• Title/Summary/Keyword: N-passivation

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Simulation Study on the Breakdown Enhancement for InAlAs/InGaAs/GaAs MHEMTs with an InP-Etchstop Layer (InP 식각정지층을 갖는 InAlAs/InGaAs/GaAs MHEMT 소자의 항복 전압 개선에 관한 연구)

  • Son, Myung Sik
    • Journal of the Semiconductor & Display Technology
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    • v.12 no.3
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    • pp.23-27
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    • 2013
  • This paper is for enhancing the breakdown voltage of MHEMTs with an InP-etchstop layer. Gate-recess structures has been simulated and analyzed for the breakdown of the devices with the InP-etchstop layer. The fully removed recess structure in the drain side of MHEMT shows that the breakdown voltage enhances from 2V to almost 4V and that the saturation current at gate voltage of 0V is reduced from 90mA to 60mA at drain voltage of 2V. This is because the electron-captured negatively fixed charges at the drain-side interface between the InAlAs barrier layer and the $Si_3N_4$ passivation layer deplete the InGaAs channel layer more and thus decreases the electron current passing the channel layer. In the paper, the fully-recessed asymmetric gate-recess structure at the drain side shows the on-breakdown voltage enhancement from 2V to 4V in the MHEMTs.

A Production and Analysis on High Quality of Thin Film Transistors Using NH3 Plasma Treatment (NH3 Plasma Treatment를 사용한 고성능 TFT 제작 및 분석)

  • Park, Heejun;Nguyen, Van Duy;Yi, Junsin
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.30 no.8
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    • pp.479-483
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    • 2017
  • The effect of $NH_3$ plasma treatment on device characteristics was confirmed for an optimized thin film transistor of poly-Si formed by ELA. When C-V curve was checked for MIS (metal-insulator-silicon), Dit of $NH_3$ plasma treated and MIS was $2.7{\times}10^{10}cm^{-2}eV^{-1}$. Also in the TFT device case, it was decreased to the sub-threshold slope of 0.5 V/decade, 1.9 V of threshold voltage and improved in $26cm^2V^{-1}S^{-1}$ of mobility. Si-N and Si-H bonding reduced dangling bonding to each interface. When gate bias stress was applied, the threshold voltage's shift value of $NH_3$ plasma treated device was 0.58 V for 1,000s, 1.14 V for 3,600s, 1.12 V for 7,200s. As we observe from this quality, electrical stability was also improved and $NH_3$ plasma treatment was considered effective for passivation.

The passivation of III-V compound semiconductor surface by laser CVD (Laser CVD법에 의한 III-V화합물 반도체 표면의 불활성화)

  • Lee, H.S.;Lee, K.S.;Cho, T.H.;Huh, Y.J.;Kim, S.J.;Sung, Y.K.
    • Proceedings of the KIEE Conference
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    • 1993.07b
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    • pp.1274-1276
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    • 1993
  • The silicon-nitride films formed by laser CVD method are used for passivating GaAs surfaces. The electrical Properties of metal-insulator-GaAs structure are studied to determined the interfacial characteristics by C-V curves and deep level transient spectroscopy(DLTS). The SiN films are photolysisly deposited from $SiH_4\;and\;NH_3$ in the range of $100^{\circ}C-300^{\circ}C$ on P type, (100) GaAs. The hysteresis is reduced and interface trap density is lowered to $10^{12}-10^{13}$ at $100^{\circ}C-200^{\circ}C$. The surface leakage current is studied too. The passivated GaAs have a little leakage current compared to non passivated GaAs.

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PECVD를 이용한 SiNx 증착 조건에 따른 수소 패시베이션 개선 효과

  • Jo, Guk-Hyeon;Jang, Hyo-Sik
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.08a
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    • pp.200.1-200.1
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    • 2013
  • 실리콘 태양전지 표면에는 구조적인 결함에 의해 소수 캐리어의 재결합이 일어난다. 재결합에 의해 캐리어의 반송자 수명은 줄어들게 되고, 태양전지의 효율은 감소하게 된다. 이를 줄이기 위해 태양전지 전 후면에 패시베이션을 하게 되는데, 이번 연구는 단결정 실리콘 태양전지 전면에 SiNx막을 증착함으로 수소 패시베이션이 반송자 수명에 미치는 영향에 대하여 연구하였다. 공정을 위해 $156{\times}156mm^2$, 200 ${\mu}m$, 0.5-3.0 ${\Omega}{\cdot}cm$ and p-type 단결정 실리콘 웨이퍼를 사용하였고, SiNx막을 올리기 전에 KOH 8.5% 용액으로 SDR을 실행하였다. RF-PECVD 장비로 SiNx 막을 증착하였고 증착 온도는 $200{\sim}400^{\circ}C$, 반응기 내부의 압력을 200~1,000 mtorr, SiH4/NH3/N2 각각의 가스 비율 조절, 그리고 플라즈마 RF power 변화시킴에 따라 증착된 SiNx막의 균일도 및 특성을 분석하였다. 반사광 측정 장비인 Reflectometer장비로 막의 두께와 굴절률, 반사율을 측정하였고, 반송자 수명을 측정하여 태양전지의 표면결함을 최대한 패시베이션 시켜주는 조건에 대한 연구를 수행하였다.

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One-pot synthesis of highly fluorescent amino-functionalized graphene quantum dots for effective detection of copper ions

  • Tam, Tran Van;Choi, Won Mook
    • Current Applied Physics
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    • v.18 no.11
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    • pp.1255-1260
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    • 2018
  • In this work, a green and simple one-pot route was developed for the synthesis of highly fluorescent aminofunctionalized graphene quantum dots (a-GQDs) via hydrothermal process without any further modification or surface passivation. We synthesized the a-GQDs using glucose as the carbon source and ammonium as a functionalizing agent without the use of a strong acid, oxidant, or other toxic chemical reagent. The as-obtained aGQDs have a uniform size of 3-4 nm, high contents of amino groups, and show a bright green emission with high quantum yield of 32.8%. Furthermore, the a-GQDs show effective fluorescence quenching for $Cu^{2+}$ ions which can serve as effective fluorescent probe for the detection of $Cu^{2+}$. The fluorescent probe using the obtained aGQDs exhibits high sensitivity and selectivity toward $Cu^{2+}$ with the limit of detection as low as 5.6 nM. The mechanism of the $Cu^{2+}$ induced fluorescence quenching of a-GQDs can be attributed to the electron transfer by the formation of metal complex between $Cu^{2+}$ and the amino groups on the surface of a-GQDs. These results suggest great potential for the simple and green synthesis of functionalized GQDs and a practical sensing platform for $Cu^{2+}$ detection in environmental and biological applications.

Selective Emitter Formation of Borosilicate-Glass (BSG) Layer using UV Laser (UV Laser를 이용한 Borosilicate-Glass (BSG)층의 선택적 에미터 형성)

  • Kim, Ga Min;Chang, Hyo Sik
    • Korean Journal of Materials Research
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    • v.31 no.12
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    • pp.727-731
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    • 2021
  • In this study, we have investigated a selective emitter using a UV laser on BBr3 diffusion doping layer. The selective emitter has two regions of high and low doping concentration alternatively and this structure can remove the disadvantages of homogeneous emitter doping. The selective emitters were fabricated by using UV laser of 355 nm on the homogeneous emitters which were formed on n-type Si by BBr3 diffusion in the furnace and the heavy boron doping regions were formed on the laser regions. In the optimized laser doping process, we are able to achieve a highly concentrated emitter with a surface resistance of up to 43 Ω/□ from 105 ± 6 Ω/□ borosilicate glass (BSG) layer on Si. In order to compare the characteristics and confirm the passivation effect, the annealing is performed after Al2O3 deposition using an ALD. After the annealing, the selective emitter shows a better effect than the high concentration doped emitter and a level equivalent to that of the low concentration doped emitter.

Effects of pH and Chloride Concentration on Corrosion Behavior of Duplex Stainless Steel and Titanium Alloys Ti 6Al 2Nb 1Ta 1Mo at Elevated Temperature for Pump Impeller Applications

  • Aymen A., Ahmed;Ammar Yaseen, Burjes;Ammar Yaseen, Burjes
    • Corrosion Science and Technology
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    • v.21 no.6
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    • pp.454-465
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    • 2022
  • The objective of this study was to determine effects of temperatures and pH of sodium chloride solution with MgCl2 ions on corrosion resistance of duplex stainless-steel X2CrNiMoN22-5-3 (DSS) and Ti 6Al 2Nb1Ta1Mo (Ti). Effects of sodium chloride concentration on corrosion resistance were also studied. Corrosion behavior and pitting morphology of duplex stainless steel (DSS) and Ti alloys were evaluated through potentiodynamic polarization, electrochemical impedance spectroscopy (EIS), and scanning electron microscopy (SEM). It was found that a decrease in pH significantly reduced the corrosion resistance of both alloys. Changes in chloride concentration and temperature had more substantial impact on corrosion behavior of DSS than on Ti alloys. Pitting corrosion was formed on DSS samples under all conditions, whereas crevice corrosion was developed on Ti samples with the presence of magnesium chloride at 90 ℃. In conclusion, magnesium chloride ions in an exceedingly strong acidity solution appear to interact with re-passivation process at the surface of these alloys and influence the resulting surface topography.

The Study of $SiO_2$, $Si_3N_4$ passivation layers grown by PECVD for the indiumantimonide photodetector

  • Lee, Jae-Yeol;Kim, Jeong-Seop;Yang, Chang-Jae;Park, Se-Hun;Yun, Ui-Jun
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2009.11a
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    • pp.24.2-24.2
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    • 2009
  • Indium Antimonide(InSb)는 $3{\sim}5\;{\mu}m$대 적외선 감지영역에서 기존 HgCdTe(MCT)를 대체할 물질로 각광받고 있다. 1970년대부터군사적 용도로 미국, 이스라엘 등 일부 선진국에서 연구되기 시작했으며,이온주입, MOCVD, MBE 등 다양한 공정을 통해 제작되어 왔다. InSb 적외선 감지소자는 $3{\sim}5{\mu}m$대에서 HgCdTe와 성능은 대등한데 반해, 기판의 대면적화와 저렴한 가격, 우주공간 및 야전에서 소자 동작의안정성 등으로 InSb적외선 감지기는 냉각형 고성능 적외선 감지영역에서 HgCdTe를 대체해 가고 있다. 하지만 InSb는 77 K에서 0.225eV의 작은 밴드갭을 갖고 있기 때문에 누설전류로 인한 성능저하가 고질적인문제로 대두되었고, 이를 해결하기 위한 고품질 절연막 연구가 InSb적외선 수광 소자 연구의 주요이슈 중 하나가 되어왔다. 그 동안 PECVD, photo-CVD, anodic oxidation 등의 공정을 이용하여 $SiO_2$, $Si_3N_4$, 양극산화막(anodic oxide) 등 다양한 절연막에 대한 연구가 진행되었고[1,2], 절연막과 반도체 사이 계면에서의 열확산을 억제하여 계면트랩밀도를 최소화하기 위한 공정개발이 이루어졌다[3]. 하지만 InSb 적외선 감지기술은 국방 및 우주개발의 핵심기술중 하나로 그 기술의 이전이 엄격히 통제되고 있으며, 현재도 미국과 이스라엘, 일본, 영국 등 일부 선진국 만이 기술을 확보하고 있고, 국내의 경우 연구가 매우 취약한 실정이다. 따라서 본 연구에서는 InSb 적외선 감지기의 암전류를 제어하기 위한 낮은 계면트랩밀도를 갖는 절연막 증착 공정을 찾고자 하였다. 본 연구에서는 n형 (100) InSb 기판 ($n=0.2{\sim}0.85{\times}10^{15}cm^{-3}$ @ 77K)에 PECVD를 이용하여 $SiO_2$, $Si_3N_4$ 등을 증착하고 절연막으로서 이들의 특성을 비교 분석하였다. $SiO_2$는 160, 200, $240^{\circ}C$에서 $Si_3N_4$는 200, $300^{\circ}C$에서 증착하였다. Atomic Force Microscopy(AFM) 사진으로 확인한 결과, 모든 샘플에서표면거칠기가 ~2 nm의 평탄한 박막을 얻을 수 있었다. Capacitance-Voltage 측정(77K)을 통해 절연막 특성을 평가하였다. $SiO_2$$Si_3N_4$ 모두에서 온도가 증가할수록 벌크트랩밀도가 감소하는 경향을 볼 수 있었는데, 이는 고온에서 증착할 수록 박막 내의 결함이 감소했음을 의미한다. 반면계면트랩밀도는 온도가 증가함에 따라, 1011 eV-1cm-2 대에서 $10^{12}eV^{-1}cm^{-2}$ 대로 증가하였는데, 이는 고온에서 증착할 수 록 InSb 표면에서의 결함은 증가하였음을의미한다. 암전류에 큰 영향을 주는 것은 계면트랩밀도 이므로, $SiO_2$$Si_3N_4$ 모두 $200^{\circ}C$이하의 저온에서 증착시켜야 함을 확인할 수 있었다.

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Simulation Design of MHEMT Power Devices with High Breakdown Voltages (고항복전압 MHEMT 전력소자 설계)

  • Son, Myung-Sik
    • Journal of the Korean Vacuum Society
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    • v.22 no.6
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    • pp.335-340
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    • 2013
  • This paper is for the simulation design to enhance the breakdown voltage of MHEMTs with an InP-etchstop layer. Gate-recess and channel structures has been simulated and analyzed for the breakdown of the MHEMT devices. The fully removed recess structure at the drain side of MHEMT shows that the breakdown voltage enhances from 2 V to almost 4 V as the saturation current at gate voltage of 0 V is reduced from 90 mA to 60 mA at drain voltage of 2 V. This is because the electron-captured negatively fixed charges at the drain-side interface between the InAlAs barrier and the $Si_3N_4$ passivation layers deplete the InGaAs channel layer more and thus decreases the electron current passing the channel layer and thus the impact ionization in the channel become smaller. In addition, the replaced InGaAs/InP composite channel with the same thickness in the same asymmetrically recessed structure increases the breakdown voltage to 5 V due to the smaller impact ionization and mobility of the InP layer at high drain voltage.

Properties of Silicon Nitride Deposited by RF-PECVD for C-Si solar cell (결정질 실리콘 태양전지를 위한 실리콘 질화막의 특성)

  • Park, Je-Jun;Kim, Jin-Kuk;Song, Hee-Eun;Kang, Min-Gu;Kang, Gi-Hwan;Lee, Hi-Deok
    • Journal of the Korean Solar Energy Society
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    • v.33 no.2
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    • pp.11-17
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    • 2013
  • Silicon nitride($SiN_x:H$) deposited by radio frequency plasma enhanced chemical vapor deposition(RF-PECVD) is commonly used for anti-reflection coating and passivation in crystalline silicon solar cell fabrication. In this paper, characteristics of the deposited silicon nitride was studied with change of working pressure, deposition temperature, gas ratio of $NH_3$ and $SiH_4$, and RF power during deposition. The deposition rate, refractive index and effective lifetime were analyzed. The (100) p-type silicon wafers with one-side polished, $660-690{\mu}m$, and resistivity $1-10{\Omega}{\cdot}cm$ were used. As a result, when the working pressure increased, the deposition rate of SiNx was increased while the effective life time for the $SiN_x$-deposited wafer was decreased. The result regarding deposition temperature, gas ratio and RF power changes would be explained in detail below. In this paper, the optimized condition in silicon nitride deposition for silicon solar cell was obtained as 1.0 Torr for the working pressure, $400^{\circ}C$ for deposition temperature, 500 W for RF power and 0.88 for $NH_3/SiH_4$ gas ratio. The silicon nitride layer deposited in this condition showed the effective life time of > $1400{\mu}s$ and the surface recombination rate of 25 cm/s. The crystalline silicon solar cell fabricated with this SiNx coating showed 18.1% conversion efficiency.