“…29,30 The IPS observation also guarantees the molecular uniformity from the viewpoint of electronic structures because IPS is observable only on an atomically flat surface. 31,32 At hν 1 > 4.6 eV, another peak strongly appears at E F +3.17 eV, and it is maximized at hν 1 = 4.90 eV, implying a resonance electron−hole excitation involving occupied and unoccupied states. In fact, an ultraviolet photoelectron spectrum (UPS, Figure S5) shows a peak at E F −1.7 eV assignable to the highest occupied molecular orbital (HOMO) of the anthracene moiety, 27 and therefore, it is reasonable that the peak at E F +3.17 eV appears from the resonance electron excitation from the HOMO with hν 1 = 4.90 eV (≅3.17 + 1.7 eV).…”