$STONE group (optional) This group defines the expansion points for Stone's distributed multipole analysis (DMA) of the electrostatic potential. The DMA takes the multipolar expansion of each overlap charge density defined by two Gaussian primitives, and translates it from the center of charge of the overlap density to the nearest expansion point. Some references for the method are A.J.Stone Chem.Phys.Lett. 83, 233-239 (1981) A.J.Stone, M.Alderton Mol.Phys. 56, 1047-1064(1985) A.J.Stone J.Chem.Theory and Comput. 1, 1128-1132(2005) The existence of $STONE input is what triggers the analysis. The first set of lines must appear as the first line after $STONE (enter a blank line if you make no choice), then enter as many choices as you wish, in any order, from the other sets. ---------------------------------------------------------- BIGEXPexponents larger than this are treated by the original Stone expansion, and those smaller by a numerical integration. The default is 0.0, meaning no numerical grid. The other parameters are meaningless if BIGEXP remains zero. NRAD number of radial grid points (default 100) NANG number of angular grid points, choose one of the Lebedev grid values (default 590) SMOOTH degree of Becke smoothing (default=2) SMRAD Radii choice, 0=constant, 1=Bragg-Slater, which is the default. ---------------------------------------------------------- ATOM i name, where ATOM is a keyword indicating that a particular atom is selected as an expansion center. i is the number of the atom name is an optional name for the atom. If not entered the name will be set to the name used in the $DATA input. ---------------------------------------------------------- ATOMS is a keyword selecting all nuclei in the molecule as expansion points. No other input on the line is necessary. ---------------------------------------------------------- BONDS is a keyword selecting all bond midpoints in the molecule as expansion points. No other input on the line is necessary. ---------------------------------------------------------- BOND i j name, where BOND is a keyword indicating that a bond mid- point is selected as an expansion center. i,j are the indices of the atoms defining the bond, corresponding to two atoms in $DATA. name an optional name for the bond midpoint. If omitted, it is set to 'BOND'. ---------------------------------------------------------- CMASS is a keyword selecting the center of mass as an expansion point. No other input on the line is necessary. ---------------------------------------------------------- POINT x y z name, where POINT is a keyword indicating that an arbitrary point is selected as an expansion point. x,y,z are the coordinates of the point, in Bohr. name is an optional name for the expansion point. If omitted, it is set to 'POINT'. ---------------------------------------------------------- While making the EFPs for QM/MM run, a single keyword QMMMBUF is necessary. Adding additional keywords may lead to meaningless results. The program will automatically select atoms and bond midpoints which are outside the buffer zone as the multipole expansion points. QMMMBUF nmo, where QMMMBUF is a keyword specifying the number of QM/MM buffer molecular orbitals, which must be the first NMO orbitals in the MO set. These orbitals must be frozen in the buffer zone, so this is useful only if $MOFRZ is given. NMO is the number of buffer MO-s (if NMO is omitted, it will be set to the number of frozen MOs in $MOFRZ) ========================================================== The second and third moments on the printout can be converted to Buckingham's tensors by formula 9 of A.D.Buckingham, Quart.Rev. 13, 183-214 (1959) These can in turn be converted to spherical tensors by the formulae in the appendix of S.L.Price, et al. Mol.Phys. 52, 987-1001 (1984) ==========================================================
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