• Title/Summary/Keyword: $Al_XGa_1As_1$

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A Study on $E_1$Transition in Si-Doped $Al_{0.32}Ga_{0.68}As$by Electroreflectance Measurement (Electroreflectance 측정에 의한 Si이 첨가된 $Al_{0.32}Ga_{0.68}As$에서의 $E_1$ 전이에 대한 연구)

  • 김동렬;손정식;김근형;이철욱;배인호
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.11 no.9
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    • pp.687-692
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    • 1998
  • Silicon doped $Al_{0.32}Ga_{0.68}As$ were growth by molecular beam epitaxy. Electroreflectance(ER) spectra of the $E_1$ transition of Schottky barrier Au/n-$Al_{0.32}Ga_{0.68}As$ have been measured at various modulation voltage($V_{ac}$) and dc bias voltage($V_{bias}$). from the $E_1$peak, band gap energy of the $Al_{0.32}Ga_{0.68}As$ is 1.883 eV which corresponds to an Al composition of 32%. As modulation voltage($V_{bias}$) is changed, a line shape at the $E_1$transition does not change, but its amplitude varies linearly. The amplitude of $E_1$signal decrease with increasing the forward dc bias voltage($V_{bias}$), but the line shape does not change. It suggests that the low field theory rather than Franz-Keldysh oscillation is Required to interpret spectra. Also, spectra at the $E_1$transition were broadened with increasing the reverse dc bias voltage($V_{bias}$) which suggests the presence of Field-induced broadening.

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A model for neural trigger circuit using AlGaAs/GaAs MQW-IMD (AlGaAs/GaAs MQW-IMD를 사용하는 신경구동회로의 모델)

  • Song, Chung-Kun
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.32A no.4
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    • pp.47-56
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    • 1995
  • In this paper the model of the MQE-IMD-based neural trigger circuit is improved, where MQW-IMD is a new semiconductor device proposed and experimentally demonstrated by the author for the hardware implementation of the neural networks. The electron energy of AlXGa1-XAsbarrier is calculated by Ensemble Monte Carlo simulation according to the variation of Al mole fraction x and the applied electric field, whtich had been roughly estimated in the previous paper because of the difficulty to get the data. And in the consideration of the tunneling of the confined electrons within the quantum well the accuracy of the impact ionization rate is enhaned. Finally, the dependance of the frequency of pulse-train on the number of quantum wells can be calculated by modelling the effect of the distance of the induced positive charge from the cathode on the electric field at the cathode.

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