Heteroaromatic molecules are found in areas ranging from biochemistry to photovoltaics. We analyze the n,π* excited states of 6π-electron heteroaromatics with in-plane lone pairs (n σ , herein n) and use qualitative theory and quantum chemical computations, starting at Mandado's 2n + 1 rule for aromaticity of separate spins. After excitation of an electron from n to π*, a (4n + 2)π-electron species has 2n + 2 π α -electrons and 2n + 1 π β -electrons (or vice versa) and becomes π α -antiaromatic and π β -aromatic. Yet, the antiaromatic π α -and aromatic π β -components seldom cancel, leading to residuals with aromatic or antiaromatic character. We explore vertically excited triplet n,π* states ( 3 n,π*), which are most readily analyzed, but also singlet n,π* states ( 1 n,π*), and explain which compounds have n,π* states with aromatic residuals as their lowest excited states (e.g., pyrazine and the phenyl anion). If the π β -electron population becomes more (less) uniformly distributed upon excitation, the system will have an (anti)aromatic residual. Among isomers, the one that has the most aromatic residual in 3 n,π* is often of the lowest energy in this state. Five-membered ring heteroaromatics with one or two N, O, and/or S atoms never have n,π* states as their first excited states (T 1 and S 1 ), while this is nearly always the case for six-membered ring heteroaromatics with electropositive heteroatoms and/or highly symmetric (D 2h ) diheteroaromatics. For the complete compound set, there is a modest correlation between the (anti)aromatic character of the n,π* state and the energy gap between the lowest n,π* and π,π* states (R 2 = 0.42), while it is stronger for monosubstituted pyrazines (R 2 = 0.84).