• Title/Summary/Keyword: CdTe/HgTe/CdTe

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A Calculation of C-V characteristics for HgCdTe Semiconductor material (HgCdTe 반도체 재료의 C-V 특성 계산)

  • Lee, S.D.;Kang, H.B.;Kim, B.H.;ADD, ATRC, D.H.Kim;Kim, J.M.
    • Proceedings of the KIEE Conference
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    • 1992.07b
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    • pp.813-815
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    • 1992
  • Accurate Capacitance-Voltage characteristics of Metal-Insulator-Semiconductor (MIS) devices in narrow band-gap semiconductors are presented. The unique band structure of narrow band-gap semiconductors is taken into account such as non-parabolicity and degeneracy. Compensated and partially ionized impurities either in the bulk or the space charge region are also considered. HgCdTe is a defect semiconductor, so this approach is very important for characterization and analysis of MIS devices.

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Tunneling Current Contribution to RoA of $Hg_{1-x}Cd_{x}$Te Photodiodes ($Hg_{1-x}Cd_{x}$Te 광다이오드에서 터널링 전류가 RoA에 미치는 영향)

  • 박장우;곽계달
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.29A no.10
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    • pp.42-48
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    • 1992
  • RoA is an important figure of merits for estimating the performance of p-n junction infrared detectors. This paper presents the tunneling current contribution to RoA of $Hg_{1-x}Cd_{x}$Te n$^{+}$-p juction photodiodes. Then, a diffusion model, a thermal generation-recombination model, an indirect tunneling model via trap, and a band-to-band direct tunneling model are considered to calculate RoA. Using these models, RoA depending on temperature, doping concentration, and mole fraction is calculated. Also from these results, under various operating conditions the dominant dark current mechanisms cna be understood.

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A study on the electron transport properties in HgCdTe using monte carlo method (몬테칼로 방법을 사용한 HgCdTe에서의 전자 전송 특성에 관한 연구)

  • 유상동;곽계달
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.35D no.2
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    • pp.40-51
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    • 1998
  • Electron transport properties are investigated by Monte Carlo simulation in n-HgCdTe. The material is easily degenerated at low temperature or being slightly doped, and is characterized by small band gap and large nonparabolic factor. The degeneracy is incorporated in the Monte Carlo simulation by taking into account the electron-electron scattering and the pauli exclusion principle. In the conventional method, however, the electron-electron scattering rate was developed under the assumption of parabolic conduction band. A new formulation of the electron-electron scattering rate is develop considering the band nonparabolicity and overlap integral. The electron-electron scattering effects on the electron distribution,impact ionization coefficienty, electron temperature, drift velocity and electron energy are presented.

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High Performance of SWIR HgCdTe Photovoltaic Detector Passivated by ZnS

  • Lanh, Ngoc-Tu;An, Se-Young;Suh, Sang-Hee;Kim, Jin-Sang
    • Journal of Sensor Science and Technology
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    • v.13 no.2
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    • pp.128-132
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    • 2004
  • Short wave infrared (SWIR) photovoltaic devices have been fabricated from metal organic vapour phase epitaxy (MOVPE) grown n- on p- HgCdTe films on GaAs substrates. The MOVPE grown films were processed into mesa type discrete devices with wet chemical etching employed for meas delineation and ZnS surface passivatlon. ZnS was thermally evaporated from effusion cell in an ultra high vacuum (UHV) chamber. The main features of the ZnS deposited from effusion cell in UHV chamber are low fixed surface charge density, and small hysteresis. It was found that a negative flat band voltage with -0.6 V has been obtained for Metal Insulator Semiconductor (MIS) capacitor which was evaporated at $910^{\circ}C$ for 90 min. Current-Voltage (I-V) and temperature dependence of the I-V characteristics were measured in the temperature range 80 - 300 K. The Zero bias dynamic resistance-area product ($R_{0}A$) was about $7500{\Omega}-cm^{2}$ at room temperature. The physical mechanisms that dominate dark current properties in the HgCdTe photodiodes are examined by the dependence of the $R_{0}A$ product upon reciprocal temperature. From theoretical considerations and known current expressions for thermal and tunnelling process, the device is shown to be diffusion limited up to 180 K and g-r limited at temperature below this.

Fabrication of a Large-Area $Hg_{1-x}Cd_{x}$Te Photovoltaic Infrared Detector ($Hg_{1-x}Cd_{x}$Te photovoltaic 대형 적외선 감지 소자의 제작)

  • Chung, Han;Kim, Kwan;Lee, Hee-Chul;Kim, Jae-Mook
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.31A no.2
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    • pp.88-93
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    • 1994
  • We fabricated a large-scale photovoltaic device for detecting-3-5$\mu$m IR, by forming of n$^{+}$-p junction in the $Hg_{1-x}Cd_{x}$Te (MCT) layer which was grown by LPE on CdTe substrate. The composition x of the MCT epitaxial layer was 0.295 and the hole concentration was 1.3${\times}10^{13}/cm^{4}$. The n$^{+}$-p junction was formed by B+ implantation at 100 keV with a does 3${\times}10^{11}/cm^{2}. The n$^{+}$ region has a circular shape with 2.68mm diameter. The vacuum-evaporated ZnS with resistivity of 2${\times}10^{4}{\Omega}$cm is used as an insulating layer over the epitaxial layer. ZnS plays the role of the anti-reflection coating transmitting more than 90% of 3~5$\mu$m IR. For ohmic contacts, gole was used for p-MCT and indium was used for n$^{+}$-MCT. The fabrication took 5 photolithographic masks and all the processing temperatures of the MCT wafer were below 90$^{\circ}C$. The R,A of the fabricated devices was 7500${\Omega}cm^{2}$. The carrier lifetime of the devices was estimated 2.5ns. The junction was linearly-graded and the concentration slope was measured to be 1.7${\times}10^{17}/{\mu}m$. the normalized detectivity in 3~5$\mu$m IR was 1${\times}10^{11}cmHz^{12}$/W, which is sufficient for real application.

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