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Essentials of Computational Chemistry

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236 7 INCLUDING ELECTRON CORRELATION IN MO THEORY<br />

However, the generally robust nature <strong>of</strong> MP2 in the above examples simply reflects the<br />

degree to which most minima are already fairly well described by HF wave functions. When<br />

this is not the case, e.g., in TS structures, there are no hard and fast rules that can be cited<br />

with respect to the expected quality <strong>of</strong> any level <strong>of</strong> theory. Instead, one is thrown back on<br />

the twin responsibilities <strong>of</strong> demonstrating either (a) agreement with known experimental data<br />

<strong>of</strong> one kind or another in the same or related systems or (b) convergence with respect to<br />

treatment <strong>of</strong> electron correlation. A rough quality ordering that is <strong>of</strong>ten observed is<br />

HF < MP2 ∼ MP3 ∼ CCD < CISD<br />

< MP4SDQ ∼ QCISD ∼ CCSD < MP4<br />

< QCISD(T) ∼ CCSD(T) ∼ BD(T) (7.59)<br />

Table 7.4 provides a more quantitative feel for the performance summary embodied in<br />

Eq. (7.59) using data provided by Bartlett (1995) for the absolute errors in various levels <strong>of</strong><br />

theory compared to full CI for HB, H2O, and HF using a polarized double-ζ basis set. In this<br />

case, calculations were carried out both at the equilibrium geometries, and also at geometries<br />

where the X–H bonds were stretched by 50% and 100%; correlation should become<br />

more important in describing these higher energy species (see also Dutta and Sherrill 2003).<br />

The ordering <strong>of</strong> the levels in the table is approximately that listed in Eq. (7.59), although<br />

CCD seems to do fortuitously well. As expected, the lower levels <strong>of</strong> correlation treatment<br />

degrade markedly compared to the higher levels when the bonds are stretched. A few levels<br />

not generally available in most electronic structure packages are included in the table for<br />

completeness, including MP5, MP6, and levels having full inclusion <strong>of</strong> triples, represented<br />

by ‘T’ instead <strong>of</strong> ‘(T)’. The heroically expensive CCSDTQ, which takes full account <strong>of</strong> all<br />

Table 7.4 Average errors in correlation energies (kcal mol −1 ) compared to full CI for various methods<br />

applied to HB, H2O, and HF at both equilibrium and bond-stretched geometries<br />

Level <strong>of</strong> theory Equilibrium geometry Equilibrium and stretched geometries<br />

MP2 10.4 17.4<br />

MP3 5.0 14.4<br />

CISD 5.8 13.8<br />

CCD 2.4 8.0<br />

MP4SDQ 2.7 7.1<br />

CCSD 1.9 4.5<br />

QCISD 1.7 4.0<br />

MP4 1.3 3.7<br />

MP5 0.8 3.2<br />

MP6 0.3 0.9<br />

CCSD(T) 0.3 0.6<br />

QCISD(T) 0.3 0.5<br />

CCSDT 0.2 0.5<br />

CCSDTQ 0.01 0.02

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