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The framework of linearised laser equations for the field and charge carriers is used to obtain an analytic expression which describes the modulation response function of a semiconductor laser and takes account of spatially inhomogeneous gain saturation caused by a standing wave. Account is also taken of spatial variations of the carrier density along the cavity axis, which appear because of different rates of stimulated recombination near the standing-wave nodes and antinodes, and because of 'expulsion' of free carriers from the wave antinodes by electrostriction forces. It is shown that the influence of the standing wave leads to a change in the response function near a resonant frequency ƒ 0 and has a minor effect on the value of this function at frequencies exceeding ƒ 0 . Therefore, this influence has practically no effect on the maximum modulation frequency ƒ m of a semiconductor laser.
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Alexandr P Bogatov (1997) studied this question.
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