Quantum dots are clusters of atoms (or molecules) that are small enough tha
t their electronic states are discrete. They can be prepared with a variety
of compositions and covering ligands but Bare not quite identical. In part
icular, the dots will have a variable size. The study of the properties of
individual dots is an active subject in its own right. Here we examine the
electronic structure of assemblies of dots, where the dots are near enough
that they interact. For the purpose of an elementary discussion, metallic d
ots are regarded as "atoms" with one valence orbital. The key point is at t
hey are "designer" atoms because their electronic properties be controlled
through the synthetic method that is used to prepare the dots. Of direct co
ncerns to us are the size of the dot and the nature of the ligands used to
passivate the dots so that they do not coalesce. An important parameter is
the energy cost, I, of adding an electron to a dot. The large size of the d
ots means that, unlike ordinary atoms, the Coulomb repulsion of the added e
lectron is low. Other experimental control parameters are externally applie
d and include the ability to compress an assembly S of dots, and thereby ch
ange the distance between them, or to subject them to static or alternating
electromagnetic fields. The response to spectral probes:for the electronic
structure is discussed with special emphasis on: new features, such as the
onset of conjugation or the insulator-to-metallic transition made accessib
le by the low charging energy of the dots. We propose a-phased diagram of e
lectronic isomers that can be: accessed under realistic conditions.