the stimulated transition in the quantum system (e.g. an atom) will likewise produce zero electric field in that direction, so the radiated power at large distance will drop to zero along the plane perpendicular to it.
EDIT: I was wrong about the angular pattern of the stimulated emission, now I think only total radiation has this pattern. See below.
Yes, in case of dipole radiation, electric field component in the direction of wave propagation is zero in the radiation zone.
The simplest model of radiation from classical theory is that of oscillating charged particle (or oscillating dipole). The radiation goes in all directions from which the oscillation can be seen, the greater the projection of the acceleration vector seen, the greater the intensity of radiation. Mathematically, field strength of radiation varies as $\sin \theta$ in polar coordinates. This angular distribution is that of dipole radiator.
In quantum theory the radiation pattern depends on which transitions are involved in the interaction with EM field. The simplest cases are where the dominant contribution is that of "transition dipole moments" $\boldsymbol{\mu}_{ik} = \langle i|\sum_k q_k\mathbf r_k|k\rangle$. If only one such moment is involved (possible if the incident radiation is resonant with only one transition), the emitted radiation has the same dipole pattern as in classical theory, and has intensity given by the formula for spontaneous emission, independent of the incident radiation...
...except for intensity in direction of the incident wave, which does depend on intensity of incident radiation. Total intensity in the original direction is that of the spontaneous emission times a factor of $n+1$, where $n$ is number of photons in EM mode for this direction [1].
So total radiation emitted from the atom/molecule has dipole-like angular distribution, with a spike in the front. If we talk only about the stimulated emission part of that, this exists only in the original direction and is responsible for that spike.
[1] D. P. Craig, T. Thirunamachandran: Molecular Quantum Electrodynamics, formula 4.12.4., Academic Press (1984)