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Second-Quantized Representation of Operators

  Operators involving systems of identical particles may be represented using annihilation and creation operators. As an example, we consider the one-electron hamiltonian

equation7032

where the summation runs over all N electrons. We may represent this operator in the basis of spin-orbitals as

  equation7036

where the closure relationship for the set of orbitals has been used. When tex2html_wrap_inline8307 operates on a determinantal function

eqnarray7046

where tex2html_wrap_inline8309 is the usual permutation operator. The fact that tex2html_wrap_inline8307 is invariant under permutation of electrons has been used to simplify the equation. If we now expand each term on the RHS using expression A.10, we obtain

eqnarray7064

This equation may be simplified using annihilation and creation operators by realizing that

equation7077

for example. (Why is this true, based on the definition of annihilation and creation operators?) So

eqnarray7083

Thus, tex2html_wrap_inline8307 may be written as

  equation7101

where the sum over q technically runs over only states occupied in the determinant upon which h acts. However, since q will give a zero result if q is not occupied in this determinant anyway, we may allow the sum to run over all orbitals without error.

Now examine the two-electron operator

equation7112

where the restricted summation runs over all N electrons. Represent this operator in the spin-orbital basis as

  equation7117

When tex2html_wrap_inline8327 operates on a determinantal wavefunction

eqnarray7127

The expansion (A.17) may be inserted above to obtain

eqnarray7144

Again we may simplify things by realizing that

equation7160

Thus

eqnarray7168

We can write tex2html_wrap_inline8327 compactly as

equation7195

where we have extended the sums over r and s to include all orbitals, and the factor of tex2html_wrap_inline8295 has been inserted to account for redundancies in r and s. Note that for the electronic Hamiltonian operator, tex2html_wrap_inline8341 . An equivalent expression for tex2html_wrap_inline8327 is

  equation7212

where tex2html_wrap_inline8345 is the standard antisymmetrized two-electron integrals and another factor of tex2html_wrap_inline8295 has been inserted to account for the additional redundancies introduced by this notation. Note that the form of equations (A.15) and (A.23) contains one- and two-electron integrals explicitly and neither depends on the number of electrons. These expressions will be invaluable in the evaluation of perturbation-theory and coupled-cluster theory equations, among others.  


next up previous contents index
Next: Usefulness of Second-Quantized Operators Up: Second Quantization Previous: Creation and Annihilation Operators

Emilio San Fabian
Mon Feb 5 10:35:31 WET 2001