Abstract
The superconducting energy gap and the transition temperature of a small grain of superconductor are larger than the corresponding quantities for bulk material. This results because the small dimensions cause a discrete, rather than continuous, spectrum of one-electron energy levels. This effect becomes important when the volume of the grain is comparable with, or smaller than, the characteristic volume λF2ξ0, where λF is the Fermi wavelength and ξ0 the T=0 Pippard coherence distance of the bulk material. As grain size is lowered, the ratio of T=0 energy gap to Boltzmann's constant times transition temperature gradually increases from the weak-coupling limit (3.528) to the strong-coupling limit (4.0).