Transverse instabilities are investigated for the slab analog of the B
ennett equilibrium of a magnetically self-focused relativistic electro
n beam propagating through a plasma. Two kinds of plasma are considere
d: a channel matched to the beam and a broad uniform plasma. The high-
frequency electrostatic transverse two-stream instability and the lowe
r-frequency resistive-hose instability are treated analytically with a
distributed tune (''mass'') model. Asymptotic growth is computed for
each instability in various regimes, and analytic results are benchmar
ked against numerical solutions of the linearized system and particle-
in-cell simulations. It is found that in the limit of large collisionl
ess skin depth the electrostatic hose is the more virulent mode of bea
m breakup. Numerical examples are discussed for parameters in the rang
e considered for plasma focusing of the asymmetric beams of interest i
n high-energy physics.