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Essentials of Computational Chemistry

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14<br />

Excited Electronic States<br />

14.1 Determinantal/Configurational Representation<br />

<strong>of</strong> Excited States<br />

An excited electronic state is one in which at least one electron is not in as low energy<br />

an orbital as it could be given the molecular geometry. Such a state may be generated by<br />

various processes, e.g., absorption <strong>of</strong> radiation by the ground state or as the product <strong>of</strong> a<br />

chemical reaction. Although unstable relative to collapse to the lower energy ground state,<br />

some excited states may have significant lifetimes owing to inefficient coupling with the<br />

ground state, as described in more detail below.<br />

Given M doubly occupied molecular orbitals and N empty virtual orbitals (and possibly<br />

some number <strong>of</strong> singly occupied orbitals), the number <strong>of</strong> possible excited states that can be<br />

generated is enormous. For the moment, we will restrict our discussion to the case where<br />

the ground state is closed-shell and in the excited state only a single excited electron exists<br />

(implying it must have come from the HOMO). Extending the discussion to more general<br />

cases is intuitively straightforward, but notationally somewhat tedious.<br />

The usual manner in which chemists think about an excited state is to take the ground state<br />

0 as context. Thus, as shown in Figure 14.1, one considers our excited state to be generated<br />

by the removal <strong>of</strong> one electron from the HOMO <strong>of</strong> the ground state and its placement into<br />

some higher-energy orbital. Since the wave function for the ground state can be represented<br />

as a single Slater determinant, e.g.<br />

1 0 =<br />

<br />

<br />

ψ 2 1 ψ 2 2 ψ 2 3 ···ψ 2 <br />

N/2<br />

(14.1)<br />

(the Slater determinant appropriate for the RHF wave function <strong>of</strong> a singlet having N electrons),<br />

then the excited state might in general be written as<br />

a N/2 = ψ 2 1 ψ 2 2 ψ 2 3 ···ψN/2ψ<br />

<br />

a<br />

(14.2)<br />

where we use the compact notation that if an orbital is not doubly occupied, it is multiplied<br />

by an α spin function unless there is a bar over it, in which case it is multiplied by a β<br />

<strong>Essentials</strong> <strong>of</strong> <strong>Computational</strong> <strong>Chemistry</strong>, 2nd Edition Christopher J. Cramer<br />

© 2004 John Wiley & Sons, Ltd ISBNs: 0-470-09181-9 (cased); 0-470-09182-7 (pbk)

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