Abstract. Because of the implications for plasmas in the laboratory and in space, attention has been drawn to inhomogeneous energy-density driven (IEDD) waves that are sustained by velocity-shear-induced inhomogeneity in crossfield plasma flow. These waves have a frequency ω r in the lab frame within an order of magnitude of the ion gyrofrequency ω ci , propagate nearly perpendicular to the magnetic field (k z /k ⊥ 1), and can be Landau resonant (0 < ω 1 /k z < ν d ) with a parallel drifting electron population (drift speed ν d ), where subscripts 1 and r indicate frequency in the frame of flowing ions and in the lab frame, respectively, and k z is the parallel component of the wavevector. A transition in phase velocity from 0 < ω 1 /k z < ν d to 0 > ω 1 /k z > ν d for a pair of IEDD eigenmodes is observed as the degree of inhomogeneity in the transverse E × B flow is increased in a magnetized plasma column. For weaker velocity shear, both eigenmodes are dissipative, i.e. in Landau resonance, with k z ν d > 0. For stronger shear, both eigenmodes become reactive, with one's wavevector component k z remaining parallel, but with ω 1 /k z > ν d , and the other's wavevector component k z becoming anti-parallel, so that 0 > ω 1 /k z . For both eigenmodes, the transition (1) involves a small frequency shift and (2) does not involve a sign change in the wave energy density, which is proportional to ω r ω 1 , both of which are previously unrecognized aspects of inhomogeneous energydensity driven waves.