• 제목/요약/키워드: $In_xGa_{1-x}N$

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0.25 μm AlGaN/GaN HEMT 소자 및 9 GHz 대역 전력증폭기 (0.25 μm AlGaN/GaN HEMT Devices and 9 GHz Power Amplifier)

  • 강동민;민병규;이종민;윤형섭;김성일;안호균;김동영;김해천;임종원;남은수
    • 한국전자파학회논문지
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    • 제27권1호
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    • pp.76-79
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    • 2016
  • 본 논문에서는 ETRI에서 개발된 50 W GaN-on-SiC HEMT 소자를 이용하여 X-band에서 동작하는 50 W 펄스 전력증폭기의 개발 결과를 정리하였다. 제작된 50 W GaN HEMT 소자는 $0.25{\mu}m$의 게이트 길이를 갖고, 총 게이트 폭은 12 mm인 소자이다. 펄스 전력증폭기는 9.2~9.5 GHz 주파수 대역에서 50 W의 출력전력과 6 dB의 전력이득 특성을 나타내었다. 전력소자의 전력밀도는 4.16 W/mm이다. 제작된 GaN-on-SiC HEMT 소자와 전력증폭기는 X-대역 레이더 시스템 등 다양한 응용분야에 적용이 가능할 것으로 판단된다.

Structural studies of $Mn^+$ implanted GaN film

  • Shi, Y.;Lin, L.;Jiang, C.Z.;Fan, X.J.
    • 한국진공학회지
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    • 제12권S1호
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    • pp.56-59
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    • 2003
  • Wurtzite GaN films are grown by low-pressure MOCVD on (0001)-plane sapphire substrates. The GaN films have a total thickness of 4 $\mu$m with a surface Mg-doped p-type layer, which has a thickness of 0.5 $\mu$m. 90k eV $Mn^{+}$ ions are implanted into the GaN films at room temperature with doses ranging from $1 \times10^{15}$ to $1 \times 10^{16}\textrm{cm}^{-2}$. After an annealing step at $770^{\circ}C$ in flowing $N_2$, the structural characteristics of the $Mn^{+}$ implanted GaN films are studied by X-ray diffraction (XRD), Rutherford backscattering spectrometry (RBS) and atomic force microscopy (AFM). The structural and morphological changes brought about by $Mn^{+}$ implantation and annealing are characterized.

TGS법으로 성장한 $In_{l-x}Ga_{x}As$의 특성에 관한 연구 (A study on the Properties of $In_{l-x}Ga_{x}As$ Grown by the TGS Methods)

  • 이원상;문동찬;김선태;서영석
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1988년도 추계학술대회 논문집 학회본부
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    • pp.372-375
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    • 1988
  • The III-V ternary alloy semiconductor $In_{l-x}Ga_{x}As$ were grown by the temperature Gradient of $0.60{\leq}x{\leq}0.98$. The electrical properties were investigated by the Hall effect measurement with the Van der Pauw method in the temperature range of $90{\sim}300K$. $In_{l-x}Ga_{x}As$ were revealed n-type and the carrier concentration at 300K were in the range of $9.69{\times}10^{16}cm^{-3}{\sim}7.49{\times}10^{17}cm^{-3}$. The resistivity was increased and the carrier mobility was decreased with increasing the composition ratio. The optical energy gap determined by optical transmission were $20{\sim}30meV$ lower than theoretical valves on the basis of absorption in the conduction band tail and it was decreased with increasing the temperature by the Varshni rule. In the photoluminescence of undoped $In_{l-x}Ga_{x}As$ at 20K, the main emission was revealed by the radiative recombination of shallow donor(Si) to acceptor(Zn) and the peak energy was increased with increasing the composition, X. The diffusion depth of Zn increases proportionally with the square root of diffusion time, and the activation energy for the Zn diffusion into $In_{0.10}Ga_{0.90}As$ was 2.174eV and temperatures dependence of diffusion coefficient was D = 87.29 exp(-2.174/$K_{B}T$). The Zn diffusion p-n $In_{x}Ga_{x}As$ diode revealed the good rectfying characteristics and the diode factor $\beta{\approx}2$. The electroluminescence spectrum for the Zn-diffusion p-n $In_{0.10}Ga_{0.90}As$ diode was due to radiative recombation between the selectron trap level(${\sim}140meV$) and Zn acceptor level(${\sim}30meV$). The peak energy and FWHM of electroluminescence spectrum at 77K were 1.262eV and 81.0meV, respectively.

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Preparation of Gallium Nitride Powders and Nanowires from a Gallium(III) Nitrate Salt in Flowing Ammonia

  • Jung, Woo-Sik
    • Bulletin of the Korean Chemical Society
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    • 제25권1호
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    • pp.51-54
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    • 2004
  • Gallium nitride (GaN) powders were prepared by calcining a gallium(III) nitrate salt in flowing ammonia in the temperature ranging from 500 to 1050 $^{\circ}C$. The process of conversion of the salt to GaN was monitored by X-ray diffraction and $^{71}Ga$ MAS (magic-angle spinning) NMR spectroscopy. The salt decomposed to ${\gamma}-Ga_2O_3$ and then converted to GaN without ${\gamma}-{\beta}Ga_2O_3$ phase transition. It is most likely that the conversion of ${\gamma}-Ga_2O_3$ to GaN does not proceed through $Ga_2O$ but stepwise via amorphous gallium oxynitride ($GaO_xN_y$) as intermediates. The GaN nanowires and microcrystals were obtained by calcining the pellet containing a mixture of ${\gamma}-Ga_2O_3$ and carbon in flowing ammonia at 900 $^{\circ}C$ for 15 h. The growth of the nanowire might be explained by the vapor-solid (VS) mechanism in a confined reactor. Room-temperature photoluminescence spectra of as-synthesized GaN powders obtained showed the emission peak at 363 nm.

InxGa1-xAs 화합물 반도체의 Indium 조성에 따른 Nanowire Field-Effect Transistor 특성 연구

  • 이현구;서준범
    • EDISON SW 활용 경진대회 논문집
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    • 제6회(2017년)
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    • pp.428-432
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    • 2017
  • Silicon 기반 Metal-oxide-semiconductor field-effect transistor (MOSFET)의 크기가 감소함에 따라 silicon자체의 물성적 한계가 나타나고 있다. 이를 극복하고자 III-V 화합물 반도체가 채널소자로서 각광받고 있다. 본 연구에서는 III-V 화합물반도체 중 $In_xGa_{1-x}As$는 Indium 조성에 따른 전자구조 및 n-type MOSFET의 소자 특성을 본다. Indium의 조성이 증가함에 따라 subband의 개수와 간격이 증가하게 되어 Density of state가 감소하게 된다. 이로 인하여 Indium의 조성이 증가함에 따라 $In_xGa_{1-x}As$ 채널 MOSFET에서 상대적으로 Fermi level을 더 많이 상승시키게 되어 potential barrier를 얇아지게 만들며 또한 에너지에 따른 전류 밀도를 넓게 분포하도록 만든다. 이로 인하여 단채널에서는 In 조성이 증가함에 따라 direct source-to-drain tunnelling current이 증가하게 된다. 이로 인하여 In 조성의 증가에 따라 subthreshold swing과 ON-state current가 저하된다.

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DLTS 방법에 의한 GaAs/$\textrm{Al}_{x}\textrm{Ga}_{1-x}\textrm{As}$/GaAs 이종구조의 물성분석에 관한 연구 (Physical Characterization of GaAs/$\textrm{Al}_{x}\textrm{Ga}_{1-x}\textrm{As}$/GaAs Heterostructures by Deep Level transient Spectroscopy)

  • 이원섭;최광수
    • 한국재료학회지
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    • 제9권5호
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    • pp.460-466
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    • 1999
  • The deep level electron traps in AP-MOCVD GaAs/undoped Al\ulcornerGa\ulcornerAs/n-type GaAs heterostructures have been investigated by means of Deep Level Transient Spectroscopy DLTS). In terms of the experimental procedure, GaAs/undoped Al\ulcornerGa\ulcornerAs/n-type GaAs heterostructures were deposited on 2" undoped semi-insulating GaAs wafers by the AP-MOCVD method at $650^{\circ}C$ with TMGa, AsH3, TMAl, and SiH4 gases. The n-type GaAs conduction layers were doped with Si to the target concentration of about 2$\times$10\ulcornercm\ulcorner. The Al content was targeted to x=0.5 and the thicknesses of Al\ulcornerGa\ulcornerAs layers were targeted from 0 to 40 nm. In order to investigate the electrical characteristics, an array of Schottky diodes was built on the heterostructures by the lift-off process and Al thermal evaporation. Among the key results of this experiment, the deep level electron traps at 0.742~0.777 eV and 0.359~0.680 eV were observed in the heterostructures; however, only a 0.787 eV level was detected in n-type GaAs samples without the Al\ulcornerGa\ulcornerAs overlayer. It may be concluded that the 0.787 eV level is an EL2 level and that the 0.742~0.777 eV levels are related to EL2 and residual oxygen impurities which are usually found in MOCVD GaAs and Al\ulcornerGa\ulcornerAs materials grown at $630~660^{\circ}C$. The 0.359~0.680 eV levels may be due to the defects related with the al-O complex and residual Si impurities which are also usually known to exist in the MOCVD materials. Particularly, as the Si doping concentration in the n-type GaAs layer increased, the electron trap concentrations in the heterostructure materials and the magnitude of the C-V hysteresis in the Schottky diodes also increased, indicating that all are intimately related.ated.

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Single-phase Gallium Nitride on Sapphire with buffering AlN layer by Laser-induced CVD

  • Hwang Jin-Soo;Lee Sun-Sook;Chong Paul-Joe
    • Bulletin of the Korean Chemical Society
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    • 제15권1호
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    • pp.28-33
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    • 1994
  • The laser-assisted chemical vapor deposition (LCVD) is described, by which the growth of single-phase GaN epitaxy is achieved at lower temperatures. Trimethylgallium (TMG) and ammonia are used as source gases to deposit the epitaxial films of GaN under the irradiation of ArF excimer laser (193 nm). The as-grown deposits are obtained on c-face sapphire surface near 700$^{\circ}$C, which is substantially reduced, relative to the temperatures in conventional thermolytic processes. To overcome the lattice mismatch between c-face sapphire and GaN ad-layer, aluminum nitride(AlN) is predeposited as buffer layer prior to the deposition of GaN. The gas phase interaction is monitored by means of quadrupole mass analyzer (QMA). The stoichiometric deposition is ascertained by X-ray photoelectron spectroscopy (XPS). The GaN deposits thus obtained are characterized by X-ray diffractometer (XRD), scanning electron microscopy (SEM) and van der Pauw method.

GaN-HEMT를 이용한 X-대역 이단 전력증폭기 설계 (Design of Two-Stage X-Band Power Amplifier Using GaN-HEMT)

  • 이우석;이휘섭;박승국;임원섭;한재경;박광근;양영구
    • 한국전자파학회논문지
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    • 제27권1호
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    • pp.20-26
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    • 2016
  • 본 논문에서는 GaN-HEMT를 이용하여 X-대역에서 동작하는 이단으로 구성된 전력증폭기를 설계 및 제작하였다. 높은 전력 이득을 얻기 위해 간단한 구조의 중간 단 정합 네트워크를 통해 이단으로 구성하였다. 3D EM 시뮬레이션을 통하여 본드와이어 인덕턴스와 기생 캐패시턴스를 예측하였다. 본드와이어 인덕턴스를 줄임으로써 정합 네트워크의 Q(quality-factor)를 최소화하여 대역 특성을 향상시켰다. 제작된 전력증폭기는 40 V의 동작 전압을 인가하였으며, 8.1~8.5 GHz에서 16 dB 이상의 전력 이득, 42.5 dBm 이상의 출력 전력, 35 % 이상의 효율 특성을 나타냈다.

X-대역 펄스압축 Solid State Radar를 위한 200W SSPA 개발 (Implementation of the 200-Watts SSPA for X-band Pulse Compression Solid State Radar)

  • 김민수;이춘성;이상록;이영철
    • 대한전자공학회논문지TC
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    • 제46권12호
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    • pp.22-29
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    • 2009
  • 본 논문에서는 X-대역 펄스압축 반도체형 레이다를 위한 200W SSPA를 개발하였다. 개발한 X-대역 SSPA는 전치증폭단, 구동증폭단, 고출력을 위한 주전력 증폭단의 3단 연계구조형 증폭기로 구성되어있다. X-대역에서 200W 이상의 출력을 내기 위해 주전력 증폭단은 충분한 이득과 전력을 얻을 수 있는 GaN HEMT소자를 사용하여 병렬구조로 설계하였다. 개발한 SSPA는 주파수범위 9.2-9.6GHz, 펄스주기 1ms, 펄스폭 100us, 듀티사이클 10% 조건에서 전체이득 59dB 이상, 출력전력 200W이상의 성능을 가진다. 본 논문에서 개발한 SSPA는 펄스압축기술을 이용한 고품위 반도체 레이다시스템에 적용할 수 있다.

HVPE법으로 성장시킨 GaN substrate 제작과 특성 평가 (Fabrication and characterization of GaN substrate by HVPE)

  • 오동근;최봉근;방신영;은종원;정준호;이성국;정진현;심광보
    • 한국결정성장학회지
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    • 제20권4호
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    • pp.164-167
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    • 2010
  • 본 연구에서는 HVPE을 이용하여 sapphire(001) 기판 위에 직경 2 inch, 두께 약 1.5 mm인 bulk GaN를 성장하고, 이를 mechanical polishing을 통해 $10{\times}10,\;15{\times}15$ mm 크기의 free-standing GaN template을 제작하여 그 특성을 평가하였다. 성장된 GaN 단결정의 X-ray diffraction pattern 결과 (002) 및 (004) 면으로부터의 회절에 의한 peak가 나타났으며, (002) 면의 DCXRD(Double crystal X-Ray diffraction) rocking curve peak의 반치폭(FWHM)은 98 arcsec으로 나타났다. 제작한 GaN template는 363 nm 파장에서 sharp한 PL spectrum을 나타내었으며, 불순물 defect에 의한 yellow 영역에서의 broad peak은 관찰되지 않았으며, 제작된 GaN template표면의 etch-pit 밀도는 $5{\times}10^6/cm^2$으로 매우 낮았다. 이러한 분석결과를 통하여 성장된 GaN template는 LED 및 LD 등의 청색 발광소자 및 고온, 고출력 소자용 기판재료로 응용이 가능할 것으로 생각 된다.