  A theory of magnetophonon resonance in quantum wells in a magnetic field
tilted to the perpendicular to 2DEG is developed. The resonance is due to the
resonant interaction of 2D conduction electrons with the longitudinal optic
phonons. The electrons are assumed to be nondegenerate. The angular dependence
of the resonant maxima is investigated. The sharpness of the angular
dependence, as well as the existence of double resonances, i.e. two resonant
peaks for each resonance number is explained. A relation between the electron
concentration dependence of the resonance amplitude in the perpendicular
magnetic field and the angular dependence in the tilted field is analyzed.
Investigation of the angular dependence can give information concerning the
electron spectra, optic phonon and electron damping and the electron-phonon
interaction in quantum wells.
