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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 />
⎭⎪