A high-sensitivity In 0.6 Ga 0.4 As/GaAs quantum-dot infrared photodetector ͑QDIP͒ with detection wave band in 6.7-11.5 m and operating temperature up to 260 K under normal incident illumination has been demonstrated. The peak detection wavelength shifts from 7.6 to 8.4 m when the temperature rises from 40 to 260 K. The background limited performance ͑BLIP͒ detectivity (D BLIP * ) measured at V b ϭϪ2.0 V, Tϭ77 K, and p ϭ7.6 m was found to be 1.1 ϫ10 10 cm Hz 1/2 /W, with a corresponding responsivity of 0.22 A/W. The high operating temperature is attributed to the very low dark current and long carrier lifetime in the quantum dots of this device. The results show that this QDIP can operate at high temperature without using the large band gap material such as AlGaAs or InGaP as blocking barrier to reduce the device dark current.

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We studied the photoluminescence spectra of rapid-thermal-annealed self-assembled InAs quantum dots at 10 K. For annealing temperatures ranging from 700 to 950 °C, we observed a blueshift in the interband transition energies, a decrease in the intersublevel spacing energies, and a narrowing of photoluminescence linewidths. In this letter, we demonstrate that the tuning of the InAs quantum dots interband transition and intersublevel spacing energies can be achieved by 30 s of rapid thermal annealing. The relation between interband transition energy changes and the intersublevel spacing energies is found to be linear, with a slope close to the ratio of the dots’ height to their diameter.

We report on the matrix-dependent strain effect in self-assembled InAs quantum-dot heterostructures using photoluminescence measurements. A series of samples were prepared to examine the effect of quantum dot position with respect to the so-called strain-reducing layer (SRL). Since the SRL reduces the residual hydrostatic strain in the quantum dots, long emission wavelength of 1.34 μm is observed for the InAs quantum dots with an In0.16Ga0.84As SRL. The dependence of the emission wavelength on the thickness of the cap layer on SRL also indicates the importance of the role of matrix in the strain relaxation process of the dots. Using In0.16Al0.84As instead of In0.16Ga0.84As as the SRL, a blueshift in wavelength is observed because the elastic stiffness of In0.16Al0.84As is higher than that of In0.16Ga0.84As and less strain is removed from the dots with In0.16Al0.84As SRL.

We present a study of the hole emission processes in InAs/GaAs quantum dots using capacitance and admittance spectroscopies. From the conductance mapping, the hole levels show a quasicontinuous distribution, instead of the clear shell structures that have been observed in electron systems. According to a comparative analysis of the capacitance and admittance spectroscopies, the hole emission process is identified to be via thermally activated tunneling through the wetting layer as an intermediate state. An energy level diagram of the quantum dot is also constructed, which shows the hole in our quantum dots to be more weakly confined. We propose a general thermally activated tunneling model to explain our results and those in other works. The conclusion is that both the localization energy and the electric field are important for the carrier emission processes. This model is further extended to predict which carrier type ͑i.e., electron or hole͒ will be more relevant during the exciton dissociation processes in quantum dots.