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Basis set superposition error : ウィキペディア英語版
Basis set superposition error
In quantum chemistry, calculations using finite basis sets are susceptible to basis set superposition error (BSSE). As the atoms of interacting molecules (or of different parts of the same molecule - intramolecular BSSE)〔 〕 approach one another, their basis functions overlap. Each monomer "borrows" functions from other nearby components, effectively increasing its basis set and improving the calculation of derived properties such as energy. If the total energy is minimised as a function of the system geometry, the short-range energies from the mixed basis sets must be compared with the long-range energies from the unmixed sets, and this mismatch introduces an error.
Other than using infinite basis sets, two methods exist to eliminate the BSSE. In the ''chemical Hamiltonian approach'' (CHA),〔(【引用サイトリンク】 title = THE CHEMICAL HAMILTONIAN APPROACH (CHA) )〕 basis set mixing is prevented ''a priori'', by replacing the conventional Hamiltonian with one in which all the projector-containing terms that would allow mixing have been removed. In the ''counterpoise method'' (CP), the BSSE is calculated by re-performing ''all'' the calculations using the mixed basis sets, and the error is then subtracted ''a posteriori'' from the uncorrected energy. (The mixed basis sets are realised by introducing "ghost orbitals", basis set functions which have no electrons or protons.) Though conceptually very different, the two methods tend to give similar results. It has however been shown that the error is often largest when using the CP method since the atoms to which the functions are centered have a greater impact on those functions whereas in the CP model, those orbitals have much greater freedom.
==References==


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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