A theory of pulsar radio emission generation, in which the observed waves a
re produced directly by maser-type plasma instabilities operating at the an
omalous cyclotron-Cherenkov resonance omega - k(parallel to)v(parallel to)
+ omega(B)/gamma(res) = 0 and the Cherenkov drift resonance omega - k(paral
lel to)v(parallel to) - k(perpendicular to)u(d) = 0, is capable of explaini
ng the main observational characteristics of pulsar radio emission. The ins
tabilities are due to the interaction of the fast particles from the primar
y beam and the tail of the distribution with the normal modes of a strongly
magnetized one-dimensional electron-positron plasma. The waves emitted at
these resonances are vacuum-like, electromagnetic waves that may leave the
magnetosphere directly, In this model, the cyclotron-Cherenkov instability
is responsible for the core-emission pattern and the Cherenkov drift instab
ility produces conal emission. The conditions for the development of the cy
clotron-Cherenkov instability are satisfied for both typical and millisecon
d pulsars provided that the streaming energy of the bulk plasma is not very
high gamma(p) approximate to 10, In a typical pulsar the cyclotron-Cherenk
ov and Cherenkov drift resonances occur in the outer parts of the magnetosp
here at r(res) approximate to 10(9) cm, This theory can account for various
aspects of pulsar phenomenology, including the morphology of the pulses, t
heir polarization properties and their spectral behaviour. We propose sever
al observational tests for the theory. The most prominent prediction is the
high altitudes of the emission region and the linear polarization of conal
emission in the plane orthogonal to the local osculating plane of the magn
etic field.