 1957 .