Real-space finite-difference approach for multi-body systems: path-integral renormalization group method and direct energy minimization method

The path-integral renormalization group and direct energy minimization method of practical first-principles electronic structure calculations for multi-body systems within the framework of the real-space finite-difference scheme are introduced. These two methods can handle higher dimensional systems with consideration of the correlation effect. Furthermore, they can be easily extended to the multicomponent quantum systems which contain more than two kinds of quantum particles. The key to the present methods is employing linear combinations of nonorthogonal Slater determinants (SDs) as multi-body wavefunctions. As one of the noticeable results, the same accuracy as the variational Monte Carlo method is achieved with a few SDs. This enables us to study the entire ground state consisting of electrons and nuclei without the need to use the Born-Oppenheimer approximation. Recent activities on methodological developments aiming towards practical calculations such as the implementation of auxiliary field for Coulombic interaction, the treatment of the kinetic operator in imaginary-time evolutions, the time-saving double-grid technique for bare-Coulomb atomic potentials and the optimization scheme for minimizing the total-energy functional are also introduced. As test examples, the total energy of the hydrogen molecule, the atomic configuration of the methylene and the electronic structures of two-dimensional quantum dots are calculated, and the accuracy, availability and possibility of the present methods are demonstrated.

[1]  J. Kainz,et al.  QUANTUM DOTS IN HIGH MAGNETIC FIELDS: CALCULATION OF GROUND-STATE PROPERTIES , 2002 .

[2]  Tomoya Ono,et al.  Timesaving Double-Grid Method for Real-Space Electronic-Structure Calculations , 1999 .

[3]  Sullivan,et al.  Real-space multigrid-based approach to large-scale electronic structure calculations. , 1996, Physical review. B, Condensed matter.

[4]  Frank R. Wagner,et al.  The CO/Pt(111) puzzle , 2000 .

[5]  N. Shibata Application of the density matrix renormalization group method to finite temperatures and two-dimensional systems , 2003, cond-mat/0310028.

[6]  J. Leburton,et al.  Von Neumann–Wigner Theorem in Quantum Dot Molecules , 2007, Physical Models for Quantum Dots.

[7]  Magnetic-Field Manipulation of Chemical Bonding in Artificial Molecules , 2001, cond-mat/0109167.

[8]  P. Jensen,et al.  The potential surface and stretching frequencies of X̃ 3B1 methylene (CH2) determined from experiment using the Morse oscillator‐rigid bender internal dynamics Hamiltonian , 1988 .

[9]  Robert H. Blick,et al.  Probing and Controlling the Bonds of an Artificial Molecule , 2002, Science.

[10]  Xinwei Zhao,et al.  Quantum-size effect in model nanocrystalline/amorphous mixed-phase silicon structures , 1999 .

[11]  L. Vandersypen,et al.  Control and Detection of Singlet-Triplet Mixing in a Random Nuclear Field , 2005, Science.

[12]  A. Szabó,et al.  Modern quantum chemistry : introduction to advanced electronic structure theory , 1982 .

[13]  N. H. March,et al.  Recent progress in the field of electron correlation , 1994 .

[14]  White,et al.  Density-matrix algorithms for quantum renormalization groups. , 1993, Physical review. B, Condensed matter.

[15]  Tsukada,et al.  Adaptive finite-element method for electronic-structure calculations. , 1996, Physical review. B, Condensed matter.

[16]  H. Petek,et al.  Analysis of CH2 ã 1A1 (1,0,0) and (0,0,1) Coriolis‐coupled states, ã 1A1–X̃ 3B1 spin–orbit coupling, and the equilibrium structure of CH2 ã 1A1 state , 1989 .

[17]  Henry Krakauer,et al.  Auxiliary-field quantum Monte Carlo study of TiO and MnO molecules , 2005, cond-mat/0510791.

[18]  U. Landman,et al.  Artificial quantum-dot helium molecules: Electronic spectra, spin structures, and Heisenberg clusters , 2009, 0907.1571.

[19]  M. Imada,et al.  Path-Integral Renormalization Group Method for Numerical Study on Ground States of Strongly Correlated Electronic Systems. , 2001, cond-mat/0104140.

[20]  Henry Krakauer,et al.  Pressure-induced diamond to β-tin transition in bulk silicon: A quantum Monte Carlo study , 2009, 0908.4477.

[21]  F. Gebhard,et al.  Density matrix renormalization group study of excitons in polydiacetylene chains , 2009, 0908.4160.

[22]  Maksym,et al.  Quantum dots in a magnetic field: Role of electron-electron interactions. , 1990, Physical review letters.

[23]  Galli,et al.  Electronic-structure calculations and molecular-dynamics simulations with linear system-size scaling. , 1994, Physical review. B, Condensed matter.

[24]  Even-odd oscillation in conductance of a single-row sodium nanowire , 2004, cond-mat/0412577.

[25]  M. Taut Two electrons in a homogeneous magnetic field: particular analytical solutions , 1994 .

[26]  L. Vandersypen,et al.  Spins in few-electron quantum dots , 2006, cond-mat/0610433.

[27]  Matthias Scheffler,et al.  Towards an exact treatment of exchange and correlation in materials: Application to the "CO adsorption puzzle" and other systems , 2007 .

[28]  Y. Kawazoe,et al.  Diffusion Monte Carlo study of correlation in the hydrogen molecule , 2007 .

[29]  Henry Krakauer,et al.  Phaseless auxiliary-field quantum Monte Carlo calculations with plane waves and pseudopotentials : Applications to atoms and molecules , 2007, cond-mat/0702085.

[30]  Tomoya Ono,et al.  Real-space electronic-structure calculations with a time-saving double-grid technique , 2004, cond-mat/0412571.

[31]  Car,et al.  Orbital formulation for electronic-structure calculations with linear system-size scaling. , 1993, Physical review. B, Condensed matter.

[32]  T. Xiang,et al.  TRANSFER-MATRIX DENSITY-MATRIX RENORMALIZATION-GROUP THEORY FOR THERMODYNAMICS OF ONE-DIMENSIONAL QUANTUM SYSTEMS , 1997 .

[33]  J. Leburton,et al.  Tunable Many-Body Effects in Triple Quantum Dots , 2009, Physical Models for Quantum Dots.

[34]  END STATES DUE TO A SPIN-PEIERLS TRANSITION IN QUANTUM WIRES , 1999 .

[35]  R. Needs,et al.  Quantum Monte Carlo simulations of solids , 2001 .

[36]  White,et al.  Density matrix formulation for quantum renormalization groups. , 1992, Physical review letters.

[37]  Jacob M. Taylor,et al.  Coherent Manipulation of Coupled Electron Spins in Semiconductor Quantum Dots , 2005, Science.

[38]  Masuo Suzuki Quantum Monte Carlo methods — recent developments , 1993 .

[39]  Baroni,et al.  Auxiliary-field quantum Monte Carlo calculations for systems with long-range repulsive interactions. , 1993, Physical review letters.

[40]  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 .

[41]  Wu,et al.  Higher-order finite-difference pseudopotential method: An application to diatomic molecules. , 1994, Physical review. B, Condensed matter.

[42]  H. Dr GENERALIZED-GRADIENT FUNCTIONALS IN ADAPTIVE CURVILINEAR COORDINATES , 1996 .

[43]  Kavita Joshi,et al.  Electronic structure of many-electron square-well quantum dots with and without an attractive impurity : Spin-density-functional theory , 2007 .

[44]  Two-dimensional quantum dots in high magnetic fields: Rotating-electron-molecule versus composite-fermion approach , 2003, cond-mat/0302504.

[45]  M. Manninen,et al.  Electronic structure of quantum dots , 2002 .

[46]  Henry Krakauer,et al.  Quantum Monte Carlo method using phase-free random walks with slater determinants. , 2003, Physical review letters.

[47]  C. Thelander,et al.  Spin relaxation in InAs nanowires studied by tunable weak antilocalization , 2005 .

[48]  Spin configurations in circular and rectangular vertical quantum dots in a magnetic field : Three-dimensional self-consistent simulations , 2005, cond-mat/0506585.

[49]  Hallberg Density-matrix algorithm for the calculation of dynamical properties of low-dimensional systems. , 1995, Physical review. B, Condensed matter.

[50]  T. Honda,et al.  Shell Filling and Spin Effects in a Few Electron Quantum Dot. , 1996, Physical review letters.

[51]  Eric Jeckelmann Dynamical density-matrix renormalization-group method , 2002 .

[52]  R. Nazmitdinov,et al.  Finite-thickness effects in ground-state transitions of two-electron quantum dots , 2007, 0711.1246.

[53]  Masatoshi Imada,et al.  Numerical Studies on the Hubbard Model and the t-J Model in One- and Two-Dimensions , 1989 .

[54]  K. Shiraishi,et al.  Large-scale density-functional calculations on silicon divacancies , 2008 .

[55]  Kikuji Hirose,et al.  Total-energy minimization of few-body electron systems in the real-space finite-difference scheme , 2009, Journal of physics. Condensed matter : an Institute of Physics journal.

[56]  Comparison of global and local adaptive coordinates for density-functional calculations , 2000, cond-mat/0008347.

[57]  On the quantum few-body problem , 1984 .

[58]  T. Iwata,et al.  Increase in specific heat and possible hindered rotation of interstitial C 2 molecules in neutron-irradiated graphite , 2010 .

[59]  U. Landman,et al.  Three-electron anisotropic quantum dots in variable magnetic fields: Exact results for excitation spectra, spin structures, and entanglement , 2007, 0710.4325.

[60]  Kavita Joshi,et al.  Impurity effects on the electronic structure of square quantum dots : A full configuration-interaction study , 2008 .

[61]  R. M. Nieminen,et al.  Electronic structure of rectangular quantum dots , 2003 .

[62]  T. D. Kuehner,et al.  Dynamical correlation functions using the density matrix renormalization group , 1998, cond-mat/9812372.

[63]  In-Ho Lee,et al.  Electron-electron interactions in square quantum dots , 2001 .

[64]  K. Hirose,et al.  First-principles path-integral renormalization-group method for Coulombic many-body systems , 2009 .

[65]  Maksym,et al.  Effect of electron-electron interactions on the magnetization of quantum dots. , 1992, Physical review. B, Condensed matter.

[66]  Spontaneous Symmetry Breaking in Single and Molecular Quantum Dots , 1999 .

[67]  D Porras,et al.  Density matrix renormalization group and periodic boundary conditions: a quantum information perspective. , 2004, Physical review letters.

[68]  Unified description of floppy and rigid rotating Wigner molecules formed in quantum dots , 2003, cond-mat/0311480.

[69]  T. Ono,et al.  Order-N first-principles calculation method for self-consistent ground-state electronic structures of semi-infinite systems. , 2006, Physical review. E, Statistical, nonlinear, and soft matter physics.

[70]  U. Landman,et al.  Group theoretical analysis of symmetry breaking in two-dimensional quantum dots , 2003, cond-mat/0302130.

[71]  Path‐integral renormalization group treatments for many‐electron systems with long‐range repulsive interactions , 2007, 0711.4761.

[72]  W. V. D. Wiel,et al.  Electron transport through double quantum dots , 2002, cond-mat/0205350.

[73]  Masatoshi Imada,et al.  Path-Integral Renormalization Group Method for Numerical Study of Strongly Correlated Electron Systems , 2000 .

[74]  Yoshitaka Fujimoto,et al.  First-principles treatments of electron transport properties for nanoscale junctions , 2003 .

[75]  Bryant,et al.  Electronic structure of ultrasmall quantum-well boxes. , 1987, Physical review letters.

[76]  Hamann Band structure in adaptive curvilinear coordinates. , 1995, Physical review. B, Condensed matter.

[77]  Galli,et al.  Real-space adaptive-coordinate electronic-structure calculations. , 1995, Physical review. B, Condensed matter.

[78]  W. Kołos,et al.  Improved Theoretical Ground‐State Energy of the Hydrogen Molecule , 1968 .

[79]  N. Umezawa,et al.  Transcorrelated method for electronic systems coupled with variational Monte Carlo calculation , 2003 .

[80]  Dynamic Correlations in Doped 1D Kondo Insulator - Finite-T DMRG Study - , 1999, cond-mat/9907416.

[81]  Tomotoshi Nishino,et al.  A Density Matrix Algorithm for 3D Classical Models , 1998 .

[82]  Watanabe,et al.  Self-consistent density functional calculation of field emission currents from metals , 2000, Physical review letters.

[83]  H. Nakatsuji,et al.  Solving the Schrödinger equation of atoms and molecules without analytical integration based on the free iterative-complement-interaction wave function. , 2007, Physical review letters.

[84]  M. Pi,et al.  Quantum Monte Carlo study of few-electron concentric double quantum rings , 2009 .

[85]  Y. Saad,et al.  Finite-difference-pseudopotential method: Electronic structure calculations without a basis. , 1994, Physical review letters.

[86]  S. Koonin,et al.  Auxiliary field Monte-Carlo for quantum many-body ground states , 1986 .

[87]  S. P. Benham,et al.  Self-consistent finite-difference electronic structure calculations , 2001 .

[88]  J. Leburton,et al.  Dimensionality Effects in the Two-Electron System in Circular and Elliptic Quantum Dots , 2006, Physical Models for Quantum Dots.

[89]  Adaptive-coordinate electronic structure of 3d bands: TiO 2 , 1997 .

[90]  T. Nishino,et al.  Product Wave Function Renormalization Group , 1995 .

[91]  R. Ashoori Electrons in artificial atoms , 1996, Nature.