analogy with its classical counterpart, a noisy quantum channel is cha
racterized by a loss, a quantity that depends on the channel input and
the quantum operation performed by the channel. The loss reflects the
transmission quality: if the loss is zero, quantum information can be
perfectly transmitted at a rate measured by the quantum source entrop
y. By using block coding based on sequences of II entangled symbols, t
he average loss (defined as the overall loss of the joint n-symbol cha
nnel divided by n, when n-->infinity) can be made lower than the loss
for a single use of the channel. In this context, we examine several u
pper bounds on the rate at which quantum information can be transmitte
d reliably via a noisy channel, that is, with an asymptotically vanish
ing average loss while the one-symbol loss of the channel is nonzero.
These bounds on the channel capacity rely on the entropic Singleton bo
und on quantum error-correcting codes [Phys. Rev. A 56, 1721 (1997]. F
inally, we analyze the Singleton bounds when the noisy quantum channel
is supplemented with a classical auxiliary channel.