Ab initio calculations were carried out to investigate various benzene dimers, including T‐shaped (T), parallel‐displaced (PD), herringbone‐type (Hb), face‐to‐face eclipsed (F2F‐E), and face‐to‐face staggered (F2F‐S) configurations in the lowest singlet (S1) and triplet (T1) excited states. Monomer and dimer geometries in the excited states were optimized at the scaled opposite‐spin (SOS) CIS(D0) level of theory, and their energetics were compared. In PD and edge‐on type dimer configurations (T and Hb), the exciton wavefunctions are localized mainly within single benzene molecules, making intermolecular interactions in the excited states nearly the same as those in the ground state. On the other hand, both the cofacial dimers (F2F‐E and F2F‐S) in the excited states present substantial enhancements in the binding energies, approximately ranging from 0.12 to 0.55 eV, compared to the ground state. However, further analyses of electronic couplings between the frontier molecular orbitals of each molecule demonstrate the significant difference between such dimers; unlike in the F2F‐E dimer, in the F2F‐S configuration, the excimer formation arises from coupling between different states of each monomer, e.g., the S1 state of one molecule and the S2 state of the other. In addition, for these cofacial dimers, the electronic coupling for triplet exciton is much weaker than that for its singlet counterpart, which can be rationalized by the different role of exchange energy in stabilizing respective states.