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Essentials of Computational Chemistry

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5.7 ONGOING DEVELOPMENTS IN SEMIEMPIRICAL MO THEORY 157<br />

test set. Such a reparameterization <strong>of</strong> a semiempirical Hamiltonian for a focused set <strong>of</strong><br />

molecules is completely analogous to the targeted parameterization <strong>of</strong> a force field, and the<br />

usual caveats apply with respect to application <strong>of</strong> a focused model to anything other than<br />

molecules falling within the target category.<br />

5.7.4 Linear Scaling<br />

As already touched upon in Section 2.4.2, the development <strong>of</strong> methods that scale linearly with<br />

respect to system size opens the door to the modeling <strong>of</strong> very large systems with maximal<br />

computational efficiency. Because the NDDO approximation is already rather efficient when<br />

it comes to forming the Fock matrix (because so many integrals are assumed to be zero,<br />

etc.), it serves as an excellent basis on which to build a linear-scaling QM model. Such<br />

models have been reported; the details associated with achieving linear scaling are sufficiently<br />

technical that interested readers are referred to the original literature (van der Vaart et al.<br />

2000; Khandogin, Hu, and York 2000; see also Stewart 1996).<br />

It is worth a pause, however, to consider how such models should best be used. Part <strong>of</strong><br />

the motivation for developing linear scaling models has been to permit QM calculations<br />

to be carried out on biomolecules, e.g., proteins or polynucleic acids. However, one may<br />

legitimately ask whether there is any point in such a calculation, beyond demonstrating that<br />

it can be done. Because <strong>of</strong> the relatively poor fashion with which semiempirical models<br />

handle non-bonded interactions, there is every reason to expect that such models would be<br />

disastrously bad at predicting biomolecular geometries – or at the very least inferior to the<br />

far more efficient force fields developed and optimized for this exact purpose.<br />

Instead, the virtue <strong>of</strong> the semiempirical models when applied to such molecules tends to<br />

be that they permit the charge distribution to be predicted more accurately given a particular<br />

structure. To the extent that biomolecules <strong>of</strong>ten employ charge–charge interactions to<br />

enhance reactivity and or specificity in the reaction and recognition <strong>of</strong> smaller molecules,<br />

such predictions can be quite useful. Since the QM calculation intrinsically permits polarization<br />

<strong>of</strong> the overall electronic structure, it is capable <strong>of</strong> showing greater sensitivity to<br />

group–group interactions as they modify the charge distribution than is the case for the<br />

typical fixed-atomic-charge, non-polarizable force field.<br />

Of course, one may also be interested in the modeling <strong>of</strong> a bond-making/bond-breaking<br />

reaction that takes place within a very large molecular framework, in which case the availability<br />

<strong>of</strong> appropriate force-field models is extremely limited and one must perforce resort to<br />

some QM approach in practice. Recognition <strong>of</strong> the complementary strengths and weaknesses<br />

<strong>of</strong> QM and MM models has led to extensive efforts to combine them in ways that allow<br />

maximum advantage to be taken <strong>of</strong> the good points <strong>of</strong> both; such QM/MM hybrid models<br />

are the subject <strong>of</strong> Chapter 13.<br />

5.7.5 Other Changes in Functional Form<br />

Two modifications to the fundamental forms <strong>of</strong> modern NDDO functions have been reported<br />

recently that merit particular attention. First, Weber and Thiel (2000) have reconsidered the

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