• Title/Summary/Keyword: InAlAs/AlGaAs

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Growth of GaAs/AlGaAs structure for photoelectric cathode (광전음극 소자용 GaAs/AlGaAs 구조의 LPE 성장)

  • Bae, Sung Geun;Jeon, Injun;Kim, Kyoung Hwa
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.27 no.6
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    • pp.282-288
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    • 2017
  • In this paper, GaAs/AlGaAs multi-layer structure was grown by liquid phase epitaxy with graphite sliding boat, which can be used as a device structure of a photocathode image sensor. The multi-layer structure was grown on an n-type GaAs substrate in the sequence as follows: GaAs buffer layer, Zn-doped p-type AlGaAs layer as etching stop layer, Zn-doped p-type GaAs layer, and Zn-doped p-type AlGaAs layer. The Characteristics of GaAs/AlGaAs structures were analyzed by using scanning electron microscope (SEM), secondary ion mass spectrometer (SIMS) and hall measurement. The SEM images shows that the p-AlGaAs/p-GaAs/p-AlGaAs multi-layer structure was grown with a mirror-like surface on a whole ($1.25mm{\times}25mm$) substrate. The Al composition in the AlGaAs layer was approximately 80 %. Also, it was confirmed that the free carrier concentration in the p-GaAs layer can be adjusted to the range of $8{\times}10^{18}/cm^2$ by hall measurement. In the result, it is expected that the p-AlGaAs/p-GaAs/p-AlGaAs multi-layer structure grown by the LPE can be used as a device structure of a photoelectric cathode image sensor.

Improved Uniformity of GaAs/AlGaAs DBR Using the Digital Alloy AlGaAs Layer (디지털 합금 AlGaAs층을 이용하여 제작된 GaAs/AlGaAs DBR의 균일도 향상)

  • Cho, N.K.;Song, J.D.;Choi, W.J.;Lee, J.I.;Jeon, Heon-Su
    • Journal of the Korean Vacuum Society
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    • v.15 no.3
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    • pp.280-286
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    • 2006
  • A distributed Bragg reflector (DBR) for the application of $1.3{\mu}m$ vertical cavity surface emitting laser (VCSEL) has grown by digital-alloy AlGaAs layer using the molecular beam epitaxy (MBE) method. The measured reflection spectra of the digital-alloy AlGaAs/GaAs DBR have uniformity in 0.35% over the 1/4 of 3-inch wafer. Furthermore, the TEM image showed that the composition and the thickness of the digital-alloy AlGaAs layer in AlGaAs/GaAs DBR was not affected by the temperature distribution over the wafer whole surface. Therefore, the digital-alloy AlGaAs/GaAs DBR can be used to get higher yield of VCSEL with the active medium of InAs quantum dots whose gain is inhomogeneously broadened.

Fabrication of a depletion mode p-channel GaAs MOSFET using $Al_2O_3$ gate insulator ($Al_2O_3$ 게이트 절연막을 이용한 공핍형 p-채널 GaAs MOSFET의 제조)

  • Jun, Bon-Keun;Lee, Tae-Hyun;Lee, Jung-Hee;Lee, Yong-Hyun
    • Journal of Sensor Science and Technology
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    • v.8 no.5
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    • pp.421-426
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    • 1999
  • In this paper, we present p-channel GaAs MOSFET having $Al_2O_3$ as gate insulator fabricated on a semi-insulating GaAs substrate, which can be operated in the depletion mode. $1\;{\mu}m$ thick undoped GaAs buffer layer, $4000\;{\AA}$ thick p-type GaAs epi-layer, undoped $500{\AA}$ thick AlAs layer, and $50\;{\AA}$ thick GaAs cap layer were subsequently grown by molecular beam epitaxy(MBE) on (100) oriented semi-insulating GaAs substrate and this wafer was oxidized. AlAs layer was fully oxidized as a $Al_2O_3$ thin film. The I-V, $g_m$, breakdown charateristics of the fabricated GaAs MOSFET showed that wet thermal oxidation of AlAs/GaAs epilayer/S I GaAs was successful in realizing depletion mode p-channel GaAs MOSFET.

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Fabrication of a Depletion mode n-channel GaAs MOSFET using $Al_2O_3$ as a gate insulator ($Al_2O_3$ 절연막을 게이트 절연막으로 이용한 공핍형 n-채널 GaAs MOSFET의 제조)

  • Jun, Bon-Keun;Lee, Suk-Hyun;Lee, Jung-Hee;Lee, Yong-Hyun
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.37 no.1
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    • pp.1-7
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    • 2000
  • In this paper, we present n-channel GaAs MOSFET having $Al_2O_3$ as gate in insulator fabricated on a semi-insulating GaAs substrate. 1 ${\mu}$m thick undoped GaAs buffer layer, 1500 ${\AA}$ thick n-type GaAs, undoped 500 ${\AA}$ thick AlAs layer, and 50 ${\AA}$ GaAs caplayer were subsequently grown by molecular beam epitaxy(MBE) on (100) oriented semi-insulating GaAs substrate oxidized. When it was wet oxidized, AlAs layer was fully converted $Al_2O_3$. The I-V, $g_m$, breakdown charateristics of the fabricated GaAs MOSFET showed that wet thermal oxidation of AlAs/GaAs epilayer/S${\cdot}$I GaAs was suitable in realizing depletion mode GaAs MOSFET.

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InAlAs/AlGaAs을 이용한 808 nm 대역 양자점 성장

  • Kim, Su-Yeon;Song, Jin-Dong;Lee, Eun-Hye;Han, Il-Gi;Lee, Jeong-Il;Kim, Tae-Hwan
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.02a
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    • pp.166-166
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    • 2010
  • 산업 전반에 걸쳐 중요한 광원인 808 nm 대역의 레이저 다이오드 제작에는 현재 InGaAsP/InGaP/GaAs 및 InGaAlAs/GaAs 양자우물을 이용하여 제작되고 있다. 이는 양자우물과 이를 둘러싸는 장벽물질간의 band-offset이 적어 효율적인 고출력 레이저 다이오드의 제작에 어려움이 있기 때문에 강한 캐리어 구속 효과를 지니는 양자점을 사용하는 것이 고출력 레이저 다이오드를 제작할 수 있는 방법이다. 실험에 사용된 InAlAs 양자점은 Riber사의 compact21 MBE 장치를 사용하여 성장하였으며 GaAs기판을 610도에서 가열하여 표면의 산화층을 제거하고 580도에서 약 100 nm 두께의 GaAs 버퍼층 및 30 nm 두께의 $Al_{0.4}Ga_{0.6}As$층을 성장하였다. GaAs 기판의 온도를 내린 후 migration enhanced epitaxy 방법을 사용하여 InAs 및 AlAs를 번갈아 주입하여 성장하였다. InAlAs 양자점의 성장 중에 InAlAs의 양, 성장 온도, As flux량 및 As 분자 상태 변화 등 다양한 조건을 변화 시켜 샘플을 성장시켰다. 그 결과 기판 온도가 600도이며 As4 flux가 $1\;{\times}\;10^{-6}\;Torr$ 조건하에서 성장한 InAlAs/AlGaAs 양자점이 양질의 808 nm의 파장 대역을 얻을 수 있었다.

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Impact Ionization Rates of Electron in GaAs/AlGaAs Qunantum Well Using EMC Simulation (EMC Simulation을 이용한 GaAs/AlGaAs 양자 우물 내 전자의 충돌 이온화율)

  • 윤기정;홍창희
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1994.11a
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    • pp.221-225
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    • 1994
  • We described the impact ionization rates of electron in GaAs/AlGaAs MQH(multi- quantum well) using EMC(ensenble Monte Carlo) simulation. Hot electron energy of injected into quantum well is increasing nearly liearly due to the applied electric field to the barrier of MQM inspite of various Al mole fraction in AlGaAs or barrier width. Impact ionization rates are decreasing exponentially by increasing Al mole fraction, and they have peak vague due to the barrier width.

Surface Photovoltage Characteristics of ${In_{0.5}}({Ga_{1-x}}{Al_x})_{0.5}P$/GaAs Double Heterostructures (${In_{0.5}}({Ga_{1-x}}{Al_x})_{0.5}P$/GaAs 이중 이종접합 구조에 대한 표면 광전압 특성)

  • Kim, Ki-Hong;Choi, Sang-Soo;Bae, In-Ho;Kim, I n-Soo;Park, Sung-Bae
    • Korean Journal of Materials Research
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    • v.11 no.8
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    • pp.655-660
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    • 2001
  • Surface photovoltage spectroscopy was used to study $In_{0.5}(Ga_{1-x}Al_x)_{0.5}P/GaAs$ grown by metalorganic chemical vapor deposition(MOCVD). Energy gap related transition in GaAs and $In_{0.5}(Ga_{1-x}Al_x)_{0.5}P$ were observed. By measuring the frequency dependence of $In_{0.5}(Ga_{1-x}Al_x)_{0.5}P/GaAs$, we observed that SPV line shape does not chance, whereas the amplitude change. This results is due to the difference in the lifetimes of the photocarriers in GaAs and in $In_{0.5}(Ga_{1-x}Al_x)_{0.5}P$. We also have evaluated the parameters that describe the temperature dependences of the band gap.

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Temperature-dependent Luminescence Properties of Digital-alloy In(Ga1-zAlz)As

  • Cho, Il-Wook;Ryu, Mee-Yi;Song, Jin Dong
    • Applied Science and Convergence Technology
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    • v.27 no.3
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    • pp.56-60
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    • 2018
  • The optical properties of the digital-alloy $(In_{0.53}Ga_{0.47}As)_{1-z}/(In_{0.52}Al_{0.48}As)_z$ grown by molecular beam epitaxy as a function of composition z (z = 0.4, 0.6, and 0.8) have been studied using temperature-dependent photoluminescence (PL) and time-resolved PL (TRPL) spectroscopy. As the composition z increases from 0.4 to 0.8, the PL peak energy of the digital-alloy $In(Ga_{1-z}Al_z)As$ is blueshifted, which is explained by the enhanced quantization energy due to the reduced well width. The decrease in the PL intensity and the broaden FWHM with increasing z are interpreted as being due to the increased Al contents in the digital-alloy $In(Ga_{1-z}Al_z)As$ because of the intermixing of Ga and Al in interface of InGaAs well and InAlAs barrier. The PL decay time at 10 K decreases with increasing z, which can be explained by the easier carrier escape from InGaAs wells due to the enhanced quantized energies because of the decreased InGaAs well width as z increases. The emission energy and luminescence properties of the digitalalloy $(InGaAs)_{1-z}/(InAlAs)_z$ can be controlled by adjusting composition z.

Comparison of Quantum Wells based on InGaAs(P)/InP and InGa(Al)As/InAlAs Material Systems in View of Carrier Escape Times for High-Saturation-Optical-Power Electroabsorption Modulators

  • Kim, Kang-Baek;Shin, Dong-Soo
    • Journal of the Optical Society of Korea
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    • v.11 no.3
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    • pp.133-137
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    • 2007
  • We compare electroabsorption modulators (EAMs) with multiple quantum wells (MQWs) based on InGaAs(P)/InP and InGa(Al)As/InAlAs material systems. We carefully choose the quantum-well structures so that the structures based on different material systems have similar band-offset energies and excition-peak wavelengths. Assuming the same light wavelength of $1.55{\mu}m$, we show the transfer functions of EAMs with each quantum-well structure and calculate the escape times of photogenerated charge carriers. As the heavy-hole escape time of the quantum well based on InGaAs(P)/InP is much longer than those of photogenerated charge carriers of InGa(Al)As/InAlAs, the EAM based on the InGa(Al)As/InAlAs material seems to be more suitable for high-optical-power operation.

A study on surface photovoltage of $Al_{0.24}Ga_{0.76}As/GaAs$ epilayer ($Al_{0.24}Ga_{0.76}As/GaAs$ 에피층에서의 표면 광전압에 관한 연구)

  • 유재인;김도균;김근형;배인호;김인수;한병국
    • Journal of the Korean Vacuum Society
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    • v.9 no.2
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    • pp.116-121
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    • 2000
  • We measured surface photovoltage (SPV) of $Al_{0.24}Ga_{0.76}As/GaAs$ epilayer grown by molecular beam epitixy (MBE). The band gap energies of $Al_{0.24}Ga_{0.76}As/GaAs$ epilayer, GaAs substrate and buffer layer obtained from SPV signals are 1.70, 1.40 and 1.42 eV, respectively. There results are in good agreements with photoreflectance (PR) measurement. The measured SPV intensity of GaAs substrate is three times larger than $Al_{0.24}Ga_{0.76}$Asepilayer by carrier mobility difference. The parameters of Varshni equation were determined from the SPV spectra as a function of temperature.

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