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QM/MM: CPMD/GROMOS<br />

• Long-­‐range: <br />

• Computed approximately by expanding the charge density of the QM <br />

system in terms of mul4poles up to quadrupolar order: <br />

QM −MM<br />

E es−lr<br />

⎧<br />

⎪ C<br />

= ∑ q I ⎨<br />

R I<br />

− R +<br />

I ∉NN<br />

⎩⎪<br />

+ 1 2<br />

∑<br />

i, j<br />

Q ij<br />

R I<br />

− R 5<br />

• Coefficients C, D i , Q ij are the usual mul4pole moments computed from the <br />

charge density n(r) of the QM subsystem with respect to the geometric <br />

center of the QM system, R = (R 1<br />

, R 2<br />

, R 3<br />

),<br />

where i=1,2,3 are the cartesian <br />

components. <br />

∑<br />

i<br />

• Refinement: third region between the other two: <br />

• Charge density approximately represented by (restraint) electrosta4c <br />

poten4al-­‐based (R/ESP) charges centered on the QM atoms as <br />

obtained from a dynamical fi~ng procedure or taken from the MM <br />

force field used. <br />

A. Laio, J. VandeVondele, U. Röthlisberger J. Chem. Phys. 2002, 116, 6941.<br />

D i<br />

R I<br />

− R 3<br />

( R Ii<br />

− R ) i<br />

( R Ii<br />

− R )( i<br />

R Ij<br />

− R ) j<br />

⎫<br />

⎪<br />

⎬<br />

⎭⎪

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