Set the ground electronic energy to zero and write the excitation energy as , or the characteristic temperature K. Counting each doubly degenerate manifold once gives the single-molecule electronic partition function
For independent molecules the electronic factor is . Hence the electronic internal energy is
The equal degeneracies cancel from the excited-state probability. At low temperature the ground manifold dominates and ; at high temperature both manifolds have equal populations, giving . These are electronic contributions only, excluding translation, rotation and vibration.

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