We prove a theorem for coding mixed-state quantum signals. For a class
of coding schemes, the von Neumann entropy S of the density operator
describing an ensemble of mixed quantum signal states is shown to be e
qual to the number of spin-1/2 systems necessary to represent the sign
al faithfully. This generalizes previous works on coding pure quantum
signal states and is analogous to the Shannon's noiseless coding theor
em of classical information theory. We also discuss an example of a mo
re general class of coding schemes which beat the limit set by our the
orem.