Abstract
The joint density-of-states integral for production of a pair of elementary excitations in an isotropic fluid is studied as a function of energy and momentum. Isotropy permits one to take advantage of the essentially two-dimensional character of the system. Specializing to liquid He4 at T=0 °K, we show that certain abrupt variations in the density of states are associated with thresholds and saddle points in the energy function. The expected influence of these phenomena on S(k,ω) is described. Resonant pairs of excitations, as judged by their linesharpening effects, are shown to exist at special values of k and ω.