QuantumDots: APrimerINTRO DUCTION C r y stallin e in organic so lid s can be divided electronically into three well-known classes: m etals, semiconductors, and insulators. In these extended solids, atomic orbitals overlap to give nearly continuous electronic energy levels known as bands.1 M etals are electronically characterized by having a partially lled band; semiconductors have a lled band (the valence band) separated from the (mostly) empty conduction band by a bandgap E g , corresponding to the familiar HOMO-LUM O energy gap for small m olecules. Insulators are conceptually the sam e as sem ico nd uctors in their electronic structure, except that the bandgap is larger in insulators (Fig. 1). In terms of E g s, m etals have E g less than ;0.1 eV; semiconductors have E g s from ;0.5 to ;3.5 eV; and insulators have E g . ;4 eV. (1 eV 5 1.602 3 10 2 19 J 5 8065.5 cm 2 1 ). There are some key differences, how ever, b etw een the electronic structure of m olecules and solid-state materials such as semiconductors.