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32 THE FULL CI PROGRAM 244<br />

32 THE FULL CI PROGRAM<br />

This module is the determinant full CI program, as described in<br />

P.J. Knowles and N.C. Handy, Chem. Phys. Letters 111 (1984) 315,<br />

P.J. Knowles and N.C. Handy, Comp. Phys. Commun. 54 (1989) 75.<br />

Published work resulting from the use of this program should cite these references.<br />

The program in normal use finds the lowest eigenvector of the complete CI hamiltonian matrix;<br />

more sophisticated use is possible, but not documented here. The program is interfaced to free<br />

standing versions such as supplied in the CPC program library by use of the DUMP option.<br />

The program is called with the command FCI.<br />

32.1 Defining the orbitals<br />

ORBIT,name.file;<br />

name.file specifies the record from which orbitals are read. The default is the set of orbitals from<br />

the last SCF, MCSCF or CI calculation.<br />

32.2 Occupied orbitals<br />

OCC,n 1 ,n 2 ,...,n 8 ;<br />

n i specifies numbers of occupied orbitals (including CORE) in irreducible representation number<br />

i. If not given, the default is the complete basis set.<br />

32.3 Frozen-core orbitals<br />

CORE,n 1 ,n 2 ,...,n 8 ;<br />

n i is the number of frozen-core orbitals in irrep number i. These orbitals are doubly occupied<br />

in all configurations, i.e., not correlated. If no CORE card is given, the program uses the same<br />

core orbitals as the last CI calculation; if there was none, then the atomic inner shells are taken<br />

as core. To avoid this behaviour and correlate all electrons, specify<br />

CORE<br />

32.4 Defining the state symmetry<br />

The number of electrons and the total symmetry of the wavefunction are specified on the WF<br />

card:<br />

WF,elec,sym,spin<br />

where<br />

elec:<br />

sym:<br />

spin:<br />

is the number of electrons<br />

is the number of the irreducible representation<br />

defines the spin symmetry, spin= 2S (singlet=0, doublet=1, triplet=2,<br />

etc.)

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