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2nd Order MP Energy

  From Eqn 44 we have
 eqnarray1282
To get the second order energy, we need to determine which of the excited determinants tex2html_wrap_inline3963 in Eqn 51 (or Eqn 55) can couple with the ground state reference wavefunction tex2html_wrap_inline3965 through tex2html_wrap_inline3837.

Ground State tex2html_wrap_inline3969 of Eqn 51 must be zero due to intermediate normalization.

Single Excitations
eqnarray1307
Single exitations also do not couple with the ground state reference determinant (i.e. tex2html_wrap_inline3971).

Double Excitations
eqnarray1344
Thus double excitations can couple with the reference wavefunction.

Higher Order Excitations
Due to the two particle nature of tex2html_wrap_inline3837, higher order excitations are unable to couple with the reference.

By summing over all possible double excitations Eqn 60 can be simplified.
eqnarray1371
Thus the MP2 energy is
eqnarray1387

So far our treatment has been solely in terms of spin orbitals. However, if we consider only closed shell systems with a RHF wavefunction the second order MPPT energy correction is greatly simplified. For an N electron system
eqnarray1399
Here a, b, r, s, are indices for spatial orbitals. Notation will revert to that for spin orbitals in the following derivations of the higher order MPPT energy corrections.



Greg Tschumper
Mon Oct 6 09:20:38 EDT 1997