The concept of an optimal electron-phonon interaction spectral density as a
n Einstein spectrum which allows to describe all physical properties of a s
uperconductor in an optimal way is developed from Carbotte's original defin
ition of an optimum spectrum. It is shown, using the borocarbides YNi2B2C a
nd LuNi2B2C as examples, that such a concept is meaningful even for anisotr
opic systems. An Einstein spectrum is sufficient for clean-limit systems, a
2 delta -peak spectrum is better suited for anisotropic systems with impur
ities.