361chromism is identical to the first-order term of the present theory LEq. (35) j. Hoffmann's results are contained, as an approximation, in the present theory.For completeness, we point out discussions of the hypochromism problem by McLachlan and Bal1. , " Fowler, ' and Bullough, " whose conclusions are in general agreement with ours.The theory, therefore, contains nothing which is basically new, but does serve to coordinate previous theories under one "theoretical roof". Ke feel that, because of the generality, directness, and completeness of the approa, ch, the use of linear response (retarded) Green's functions will point the way to better approximation methods.The same method should be readily applicable to other optical phenomena, besides absorption, such as rotatory dispersion and molecular crystal reQection.This article presents a simplified treatment of the high density, collisionless, free-electron gas, based on the ideas of a wave number and frequency-dependent conductivity and dielectric constant. The formalism is applied to solve a number of problems: the screening of the electrostatic potential of a foreign point charge placed in the electron gas, the rate of energy loss of a charged particle moving through the electron gas, plasma oscillations, the reflection of electromagnetic waves from the electron gas, and ultrasonic attenuation in metals due to the interaction of the sound waves with the conduction electrons. In a Anal section it is indicated how the methods may be generalized. Explicit expressions for the conductivity of the electron gas are obtained in an appendix. ' J. Lindhard, Kgl. Danske Videnskab. Selskab, Mat. -I'ys.