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Efficient solution of Poissonrsquo;s equation in linear combination of atomic orbitals (LCAO) electronic structure calculations

机译:Efficient solution of Poissonrsquo;s equation in linear combination of atomic orbitals (LCAO) electronic structure calculations

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An accurate and efficient method is described for the evaluation of electrostatic contributions in LCAO electronic structure calculations. The charge density thinsp;rgr;(r) is decomposed into thinsp;rgr;(1)(r), a component whose rapid variation near any nucleus reproduces that of thinsp;rgr;(r) to a very good approximation, and a remainder density dgr;rgr;(r)equiv;rgr;(r)minus;rgr;(1)(r), which is thereby guaranteed to be slowly varying in space. The power of the decomposition resides in the fact that thinsp;rgr;(1)(r) can be expressed exactly as a sum of onehyphen;center densities, without the use of any fit procedure. Because thinsp;rgr;(1)(r) is a sum of onehyphen;center multipolar densities, the Hartree potential is a function with a simple onehyphen;dimensional integral representation, and its matrix elements can be obtained by performing onehyphen;dimensional integrals over it. Since dgr;rgr;(r) is spatially slowly varying, the Hartree potential to which it corresponds and the matrix elements of this potential can accurately be evaluated on a relatively coarse coordinate space mesh, using fast Fourier transforms. The method is illustrated via molecular structure calculations for N2and NH3. The calculations are accurate to a few percent when the required integrals over dgr;rgr;(r) and dgr;V(r) are performed on a mesh of spacing 0.4 a.u. The Nndash;N bond length and stretch frequency are found to equal 2.10 a.u. and 2.3times;103cmminus;1, respectively. The equilibrium Nndash;H bond length and Hndash;Nndash;H angle are calculated to be 1.93 a.u. and 105deg;, respectively, while the NH3inversion barrier turns out to equal 0.25 eV. These results are in good agreement with earlier calculations.

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