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Essentials of Computational Chemistry

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Link<br />

atom<br />

LSCF<br />

GHO<br />

13.4 EMPIRICAL VALENCE BOND METHODS 477<br />

A<br />

A<br />

A<br />

r AB<br />

r AB<br />

r AB<br />

MM region QM region<br />

q ABC<br />

B<br />

qABC B<br />

B<br />

w ABCX<br />

wABCX<br />

w ABCX<br />

q ABC<br />

qBCX r BC<br />

w<br />

r BCXY<br />

CX<br />

C H qCXY C<br />

qBCX r BC<br />

r BC<br />

C<br />

q BCX<br />

q CXH<br />

X<br />

w<br />

r BCXY<br />

CX<br />

qCXY r CX<br />

X<br />

w BCXY<br />

q CXY<br />

X<br />

Y<br />

w CXYZ<br />

Y<br />

w CXYZ<br />

Figure 13.6 Comparison <strong>of</strong> QM/MM partitioning schemes across covalent bonds. Included MM bond<br />

stretch, angle bend, and torsion terms are indicated; those that are boxed are ignored by some authors.<br />

Frozen orbitals are in gray for the LSCF and GHO methods<br />

Analytic derivatives have been reported for both the LSCF and GHO models, making them<br />

attractive options for MD simulations (Amara et al. 2000). Their generalization to ab initio<br />

levels <strong>of</strong> theory through the use <strong>of</strong> core pseudopotentials (along the lines <strong>of</strong> the pseudohalogen<br />

capping atoms described above) ensures that they will see continued development.<br />

13.4 Empirical Valence Bond Methods<br />

A method that has certain connections with QM/MM techniques even if it does not usually<br />

involve simultaneous evaluation <strong>of</strong> QM and MM operators during a particular calculation<br />

is the empirical valence bond method (EVB; Warshel and Weiss 1980). At the heart <strong>of</strong> the<br />

EVB method is the notion that arbitrarily complex reactions may be modeled as the influence<br />

<strong>of</strong> a surrounding environment on a fundamental process that may be represented by some<br />

combination <strong>of</strong> valence bond resonance structures. For example, the proton transfer from<br />

one water molecule to another may, at any point along the reaction path, be envisaged as<br />

involving some admixture <strong>of</strong> the two VB wave functions corresponding formally to<br />

1 = HO a –H ∗ + O b H2<br />

2 = HO a− + H ∗ –O b H2 +<br />

Y<br />

Z<br />

Z<br />

Z<br />

(13.8)<br />

(13.9)

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