G3(MP2) theory - again saving some time
G3(MP2) is a cheaper variant of G3 theory, in which the effects of basis set extension
are obtained from calculations at the MP2 level of theory. The G3(MP2) energy at
0 degrees Kelvin E0(G3MP2) is defined as:
E0(G3MP2) = E[QCISD(T,FC)/6-31G(d)//MP2(FULL)/6-31G(d)]
+ DE(G3MP2large)
+ DE(HLC)
+ ZPE
+ DE(SO)
The definition of the components being:
DE(G3MP2large) = E[MP2(FULL)/G3MP2large//MP2(FULL)/6-31G(d)] - E[MP2(FC)/6-31G(d)//MP2(FULL)/6-31G(d)]
DE(HLC) = -An(beta) - B(n(alpha) - n(beta))
A = 9.279 mHartrees; B = 4.471 mHartrees (for molecules)
A = 9.345 mHartrees; B = 2.021 mHartrees (for atoms)
n(alpha) = No. of alpha valence electrons
n(beta) = No. of beta valence electrons
ZPE = 0.8929 * ZPE[HF/6-31G(d)]
The necessary energies can be calculated most efficiently in the following sequence:
- Optimization and frequency calculation at the HF/6-31G(d) level of theory
- Optimization at the MP2(FULL)/6-31G(d) level of theory
- QCISD(T,FC)/6-31G(d)//MP2(FULL)/6-31G(d) single point
- MP2(FC)/G3MP2large//MP2(FULL)/6-31G(d) single point
Comments:
- Open shell systems are treated using unrestricted wavefunctions (UHF, UMP2 . . )
- The higher level correction (HLC) is included to compensate for remaining deficiencies
of the method. In contrast to G2 theory, separate values for parameters A and B have been
optimized for atoms and molecules to give the smallest average absolute deviation from
experiment. - Spin orbit correction terms E(SO) (mainly of experimental origin) are added only for atoms
- The G3MP2large basis set is almost identical to the G3large basis used in G3 except that
core polarization functions are not included. A local copy of the G3MP2large basis set can be found here. - In contrast to G3 theory, the MP2 single point calculation is performed within the
frozen core approximation (MP2(FC)). - The mean absolute devitiation for the extended G2 neutral set (148 reaction energies) is
1.18 kcal/mol.
Literature:
- L. A. Curtiss, K. Raghavachari,
"G2 Theory"
The Encyclopedia of Computational Chemistry, P. v. R. Schleyer (editor-in-chief),
John Wiley & Sons Ltd, Athens, USA, 1998, 2, 1104 - 1114. - L. A. Curtiss, P. C. Redfern, K. Raghavachari, V. Rassolov, J. A. Pople,
"Gaussian-3 theory using reduced Møller-Plesset order"
J. Chem. Phys. 1999, 110, 4703 - 4709.