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Essentials of Computational Chemistry

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210 7 INCLUDING ELECTRON CORRELATION IN MO THEORY<br />

E<br />

frozen HF<br />

virtual orbitals<br />

enforced empty<br />

no more than<br />

n excitations<br />

in permitted<br />

Complete active space<br />

all possible<br />

occupation<br />

schemes allowed<br />

no more than<br />

n excitations<br />

out permitted<br />

enforced doubly<br />

occupied<br />

frozen HF<br />

occupied orbitals<br />

restricted<br />

active<br />

space<br />

Figure 7.3 Possible assignment <strong>of</strong> different orbitals in a completely general MCSCF formalism.<br />

Frozen orbitals are not permitted to relax from their HF shapes, in addition to having their occupation<br />

numbers <strong>of</strong> zero (virtual) or two (occupied) enforced<br />

While all <strong>of</strong> the above details are useful for making calculations more efficient, they still<br />

are not necessarily very helpful in evaluating just which orbitals should be included in any<br />

given space. Typically, a certain amount <strong>of</strong> trial and error is required in the selection <strong>of</strong> an<br />

active space. After selection <strong>of</strong> a given active space and convergence <strong>of</strong> the MCSCF wave<br />

function, one should inspect the occupation numbers <strong>of</strong> the active orbitals. A reasonable<br />

rule <strong>of</strong> thumb is that any orbital having an occupation number greater than 1.98 or less<br />

than 0.02 is not important enough to include in the CAS space, and should be removed to<br />

avoid instability. In addition, <strong>of</strong> course, it may be wise to add some orbitals not previously<br />

considered to see if their occupation numbers justify inclusion in the active space. And,

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