IntroductionUltrafast all-optical switches operating in the 1.55 µm waveband are among the most important devices in highbit-rate optical fiber communication systems. The planartype switches are especially attractive for dense parallel processing and simultaneous multichannel demultiplexing. Recently, we have proposed planar-type optical Kerr gate switches based on GaAs/AlAs multilayer cavity structures.[1] The strong internal light intensity due to the cavity effect yields drastic enhancement of nonlinear phase shift in the half-wave length (λ/2) cavity layer. Moreover, the optical Kerr signal intensity caused by the nonlinear phase shift can be further enhanced by using excellent nonlinear materials only in the λ/2 cavity layer. InAs quantum dots (QDs) in the 1.55 µm waveband are one of desirable nonlinear materials in the λ/2 cavity layer, since state filling in the QDs at low-excitation-power results in the large nonlinear refractive index change. [2,3] However, a slow decay (~ ns) of photogenerated carriers in the QDs is a crucial problem for the high-bit-rate operation because it leads to a strong dependence of response signal intensity on the pattern of pulse trains (pattern effect). In our recent study, self-assembled InAs QDs were successfully formed on strain-relaxed In 0.35 Ga 0.65 As barrier by molecular beam epitaxy (MBE).[4] The 20-layer stacked InAs QDs with strain-relaxed barriers showed optical absorption in the wavelength range of 1.35-1.65 µm. The fast carrier relaxation of 12-18 ps was demonstrated for the excitation wavelength of 1. 35-1.55 µm, [5] which comes from carrier relaxation into the nonradiative centers arising from the crystal defects related to the lattice-relaxation.In this paper, we report on successful fabrication of the GaAs/AlAs multilayer cavity structure with InAs QDs embedded in strain-relaxed barriers grown by MBE. Two InAs QD layers were inserted into the λ/2 cavity layer consisting of the strain-relaxed In 0.35 Al 0.65 As and In 0.35 Ga 0.65 As barriers. Decay of phtogenerated carriers in the QD-cavity sample was characterized by time-resolved transmission change measurement based on a pump-probe technique.