For two orbitals a and b and the electron repulsion e2/4πε0r12, the exchange integral is
Kab=∬a(1)b(2)4πε0r12e2b(1)a(2)dτ1dτ2,
the same integral as the classical electron repulsion Jab (with a(1)b(2) on both sides) except that the electrons are swapped on one side. Kab is positive and has no classical counterpart.
Examples
Example 2.9 (The exchange integral of helium, measured)
The 1s2s levels of helium lie at 159856cm−1 (3S) and 166277cm−1 (1S) above the ground state: the singlet is 6421cm−1, 0.796eV, higher, and K(1s,2s)=0.398eV. The figure below shows the two families.