Quantum teleportation of an unknown broadband electromagnetic field is inve
stigated. The continuous-variable teleportation protocol by Braunstein and
Kimble [Phys. Rev. Leu. 80, 869 (1998)] for teleporting the quantum state o
f a single mode of the electromagnetic held is generalized for the case of
a multimode field with finite bandwith. We discuss criteria for continuous-
variable teleportation with various sets of input states and apply them to
the teleportation of broadband fields. We first consider as a set of input
fields (from which an independent state preparer draws the inputs to be tel
eported) arbitrary pure Gaussian states with unknown coherent amplitude (sq
ueezed or coherent states). This set of input states, further restricted to
an alphabet of coherent states, was used in the experiment by Furusawa et
al. [Science 282, 706 (1998)]. It requires unit-gain teleportation for opti
mizing the teleportation fidelity. In our broadband scheme, the excess nois
e added through unit-gain teleportation due to the finite degree of the squ
eezed-state entanglement is just twice the (entanglement) source's squeezin
g spectrum for its "quiet quadrature." The teleportation of one half of an
entangled state (two-mode squeezed vacuum state), i.e., "entanglement swapp
ing," and its verification are optimized under a certain nonunit gain condi
tion. We will also give a broadband description of this continuous-variable
entanglement swapping based on the single-mode scheme by van Loock and Bra
unstein [Phys. Rev. A 61., to 302 (2000)].