Due to the reversal in electron counts for aromaticity and antiaromaticity in the closed-shell singlet state (normally ground state, S 0 )a nd lowest pp*t riplet state (T 1 or T 0 ), as given by Hückel's and Baird's rules, respectively,fulvenes are influenced by their substituents in the opposite manner in the T 1 and S 0 states. This effect is causedb yareversal in the dipole moment when going from S 0 to T 1 as fulvenes adapt to the differencei ne lectron counts for aromaticity in variouss tates;t hey are aromaticc hameleons. Thus, a substituent pattern that enhances (reduces) fulvene aromaticity in S 0 reduces (enhances) aromaticity in T 1 ,a llowing for rationalizationso ft he triplet state energies (E T )o fs ubstitut-ed fulvenes. Through quantum chemical calculations, we now assessw hich substituents and which positions on the pentafulvene core are the most powerful for designing compounds with low or inverted E T .A sam eans to increase the p-electron withdrawing capacity of cyano groups, we found that protonation at the cyano Na toms of 6,6-dicyanopentafulvenes can be ar oute to on-demandf ormation of af ulvenium dication with at riplet ground state (T 0 ). The five-membered ring of this speciesi sm arkedly Baird-aromatic, althoughl ess than the cyclopentadienyl cation knownt oh ave aB aird-aromatic T 0 state. [a] Dr.