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39 THE VB PROGRAM CASVB 285<br />

39.9.5 Defining several optimizations<br />

More than one optimization may be performed in the same CASVB deck, by the use of OPTIM<br />

keywords:<br />

OPTIM[;. . . ;FINOPTIM];<br />

The subcommands may be any optimization declarations defined in this section, as well as<br />

any symmetry or constraints specifications described in section 39.10. Commands given as<br />

arguments to OPTIM will be particular to this optimization step, whereas commands specified<br />

outside will act as default definitions for all subsequent OPTIM keywords.<br />

If only one optimization step is required, the OPTIM keyword need not be specified.<br />

When only a machine-generated guess is available, CASVB will attempt to define a sequence of<br />

optimization steps chosen such as to maximize the likelihood of successful convergence and to<br />

minimize CPU usage. To override this behaviour, simply specify one or more OPTIM cards.<br />

39.9.6 Multi-step optimization<br />

A loop over two or more optimization steps may be specified using:<br />

ALTERN,Niter;. . . ;FINALTER<br />

With this specification the program will repeat the enclosed optimization steps until either all<br />

optimizations have converged, or the maximum iteration count, Niter, has been reached.<br />

39.10 Point group symmetry and constraints<br />

The problems associated with symmetry-adapting valence bond wavefunctions are considered,<br />

for example, in: T. Thorsteinsson, D. L. Cooper, J. Gerratt and M. Raimondi, Theor. Chim. Acta<br />

95, 131 (1997).<br />

39.10.1 Symmetry operations<br />

SYMELM,label,sign;<br />

Initiates the definition of a symmetry operation referred to by label (any three characters). sign<br />

can be + or −; it specifies whether the total wavefunction is symmetric or antisymmetric under<br />

this operation, respectively. A value for sign is not always necessary but, if provided, constraints<br />

will be put on the structure coefficients to ensure that the wavefunction has the correct overall<br />

symmetry (note that the configuration list must be closed under the orbital permutation induced<br />

by label for this to be possible).<br />

The operator is defined in terms of its action on the active MOs as specified by one or more of<br />

the keywords IRREPS, COEFFS, or TRANS (any other keyword will terminate the definition<br />

of this symmetry operator). If no further keyword is supplied, the identity is assumed for label.<br />

The alternative format SYMELM,label,sign;key-1,. . . ;key-2,. . . ;. . . may also be used.<br />

39.10.2 The IRREPS keyword<br />

IRREPS,i 1 , i 2 ,. . . ;

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