The optimal rate at which information can be sent through a quantum channel
when the transmitted signal must simultaneously carry some minimum amount of
energy is characterized. To do so, we introduce the quantum-classical analogue
of the capacity-power function and generalize results in classical information
theory for transmitting classical information through noisy channels. We show
that the capacity-power function for a quantum channel, for both unassisted and
private protocol, is concave and also prove additivity for unentangled and
uncorrelated ensembles of input signals. This implies we do not need
regularized formulas for calculation. We numerically demonstrate these
properties for some standard channel models. We obtain analytical expressions
for the capacity-power function for the case of noiseless channels using
properties of random quantum states and concentration phenomenon in large
Hilbert spaces.Comment: 13 pages, 16 figure