G3(MP2)B3 theory - the most economical method

G3(MP2)B3 is an adaption of G3(MP2) theory based on geometries and zero point vibrational
energies calculated at the Becke3LYP/6-31G(d) level of theory. The G3(MP2)B3 energy at
0 degree Kelvin E0(G3MP2B3) is defined as:

E0(G3MP2B3) = E[QCISD(T,FC)/6-31G(d)//B3LYP/6-31G(d)]
        + DE(G3MP2large)
        + DE(HLC)
        + ZPE
        + DE(SO)

The definition of the components being:

DE(G3MP2large) = E[MP2(FC)/G3MP2large//B3LYP/6-31G(d)] - E[MP2(FC)/6-31G(d)//B3LYP/6-31G(d)]

DE(HLC) = -An(beta) - B(n(alpha) - n(beta))
                     A = 10.041 mHartrees; B = 4.995 mHartrees (for molecules)
                     A = 10.188 mHartrees; B = 2.323 mHartrees (for atoms)
                     n(alpha) = No. of alpha valence electrons
                     n(beta) = No. of beta valence electrons

ZPE = 0.960 * ZPE[B3LYP/6-31G(d)]

The necessary energies can be calculated most efficiently in the following sequence:

Comments:

Literature: