While ac multipactors between gaps have been extensively studied, traveling
wave multipactors, widely thought responsible for hub formation in cold-ca
thode crossed-field devices, have received much less attention. It is shown
that a single surface multipactor is induced by a slow wave with two-dimen
sional space variation. Phase locking with the rf occurs when the distance
traveled, and flight time between successive impacts correspond to a collis
ional drift velocity upsilon(c) = Delta y/Delta t equal to the phase veloci
ty upsilon(p). The flight time is not a multiple of the rf period, as in ac
multipactor, but closer to the cyclotron period. A stable resonant orbit i
s an attractor in space, pulling nearby orbits; in a rf-synchronous moving
window, particles cluster into a Larmor radius size ring, as the rest of th
e wavelength is swept clean. The bunched charge is later dispersed due to t
he mutual repulsion, creating a nonuniform hub. The parameter space where a
valanching occurs for secondary yield above unity is found much more extend
ed than for an ac multipactor. A crossed-field device based on secondary em
itting ("cold'') cathode must operate in the same parameter range. (C) 1999
American Institute of Physics. [S1070-664X(99)02901-8].