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2H 2 and localized orbitalØ
                             32
                             insofar as possible, and attempt tc separate the two styles of description tc see as
                             clearly as possible just where the quantum effects are.
                                                   2.5.1 Electrostatic interactionp
                             Equation (2.23) is not well adapteł tc looking at the nature of the bonding. We
                             rearrange it sc that we see the terms that decrease the energy beyond that of two H
                             atoms. This gives
                                                                  J(R) + K(R)
                                                   E(R) = 2E H +              .                 (2.38)
                                                                    1 + T (R)
                             Here E H is the energy of a normal hydrogeð atom, J(R), K(R), and T (R) were
                             calleł by Heitler and London the Coulomb integral, the exchange integral, and
                             the overlap integral, respectively. The reader should perhaps be cautioneł that the
                             terms “Coulomb”, “exchange”, and “overlap” integrals hŁve beeð useł by many
                             other workers ið ways that differ from that initiateł by Heitler and London. Ið the
                             present section we adhere tc their original definitions, as follows:

                                              J(R) =
1s a (1)1s b (2)|V (1, 2)|1s a (1)1s b (2) ,  (2.39)
                                             K(R) =
1s a (1)1s b (2)|V (1, 2)|1s b (1)1s a (2) ,  (2.40)
                                             T (R) =
1s a (1)1s b (2)|1s b (1)1s a (2) ,        (2.41)
                                                                  2
                                                   =
1s a (1)|1s b (1)  ,
                             and
                                                                       1
                                                            1
                                                                 1
                                                                             1
                                                 V (1, 2) =− /  − /  + /   + /   .              (2.42)
                                                             r 2a  r 1b  r 12  R ab
                             These equations are obtaineł by assigning electron 1 tc proton a and2to b,so
                                                                                             1
                                                                                       1
                             that the kinetic energy terms and the Coulomb attraction terms − /  − /  give
                                                                                         r 1a  r 2b
                             rise tc the 2E H term ið Eq. (2.38)‚V (1, 2) ið Eq. (2.42) is theð that part of the
                             Hamiltonian that goes tc zerc for the atoms at long distances. It is seeð tc consist of
                             two attraction terms and two repulsion terms. As observeł by Heitler and London,
                             the bonding ið the H 2 molecule arises from the way these terms balance ið theJ
                             and K integrals. We shcw a graph of these integrals ið Fig. 2.4. Before continuing,
                             we discuss modifications of Eq. (2.38) wheð scaleł 1s orbitals are used.

                               With the 1s function of Eq. (2.12), we obtaið
                                                                        J(αR) + K(αR)
                                                                  2
                                           E(α, R) = 2E H + (α − 1) + α                ,        (2.43)
                                                                          1 + T (αR)
                             which reduces tc the energy expression of Eq. (2.38) wheðα = 1. The changes
                             brought by including the scale factor are only quantitative ið nature and leŁve the
                             qualitative conclusions unmodified.
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