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內容簡介

It is traditional for quantum theory of molecular systems （molecular quantum chemistry） to describe the properties of a many-atom system on the grounds of in- teratomic interactions applying the linear combination of atomic orbitals （LCAO） approximation in the electronic-structure calculations. The basis of the theory of the electronic structure of solids is the periodicity of the crystalline potential and Bloch- type one-electron states， in the majority of cases approximated by a linear combina- tion of plane waves （LCPW）. In a quantum chemistry of solids the LCAO approach is extended to periodic systems and modified in such a way that the periodicity of the potential is correctly taken into account， but the language traditional for chemistry is used when the interatornic interaction is analyzed to explain the properties of the crystalline solids. At first， the quantum chemistry of solids was considered simply as the energy-band theory or the theory of the chemical bond in tetrahedral semi-conductors . From the beginning of the 1970s the use of powerful computer codes has become a common practice in molecular quantum chemistry to predict many properties of molecules in the first-principles LCAO calculations. In the condensed-matter studies the accurate description of the system at an atomic scale was much less advanced .

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目錄

part i theory
1 introduction
2 space groups and crystalline structures
2.1 translation and point symmetry of cryst&lz;
2.1.1 symmetry of molecules and crystals: similarities and differences
2.1.2 translation symmetry of crystals. point symmetry of bravais lattices. crystal class
2.2 space groups
2.2.1 space groups of brawis lattices. symmorphic and nonsymmorphic space groups
2.2.2 three-periodic space groups
2.2.3 site symmetry in crystals. wyckoff positions
2.3 crystalline structures
2.3.1 crystal-structure types. structure information for computer codes
2.3.2 cubic structures: diamond, rocksalt, fluorite, zincblende, cesium chloride, cubic perovskite
2.3.3 tetragonoj structures: rutile, anatase and la~cuo4
2.3.4 orthorhombic structures: lamno3 and yba2cuso?
2.3.5 hexagonal and trigonal structures: graphite, wurtzite, corundum and scmno3

3 symmetry and localization of crystalline orbitals
3.1 translation and space symmetry of crystalline orbitals.bloch functions
3.1.1 symmetry of molecular and crystalline orbitals
3.1.2 irreducible representations of translation group. brillouin zone
3.1.3 stars of wavevectors. little groups. fhll representations of space groups
3.1.4 small representations of a little group. projective representations of point groups
3.2 site symmetry and induced representations of space groups
3.2.1 induced representations of point groups. localized molecular orbitals
3.2.2 induced representations of space groups in q-basis
3.2.3 induced representations of space groups in k-basis.band representations
3.2.4 simple and composite induced representations
3.2.5 simple induced representations for cubic space groups ok, and
3.2.6 symmetry of atomic and crystalline orbitals in mgo, si and srzro3 crystals
3.3 symmetry of localized crystalline orbitals. wannier functions
3.3.1 symmetry of localized orbitals and band representations of space groups
3.3.2 localization criteria in wannier-function generation
3.3.3 localized orbitals for valence bands: lcao approximation
3.3.4 variational method of localized wannier-function generation on the base of bloch functions

4 hartree-fock lcao method for periodic systems
4.1 one-electron approximation for crystals
4.1.1 one-electron and one-determinant approximations for molecules and crystals
4.1.2 symmetry of the one-electron approximation hamiltonian
4.1.3 restricted and unrestricted hartree-fock lcao methods for molecules
4.1.4 specific features of the hartree-fock method for a cyclic model of a crystal
4.1.5 restricted hartree-fock lcao method for crystals
4.1.6 unrestricted and restricted open-shell hartree-fock methods for crystals
4.2 special points of brillouin zone
4.2.1 superceus of three-dimensional bravais lattices
4.2.2 special points of brillouin-zone generating
4.2.3 modification of the monkhorst-pack special-points meshes
4.3 density matrix of crystals in the hartree-fock method
4.3.1 properites of the one-electron density matrix of a crystal
4.3.2 the one-electron density matrix of the crystal in the lcao approximation
4.3.3 interpolation procedure for constructing an approximate density matrix for periodic systems

5 electron correlations in molecules and crystals
5.1 electron correlations in molecules: post-hartree-fock methods
5.1.1 what is the electron correlation ?
5.1.2 configuration interaction and multi-configuration self-consistent field methods
5.1.3 coupled-cluster methods
5.1.4 many-electron perturbation theory
5.1.5 local electron-correlation methods
5.2 incremental scheme for local correlation in periodic systems
5.2.1 weak and strong electron-correlation
5.2.2 method of incfements: ground state
5.2.3 method of increments: valence-band structure and bandgap
5.3 atomic orbital laplace-transformed mp2 theory for periodic systems
5.3.1 laplace mp2 for periodic systems: unit-cell correlation energy
5.3.2 laplace mp2 for periodic systems:bandgap
5.4 local mp2 electron-correlation method for nonconducting crystals
5.4.1 local mp2 equations for periodic systems
5.4.2 fitted wannier functions for periodic local correlation methods
5.4.3 symmetry exploitation in local mp2 method for periodic systems

6 semiempirical lcao methods for molecules and periodic systems
6.1 extended h/ickel and mulliken-r/idenberg approximations
6.1.1 nonself-consistent extended h/ickel-tight-binding method
6.1.2 iterative mulliken-r/idenberg method for crystals
6.2 zero-differential overlap approximations for molecules and crystals
6.2.1 zero-differential overlap apl~roximations for molecules
6.2.2 complete and intermediate neglect of differential overlap for crystals
6.3 zero-differential overlap approximation in cyclic-cluster model
6.3.1 symmetry of cyclic-cluster model of perfect crystal
6.3.2 semiempirical lcao methods in cyclic-cluster model
6.3.3 implementation of the cyclic-clnster model in msindo and hartree-fock lcao methods

7 kohn-sham lcao method for periodic systems
7.1 foundations of the density-functional theory
7.1.1 the basic formulation of the density-functional theory
7.1.2 the kohn-sham single-particle equations
7.1.3 exchange and correlation functionals in the local density approximation
7.1.4 beyond the local density approximation
7.1.5 the pair density. orbital-dependent exchange-correlation functionals
7.2 density-functional lcao methods for solids
7.2.1 implementation of kohn-sham lcao method in crystals calculations
7.2.2 linear-scaling dft lcao methods for solids
7.2.3 heyd-scnseria-ernzerhof screened coulomb hybrid functional
7.2.4 are molecular exchange-correlation functionals transferable to crystals?
7.2.5 density-functional methods for strongly correlated systems: sic dft and dft+u approaches part ii applications
basis sets and pseudopotentlals in periodic lcao calculations

8.1 basis sets in the electron-structure calculations of crystals
8.1.1 plane waves and atomic-like basis sets. slater-type functions
8.1.2 molecular basis sets of gaussian-type functions
8.1.3 molecular basis sets adaptation for periodic systems
8.2 nonrelativistic effective core potentials and valence basis sets
8.2.1 effective core potentials: theoretical grounds
8.2.2 gaussian form of effective core potentials and valence basis sets in periodic lcao calculations
8.2.3 separable embedding potential
8.3 relativistic effective core potentials and valence basis sets
8.3.1 relativistic electronic structure theory: dirac-hartree-fock and dirac-kohn-sham methods for molecules
8.3.2 relativistic effective core potentials
8.3.3 one-center restoration of electronic structure in the core region
8.3.4 basis sets for relativistic calculations of molecules
8.3.5 relativistic lcao methods for periodic systems lcao calculations of perfect-crystal properties

9.1 theoretical analysis of chemical bonding in crystals
9.1.1 local properties of electronic structure in lcao hf and dft methods for crystals and post-hf methods for molecules
9.1.2 chemical bonding in cyclic-cluster model: local properties of com 固體量子化學：晶體的原子軌道綫性組閤第一性原理計算方法 [Quantum Chemistry of Solids:The LCAO First Principles Treatment of Crys 下載 mobi epub pdf txt 電子書

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書是英文版的，可以慢慢看的，專業必備！！！是影印版的。

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書是英文版的，可以慢慢看的，專業必備！！！是影印版的。

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原子綫性軌道siesta的使用原理，很深奧的。研究生難度

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