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Essentials of Computational Chemistry

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7.2 MULTICONFIGURATION SELF-CONSISTENT FIELD THEORY 207<br />

squares <strong>of</strong> all CSF coefficients is unity and the percent contribution <strong>of</strong> any CSF to the wave<br />

function is simply its expansion coefficient squared.<br />

MCSCF calculations in practice require much more technical expertise than do singleconfiguration<br />

HF analogs. One particularly difficult problem is that spurious minima in<br />

coefficient space can <strong>of</strong>ten be found, instead <strong>of</strong> the variational minimum. Thus, convergence<br />

criteria are met for the self-consistent field, but the wave function is not really optimized. It<br />

usually requires a careful inspection <strong>of</strong> the orbital shapes and, where available, some data<br />

on relative energetics between related species or along a reaction coordinate to ascertain if<br />

this has happened.<br />

A different issue requiring careful attention is how to go about selecting the orbitals that<br />

should be allowed to be partially occupied, and how to specify the ‘flexibility’ <strong>of</strong> the CSF<br />

expansion. We turn to this issue next.<br />

7.2.2 Active Space Specification<br />

Selection <strong>of</strong> orbitals to include in an MCSCF requires first and foremost a consideration <strong>of</strong><br />

the chemistry being examined. For instance, in the TMM example above, a two-configuration<br />

wave function is probably not a very good choice in this system. When the orbitals being<br />

considered belong to a π system, it is typically a good idea to include all <strong>of</strong> them, because<br />

as a rule they are all fairly close to one another in energy. Thus, a more complete active<br />

space for TMM would consider all four π orbitals and the possible ways to distribute the<br />

four π electrons within them. MCSCF active space choices are <strong>of</strong>ten abbreviated as ‘(m,n)’<br />

where m is the number <strong>of</strong> electrons and n is the number <strong>of</strong> orbitals, so this would be a (4,4)<br />

calculation.<br />

Sometimes reaction coordinates are studied that involve substantial changes in bonding.<br />

In such an instance, it is critical that a consistent choice <strong>of</strong> orbitals be made. For instance,<br />

consider the electrocyclization <strong>of</strong> 1,3-butadiene to cyclobutene (Figure 7.2). The frontier<br />

orbitals <strong>of</strong> butadiene are those associated with the π system, so, as just discussed, a (4,4)<br />

approach seems logical. However, the electrocyclization reaction transforms the two π bonds<br />

into one different π bond and one new σ bond. Thus, a consistent (4,4) choice in cyclobutene<br />

would involve the π and π* orbitals and the σ and σ * orbitals <strong>of</strong> the new single bond.<br />

frontier orbitals<br />

p1 , p2 , p3 , p4 diabatic correlation<br />

active orbitals<br />

p, p*, s, s*<br />

Figure 7.2 The frontier orbitals <strong>of</strong> s-cis-1,3-butadiene are the four π orbitals (π2 is the specific<br />

example shown). If these orbitals are followed in a diabatic sense along the electrocyclization reaction<br />

coordinate, they correlate with the indicated orbitals <strong>of</strong> cyclobutadiene

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