• 제목/요약/키워드: GaP

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양자간섭소자를 위한 InGaAs/InGaAsP/InP 양자점 분자구조 연구 (Study on InGaAs/InGaAsP/InP Quantum-dot Molecules for Quantum Interference devices)

  • 김진석;김은규;정원국
    • 한국진공학회지
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    • 제15권2호
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    • pp.186-193
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    • 2006
  • 유기금속화학기상증착법으로 InGaAs/InGaAsP/InP 양자점 분자구조를 두 양자점 층간의 거리가 10 nm가 되도록 성장하여 성장된 구조에 대해 C-V, DLTS 및 PL 등의 전기 광학적 물성측정을 하였다. 그 결과 큰 양자점은 작은 양자점과 비교하여 장벽물질의 전도대역 가장자리로부터 먼 쪽에 에너지 준위가 형성되어 있음을 확인하였다. 큰 쪽 양자점에는 최소한 2개 이상의 에너지 준위에 운반자를 포획시킬 수 있음이 확인되었는데, -4 V의 역전압 하에서 측정된 양자점 분자구조의 에너지 준위는 장벽 가장자리로부터 0.35, 0.42, 0.45 eV 의 깊이에 각각 존재하였다. 인가된 전압의 변화에 대하여 약한 전기장 하에서는 양자점 분자구조의 에너지 준위들이 서로 결합되어 있다가 전기장이 증가하면서 이들 두 에너지 준위가 확연히 분리되는 모습을 확인할 수 있었다.

EDMln, TBP와 TBAs를 이용한 InP/GaAs와 GalnAs/GaAs의 MOVPE 성장 (Movpe Growth of InP/GaAs and GalnAs/GaAs from EDMln, TBP and TBAs)

  • 유충현
    • 한국전기전자재료학회논문지
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    • 제11권1호
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    • pp.12-17
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    • 1998
  • The heteroepitaxial growth of InP and GaInAs on GaAs substrates has been studied by using a new combination of source materials: ethyldimethylindium (EDMIn) and trimethylgallium (TMGa) as group III sources, and tertiarybutylarsine (TBAs) and tertiarybutylphosphine (TBP) as group V sources. Device quality InP heteroepitaxial layers were obtained by using a two-step growth process under atmospheric pressure, involving a growth of an initial nucleation layer at low temperature followed by high temperature annealing and the deposition of epitaxial layer at a growth temperature. The continuity and thickness of nucleation layer were important parameters. The InP layers deposited at 500$^{\circ}$- 55$0^{\circ}C$ are all n-type, and the electron concentration decreases with decreasing TBP/EDMIn molar ratio. The excellent optical quality was revealed by the 4.4 K photoluminescence (PL) measurement with the full width at half maximum (FWHM) of 4.94 meV. Epitaxial Ga\ulcorner\ulcorner\ulcornerIn\ulcorner\ulcorner\ulcornerAs layers have been deposited on GaAs substrates at 500$^{\circ}$ - 55$0^{\circ}C$ by using InP buffer layers. The composition of GaInAs was determined by optical absorption measurements.

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p형 GaP 반도체 계면의 광효과 (Photoeffects at p-GaP Semiconductor Interfaces)

  • Chun, Jang-Ho
    • 대한전자공학회논문지
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    • 제26권10호
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    • pp.1528-1534
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    • 1989
  • Photoeffects at the p-GaP semiconductor/CsNO3 electrolyte interface were investigated in terms of their current-voltage characteristics. The photoeffects at the semiconductor-electrolyte interfaces and their photocurrent variations are verified using Ar ion laser and continuous cyclic voltammetric methods. The mechanism of charge transfer at the photogeneration in the depletion layer rather than the photodecomposition of the p-GaP semiconductor electrode surface and/or the water photoelectrolysis. The adsorption of Cs+ ions at the interface is physical adsorption.

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AlGaAs/InGaAs/GaAs Pseudomorphic 구조의 MOCVD 성장 및 2차원 전자가스의 전송특성 (MOCVD Growth of AlGaAs/InGaAs/GaAs Pseudomorphic Structures and Transport Properties of 2DEG)

  • 양계모;서광석;최병두
    • 한국진공학회지
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    • 제2권4호
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    • pp.424-432
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    • 1993
  • AlGaAs/InGaAs/GaAs pseudomorphic structures have been grown by atmosheric pressure-MOCVD . The Al incorporation efficiency is constant but slightly exceeds the Ga incorporation during the growth of AlGaAs layers at $650^{\circ}C$ . Meanwhile , the In incorporation efficiency is constant but slightly less than the Ga incorporation in InGAAs layers. InGaAs/GaAs QWs were grown and their optical properties were characterized . $\delta$-doped Al0.24Ga0.76As/In0.16 Ga0.84As p-HEMT structures were successfully grown by MOCVD and their transport properties were characterized by Hall effect and SdH measurements. SdH Measurements at 3.7K show clear magnetoresistance oscillations and plateaus in the quantum Hall effect confirming the existence of a two-dimensional electron gas(2DEG) and a parallel conduction through the GaAs buffer layer. The fabricated $1.5\mu\textrm{m}$gatelength p-HEMTs having p-type GaAs in the buffer layer show a high transconductance of 200 mS/mm and a good pinch-off characteristics.

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p-type GaN의 Activation을 통한 광전기화학적 특성 향상 (Improvement of Photoelectrochemical Properties through Activation Process of p-type GaN)

  • 방승완;김하성;배효정;주진우;강성주;하준석
    • 마이크로전자및패키징학회지
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    • 제24권4호
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    • pp.59-63
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    • 2017
  • n-type GaN 반도체는 광전극으로서 우수한 성질을 가지고 있지만, 표면에서 일어나는 산소반응으로 인한 광부식으로 신뢰성이 저하되는 큰 단점이 있다. 이를 근본적으로 억제하기 위하여 표면에서 수소 발생 반응이 일어나는 p-type GaN를 광전극으로 사용함으로써 광부식을 피하고자 하는 연구가 진행되고 있다. 하지만 p-type GaN은 비저항이 높고 정공 이동도가 낮기 때문에 효율이 낮다는 단점을 가지고 있다. 본 연구에서는 이러한 문제를 p-type GaN의 activation 공정을 통해 개선하고자 한다. 전극으로 사용될 p-type GaN을 $N_2$ 분위기의 $500^{\circ}C$에서 1 분 동안 annealing을 하였다. Hall effect 측정을 통하여 전기적 특성을 확인하였으며, potentiostat (PARSTAT4000) 측정을 통하여 광전기화학적 (photoelectrochemical, PEC) 특성을 분석하였다. 그 결과 annealing 공정을 통하여 광전류밀도가 1.5배 이상 향상되었으며, 3시간 동안 안정적인 광전류 값을 확인하였다.

반도체 나노와이어에서 전자방출 안정성 (Emission Stability of Semiconductor Nanowires)

  • 유세기;정태원;이상현;허정나;이정희;이철진;김진영;이형숙;국윤필;김종민
    • 한국진공학회지
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    • 제15권5호
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    • pp.499-505
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    • 2006
  • 열 화학기상법으로 만든 GaN와 GaP 나노와이어에서 전계 방출과, 산소와 아르곤 분위기에서 안정성에 대해 조사하였다. GaN 나노와이어의 경우 산소 분위기에서 전계 방출이 급격하게 줄었으나, GaP에서는 그렇지 않았다. 두 나노와이어 모두 아르곤 분위기에서는 큰 변화가 없었다. GaP 나노와이어의 외부에 존재하는 산화물 층이 전자 방출 안정성에 크게 기여한 것으로 생각된다. 나노와이어에서 방출된 전자의 에너지 분포를 통해 반도체 나노와이어는 탄소 나노튜브와 그 전계 방출 메카니즘이 다름을 유추할 수 있었다.

Chalcopyrite (Al,Ga)As 반도체와 Mn의 반금속 강자성 (Half-metallic Ferromagnetism for Mn-doped Chalcopyrite (Al,Ga)As Semiconductor)

  • 강병섭;송기문
    • 반도체디스플레이기술학회지
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    • 제19권3호
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    • pp.49-54
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    • 2020
  • We studied the electronic and magnetic properties for the Mn-doped chalcopyrite (CH) AlAs, GaAs, and AlGaAs2 semiconductor by using the first-principles calculations. The chalcopyrite AlGaP2, AlGaAsP, and AlGaAs2 compounds have a semiconductor characters with a small band-gap. The interaction between Mn-3d and As-4p states at the Fermi level dominate rather than the other states. The ferromagnetic ordering of dopant Mn with high magnetic moment is induced due to the Mn(3d)-As(4p) strong coupling, which is attributed by the partially filled As-4p bands. The holes are mediated with keeping their 3d-electrons, therefore the ferromagnetic state is stabilized by this double-exchange mechanism. We noted that the ferromagnetic state with high magnetic moment is originated from the hybridized As(4p)-Mn(3d)-As(4p) interaction mediated by the holes-carrier.

Kinetic Study on the Low-lying Excited States of Ga Atoms in Ar

  • Kuntack Lee;Ju Seon Goo;Ja Kang Ku
    • Bulletin of the Korean Chemical Society
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    • 제15권8호
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    • pp.663-669
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    • 1994
  • Decay kinetics of Ga(5s), Ga(5p) and Ga(4d) atoms in Ar were studied by laser induced fluorescence technique. Theground state gallium atoms in the gas phase were generated by pulsed dc discharge of trimethyl gallium and argon mixtures. Both pulsed discharge and YAG-DYE laser system were controlled by a dual channel pulse generator and the delay time between the end of discharge and laser pulses was set 3.0-6.0 ms. The Ga(5s) and Ga(4d) atoms were generated by single photon excitation from the ground state Ga atoms and radiative lifetimes as well as the total quenching rate constants in Ar were obtained from the pressure dependence of the fluorescence decay rates. The Ga(5p) atoms were populated by a two-photon excitation method and the cascade fluorescence from Ga(5s) atoms were analyzed to extract quenching rate constant of Ga(5p) atoms by Ar in addition to radiative lifetimes of Ga(5p) state. The magnitudes of the quenching rate constants by Ar for the low-lying excited states of Ga atoms are 1.6-3$ {\times}10^{-11}cm^3$ molecul$e^{-1}s^{-1}$, which are much larger than those for alkali, alkaline earth and Group 12 metals. Based on the measured rate constants, kinetic simulations were done to assign state-to-state rate constants.

n-ZnO/i-ZnO/p-GaN:Mg 이종접합을 이용한 UV 발광 다이오드 (Ultraviolet LEDs using n-ZnO:Ga/i-ZnO/p-GaN:Mg heterojunction)

  • 한원석;김영이;공보현;조형균;이종훈;김홍승
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2008년도 추계학술대회 논문집 Vol.21
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    • pp.50-50
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    • 2008
  • ZnO has been extensively studied for optoelectronic applications such as blue and ultraviolet (UV) light emitters and detectors, because it has a wide band gap (3.37 eV) anda large exciton binding energy of ~60 meV over GaN (~26 meV). However, the fabrication of the light emitting devices using ZnO homojunctions is suffered from the lack of reproducibility of the p-type ZnO with high hall concentration and mobility. Thus, the ZnO-based p-n heterojunction light emitting diode (LED) using p-Si and p-GaN would be expected to exhibit stable device performance compared to the homojunction LED. The n-ZnO/p-GaN heterostructure is a good candidate for ZnO-based heterojunction LEDs because of their similar physical properties and the reproducibleavailability of p-type GaN. Especially, the reduced lattice mismatch (~1.8 %) and similar crystal structure result in the advantage of acquiring high performance LED devices with low defect density. However, the electroluminescence (EL) of the device using n-ZnO/p-GaN heterojunctions shows the blue and greenish emissions, which are attributed to the emission from the p-GaN and deep-level defects. In this work, the n-ZnO:Ga/p-GaN:Mg heterojunction light emitting diodes (LEDs) were fabricated at different growth temperatures and carrier concentrations in the n-type region. The effects of the growth temperature and carrier concentration on the electrical and emission properties were investigated. The I-V and the EL results showed that the device performance of the heterostructure LEDs, such as turn-on voltage and true ultraviolet emission, developed through the insertion of a thin intrinsic layer between n-ZnO:Ga and p-GaN:Mg. This observation was attributed to a lowering of the energy barriers for the supply of electrons and holes into intrinsic ZnO, and recombination in the intrinsic ZnO with the absence of deep level emission.

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III-V 화합물 반도체 마이크로머시닝을 위한 InP를 기반으로 한 미세구조의 제조에 관한 연구 (Fabrication of InP-Based Microstructures for III- V Compound Semiconductor Micromachining)

  • 심준환;노기영;이종현;황상구;홍창희
    • 한국정보통신학회논문지
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    • 제4권5호
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    • pp.1151-1156
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    • 2000
  • 본 논문에서는 III-V 화합물 반도체 마이크로머시닝을 위한 InP를 기반으로한 미세구조의 제조에 관하여 보고한다. InP/InGaAsP/InP 구조를 성장시키기 위하여 수직 LPE 시스템을 사용하였다. 성장된 InGaAsP층의 두께는 $0.4\mum$이고, InP top-layer의 두께는 $1\mum$이었다. InGaAsP 미세구조의 제조는 front-side 벌크 마이크로 머시닝으로 이루어졌다. 실험결과에서 <100> 방향으로 놓인 빔의 에칭이<110>와 <110> 방향에서의 에칭보다 더 빠르기 때문에 빔은 <100> 방향으로 정렬되어야 함을 보였다.

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