• 제목/요약/키워드: Semiconductor devices

검색결과 1,723건 처리시간 0.03초

습식 에칭 공정에서의 과산화수소 이상반응에 대한 안전 대책 및 제어에 관한 연구 (A study on Safety Management and Control in Wet-Etching Process for H2O2 Reactions)

  • 유흥렬;손영득
    • 한국산학기술학회논문지
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    • 제19권4호
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    • pp.650-656
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    • 2018
  • TFT-LCD 산업은 반도체와 유사한 공정기술을 갖는 대규모 장치 산업으로 일종의 Giant Microelectronics 산업이다. 습식 에칭(Wet Etching)은 전체 TFT 공정에서 비교적 큰 비중을 차지하고 있지만 발표된 연구사례는 부족한 실정이다. 그 주요 원인은 반응이 일어나는 에칭액(Etchant) 성분이 기업의 비밀로 간주되어 외부에 발표되는 사례가 거의 없기 때문이다. 최근 대면적 LCD 제조를 위하여 사용되는 알루미늄(Al)과 구리(Cu)는 습식 에칭을 진행하기에 매우 까다로운 물질이다. 저 저항성 재료인 Cu는 습식 에칭 공정에서만 가능하며 높은 속도와 낮은 실패율, 적은 소비전력으로 Al 에칭 대용으로 사용하고 있다. 그리고 에칭액으로 사용하는 과산화수소($H_2O_2$)의 이상 반응으로 추가적인 배관 및 전기적인 안전장치가 필요하다. 본 논문에서는 과산화수소의 이상 반응을 제한하지는 못하나 이상 반응 발생 시 설비의 피해를 최소화 할 수 있는 방법을 제안한다. 또한 최근에 알루미늄 에칭설비에서 구리 에칭설비로 변경하는 사례가 많아 구리 에칭설비에 대한 하드웨어 인터록을 제안하고 안전 등급이 높은 안전 PLC로 구현하여 이상 반응에 대한 대비책을 강구하는 방안을 제안한다.

공정변화에 따른 LDO 레귤레이터의 특성 분석 (Characteristic Analysis of LDO Regulator According to Process Variation)

  • 박원경;김지만;허윤석;박용수;송한정
    • 전자공학회논문지 IE
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    • 제48권4호
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    • pp.13-18
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    • 2011
  • 본 논문에서는 LDO 레귤레이터의 공정변화에 따른 특성변화를 1 ${\mu}m$ 20 V 고 전압 CMOS 공정을 사용하여 시뮬레이션 하였다. 공정변화에 따른 3종류의 SPICE 파라미터(문턱전압과 실효채널길이가 평균적인 Typ(typical), 평균 이하인 FF(fast), 평균 이상인 SS(slow) 파라미터)를 LDO 레귤레이터 시뮬레이션에 활용하였다. 시뮬레이션 결과,SS 파라미터 사용의 경우, 라인 레귤레이션이 3.6 mV/V, 부하 레귤레이션이 0.4 mV/mA, 부하전류 변화에 따른 출력전압이 안정화되는 시간이 평균 0.86 ${\mu}s$였다. 그리고 Typ 파라미터 사용의 경우, 라인 레귤레이션이 4.2 mV/V, 부하 레귤레이션이 0.44 mV/mA, 부하전류 변화에 따른 출력전압이 안정화되는 시간이 평균 0.62 ${\mu}s$였다. 마지막으로 FF 파라미터 사용의경우 라인 레귤레이션이 7.0 mV/V, 부하 레귤레이션이 0.56 mV/mA, 부하전류 변화에 따른 출력전압이 안정화되는 시간이 평균 0.27 ${\mu}s$였다. 향후, 이러한 공정변화에 따른 회로 특성의 변화를 고려한 효율적 회로설계가 필요할 것으로 사료된다.

Optical Characterizations of TlBr Single Crystals for Radiation Detection Applications

  • Oh, Joon-Ho;Kim, Dong Jin;Kim, Han Soo;Lee, Seung Hee;Ha, Jang Ho
    • Journal of Radiation Protection and Research
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    • 제41권2호
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    • pp.167-171
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    • 2016
  • Background: TlBr is of considerable technological importance for radiation detection applications where detecting high-energy photons such as X-rays and ${\gamma}$-rays are of prime importance. However, there were few reports on investigating optical properties of TlBr itself for deeper understandings of this material and for making better radiation detection devices. Thus, in this paper, we report on the optical characterizations of TlBr single crystals. Spectroscopic ellipsometry (SE) and photoluminescence (PL) measurements at RT were performed for this work. Materials and Methods: A 2-inch TlBr single crystalline ingot was grown by using the vertical Bridgman furnace. SE measurements were performed at RT within the photon energy range from 1.1 to 6.5 eV. PL measurements were performed at RT by using a home-made PL system equipped with a 266 nm-laser and a spectrometer. Results and Discussion: Dielectric responses from SE analysis were shown to be slightly different among the different samples possibly due to the different structural/optical properties. Also from the PL measurements, it was observed that the peak intensities of the middle samples were significantly higher than those of the other two samples. With the given values for permittivity of free space (${\varepsilon}_0=8.854{\times}10^{-12}F{\cdot}m^{-1}$), thickness (d = 1 mm), and area ($A=10{\times}10mm^2$) of the TlBr sample, capacitances of TlBr were 6.9 pF (at $h{\nu}=3eV$) and 4.4 pF (at $h{\nu}=6eV$), respectively. Conclusion: SE and PL measurement and analysis were performed to characterize TlBr samples from the optical perspective. It was observed that dielectric responses of different TlBr samples were slightly different due to the different material properties. PL measurements showed that the middle sample exhibited much stronger PL emission peaks due to the better material quality. From the SE analysis, optical, dielectric constants were extracted, and calculated capacitances were in the few pF range.

저온 공정 온도에서 $Al_2O_3$ 게이트 절연물질을 사용한 InGaZnO thin film transistors

  • 우창호;안철현;김영이;조형균
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2010년도 하계학술대회 논문집
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    • pp.11-11
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    • 2010
  • Thin-film-transistors (TFTs) that can be deposited at low temperature have recently attracted lots of applications such as sensors, solar cell and displays, because of the great flexible electronics and transparent. Transparent and flexible transistors are being required that high mobility and large-area uniformity at low temperature [1]. But, unfortunately most of TFT structures are used to be $SiO_2$ as gate dielectric layer. The $SiO_2$ has disadvantaged that it is required to high driving voltage to achieve the same operating efficiency compared with other high-k materials and its thickness is thicker than high-k materials [2]. To solve this problem, we find lots of high-k materials as $HfO_2$, $ZrO_2$, $SiN_x$, $TiO_2$, $Al_2O_3$. Among the High-k materials, $Al_2O_3$ is one of the outstanding materials due to its properties are high dielectric constant ( ~9 ), relatively low leakage current, wide bandgap ( 8.7 eV ) and good device stability. For the realization of flexible displays, all processes should be performed at very low temperatures, but low temperature $Al_2O_3$ grown by sputtering showed deteriorated electrical performance. Further decrease in growth temperature induces a high density of charge traps in the gate oxide/channel. This study investigated the effect of growth temperatures of ALD grown $Al_2O_3$ layers on the TFT device performance. The ALD deposition showed high conformal and defect-free dielectric layers at low temperature compared with other deposition equipments [2]. After ITO was wet-chemically etched with HCl : $HNO_3$ = 3:1, $Al_2O_3$ layer was deposited by ALD at various growth temperatures or lift-off process. Amorphous InGaZnO channel layers were deposited by rf magnetron sputtering at a working pressure of 3 mTorr and $O_2$/Ar (1/29 sccm). The electrodes were formed with electron-beam evaporated Ti (30 nm) and Au (70 nm) bilayer. The TFT devices were heat-treated in a furnace at $300^{\circ}C$ and nitrogen atmosphere for 1 hour by rapid thermal treatment. The electrical properties of the oxide TFTs were measured using semiconductor parameter analyzer (4145B), and LCR meter.

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후열 처리 온도 변화에 따른 phosphorus doped ZnO 박막의 전기적 및 광학적 특성 (Electrical and Optical Properties of phosphorus doped ZnO Thin Films at Various Post-Annealing Temperatures)

  • 한정우;강성준;윤영섭
    • 대한전자공학회논문지SD
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    • 제46권2호
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    • pp.9-14
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    • 2009
  • 본 연구에서는 sapphire 기판위에 P (phosphorus) 도핑된 ZnO 박막을 제작한 후, 산소 분위기에서 후열 처리 온도가 박막의 전기적 및 광학적 특성에 미치는 영향에 대해서 조사하였다. XRD 측정 결과, 후열 처리 온도에 무관하게 모든 박막이 c축 배향성을 나타내었다. Hall 측정 결과, $850^{\circ}C$에서 후열 처리한 박막에서만 p형 전도 특성이 관찰되었다. 이때의 홀 캐리어 농도와 홀 이동도는 각각 $1.18{\times}1016cm^{-3}$$0.96cm^2/Vs$의 값을 나타내었다. 저온 PL 측정 결과, $850^{\circ}C$에서 후열 처리한 박막의 경우 p형 특성을 나타내는 상당량의 억셉터가 관련된 A0X (3.351eV), FA(3.283eV) 및 DAP (3.201eV) 피크가 관찰되었다. 향후 P 도핑된 ZnO 박막의 공정 조건과 후열 처리 조건을 최적화시킨다면, 차세대 광소자에 응용될 수 있는 매우 유망한 재료로 주목받을 것으로 기대된다.

${N_2}O$ 플라즈마에 의한 AlGaN/GaN HEMT의 누설전류 감소 (Reduction of gate leakage current for AlGaN/GaN HEMT by ${N_2}O$ plasma)

  • 양전욱
    • 전기전자학회논문지
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    • 제11권4호
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    • pp.152-157
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    • 2007
  • 본 연구에서는 AlGaN/GaN HEMT (High electron mobility transistor)를 제작하고 20 mTorr의 챔버 압력과 15 sccm의 ${N_2}O$ 유량, 40 W의 RF 전력의 조건으로 원거리에서 형성된 플라즈마로 소스와 드레인 영역을 10초${\sim}$120초 동안 처리하여 HEMT의 전기적 특성을 관찰하였다. 상온에서 ${N_2}O$ 플라즈마에 처리한 경우 HEMT의 특성이 변화하지 않았으나 $200^{\circ}C$의 온도에서 10초 동안 처리한 경우 게이트 길이가 1um, 소스와 드레인 사이의 거리가 4um인 HEMT의 게이트 누설전류가 246 nA로부터 1.2 pA로 크게 감소하였다. 또한 25 um 떨어진 200um 폭의 두 활성층 사이 누설전류가 3 uA로부터 7 nA로 감소하였으며 720 ${\Omega}/{\box}$의 활성층의 면저항을 608 ${\Omega}/{\box}$로 감소시켜 도전율의 증가를 나타내기도 하였다. ${N_2}O$ 플라즈마의 처리에 의한 전기적 특성 개선은 10초 이내의 짧은 시간 동안 이루어지며 더 이상의 처리는 누설전류 특성 개선에 도움이 되지 않았다. 또한 ${N_2}O$ 플라즈마 처리로 개선된 특성은 $SiO_2$의 증착과 식각 후에도 개선된 특성이 유지되었다. ${N_2}O$ 플라즈마의 처리는 트랜지스터의 트랜스컨덕턴스와 드레인 전류의 증가, 드레인 전류의 차단특성의 개선에도 기여하여 고품위의 AlGaN/GaN HEMT 제작에 효과적으로 이용될 수 있음이 확인되었다.

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Growth of SiC Oxidation Protective Coating Layers on graphite substrates Using Single Source Precursors

  • Kim, Myung-Chan;Heo, Cheol-Ho;Park, Jin-Hyo;Park, Seung-Jun;Han, Jeon-Geon
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 1999년도 제17회 학술발표회 논문개요집
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    • pp.122-122
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    • 1999
  • Graphite with its advantages of high thermal conductivity, low thermal expansion coefficient, and low elasticity, has been widely used as a structural material for high temperature. However, graphite can easily react with oxygen at even low temperature as 40$0^{\circ}C$, resulting in CO2 formation. In order to apply the graphite to high temperature structural material, therefore, it is necessary to improve its oxidation resistive property. Silicon Carbide (SiC) is a semiconductor material for high-temperature, radiation-resistant, and high power/high frequency electronic devices due to its excellent properties. Conventional chemical vapor deposited SiC films has also been widely used as a coating materials for structural applications because of its outstanding properties such as high thermal conductivity, high microhardness, good chemical resistant for oxidation. Therefore, SiC with similar thermal expansion coefficient as graphite is recently considered to be a g행 candidate material for protective coating operating at high temperature, corrosive, and high-wear environments. Due to large lattice mismatch (~50%), however, it was very difficult to grow thick SiC layer on graphite surface. In theis study, we have deposited thick SiC thin films on graphite substrates at temperature range of 700-85$0^{\circ}C$ using single molecular precursors by both thermal MOCVD and PEMOCVD methods for oxidation protection wear and tribological coating . Two organosilicon compounds such as diethylmethylsilane (EDMS), (Et)2SiH(CH3), and hexamethyldisilane (HMDS),(CH3)Si-Si(CH3)3, were utilized as single source precursors, and hydrogen and Ar were used as a bubbler and carrier gas. Polycrystalline cubic SiC protective layers in [110] direction were successfully grown on graphite substrates at temperature as low as 80$0^{\circ}C$ from HMDS by PEMOCVD. In the case of thermal MOCVD, on the other hand, only amorphous SiC layers were obtained with either HMDS or DMS at 85$0^{\circ}C$. We compared the difference of crystal quality and physical properties of the PEMOCVD was highly effective process in improving the characteristics of the a SiC protective layers grown by thermal MOCVD and PEMOCVD method and confirmed that PEMOCVD was highly effective process in improving the characteristics of the SiC layer properties compared to those grown by thermal MOCVD. The as-grown samples were characterized in situ with OES and RGA and ex situ with XRD, XPS, and SEM. The mechanical and oxidation-resistant properties have been checked. The optimum SiC film was obtained at 85$0^{\circ}C$ and RF power of 200W. The maximum deposition rate and microhardness are 2$mu extrm{m}$/h and 4,336kg/mm2 Hv, respectively. The hardness was strongly influenced with the stoichiometry of SiC protective layers.

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Bi$_{4}$Ti$_{3}$O$_{12}$ 박막의 제작과 그 특성에 관한 연구 (Preparation of a Bi$_{4}$Ti$_{3}$O$_{12}$ Thin Film and Its Electrical Properties)

  • 강성준;장동훈;민경진;김성진;정양희;윤영섭
    • 대한전자공학회논문지SD
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    • 제37권4호
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    • pp.7-14
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    • 2000
  • Bi/sub 4/Ti/sub 3/O/sub 12/ (BIT) 박막을 acetate 계 precursor 를 이용한 sol-gel 법으로 제작한 후, 구조적 및 전기적 특성을 조사하여 NVFRAM (Won-Volatile Ferroelectric RAM)으로의 응용가능성을 조사하였다. DT-TG (Differential Thermal-Thermal Gravimetric) 분석으로 drying 온도와 annealing 온도가 각각 400℃ 와 650℃ 인 BIT 박막의 열처리조건을 확립하였다. Pt/Ta/Sio/sub 2//Si 기판 위에 제작된 BIT 박막은 완전한 orthorhombic perovskite상을 가지며, 입자크기가 약 100nm 이고 표면 거칠기는 약 70.2Å 으로 비교적 치밀한 형상을 나타내었다. 10㎑ 의 주파수에서 비유전률과 유전손실은 각각 176 과 0.038 이었으며, 100 ㎸/cm 의 전기장에서 누설전류밀도는 4.71㎂/㎠ 이었다. ±250㎸/㎝ 에서 이력곡선을 측정한 결과, 잔류분극 (Pr)과 항전계 (Ec)는 각각 5.92μC/㎠ 과 86.3㎸/㎝ 이었다. BIT 박막에 ±5V 의 사각펄스를 인가하여 피로특성을 측정한 결과, 잔류분극은 초기값 5.92μC/㎠ 에서 10/sup 9/회에서는 3.95μC/㎠ 로 약 33% 감소하였다.

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Characteristics of InGaAs/GaAs/AlGaAs Double Barrier Quantum Well Infrared Photodetectors

  • 박민수;김호성;양현덕;송진동;김상혁;윤예슬;최원준
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.324-325
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    • 2014
  • Quantum wells infrared photodetectors (QWIPs) have been used to detect infrared radiations through the principle based on the localized stated in quantum wells (QWs) [1]. The mature III-V compound semiconductor technology used to fabricate these devices results in much lower costs, larger array sizes, higher pixel operability, and better uniformity than those achievable with competing technologies such as HgCdTe. Especially, GaAs/AlGaAs QWIPs have been extensively used for large focal plane arrays (FPAs) of infrared imaging system. However, the research efforts for increasing sensitivity and operating temperature of the QWIPs still have pursued. The modification of heterostructures [2] and the various fabrications for preventing polarization selection rule [3] were suggested. In order to enhance optical performances of the QWIPs, double barrier quantum well (DBQW) structures will be introduced as the absorption layers for the suggested QWIPs. The DBWQ structure is an adequate solution for photodetectors working in the mid-wavelength infrared (MWIR) region and broadens the responsivity spectrum [4]. In this study, InGaAs/GaAs/AlGaAs double barrier quantum well infrared photodetectors (DB-QWIPs) are successfully fabricated and characterized. The heterostructures of the InGaAs/GaAs/AlGaAs DB-QWIPs are grown by molecular beam epitaxy (MBE) system. Photoluminescence (PL) spectroscopy is used to examine the heterostructures of the InGaAs/GaAs/AlGaAs DB-QWIP. The mesa-type DB-QWIPs (Area : $2mm{\times}2mm$) are fabricated by conventional optical lithography and wet etching process and Ni/Ge/Au ohmic contacts were evaporated onto the top and bottom layers. The dark current are measured at different temperatures and the temperature and applied bias dependence of the intersubband photocurrents are studied by using Fourier transform infrared spectrometer (FTIR) system equipped with cryostat. The photovoltaic behavior of the DB-QWIPs can be observed up to 120 K due to the generated built-in electric field caused from the asymmetric heterostructures of the DB-QWIPs. The fabricated DB-QWIPs exhibit spectral photoresponses at wavelengths range from 3 to $7{\mu}m$. Grating structure formed on the window surface of the DB-QWIP will induce the enhancement of optical responses.

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Formation and Characteristics of the Fluorocarbonated SiOF Film by $O_2$/FTES-Helicon Plasma CVD Method

  • Kyoung-Suk Oh;Min-Sung Kang;Chi-Kyu Choi;Seok-Min Yun
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 1998년도 제14회 학술발표회 논문개요집
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    • pp.77-77
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    • 1998
  • Present silicon dioxide (SiOz) 떠m as intennetal dielectridIMD) layers will result in high parasitic c capacitance and crosstalk interference in 비gh density devices. Low dielectric materials such as f f1uorina뼈 silicon oxide(SiOF) and f1uoropolymer IMD layers have been tried to s이ve this problem. I In the SiOF ftlm, as fluorine concentration increases the dielectric constant of t뼈 film decreases but i it becomes unstable and wa않r absorptivity increases. The dielectric constant above 3.0 is obtain어 i in these ftlms. Fluoropolymers such as polyte$\sigma$따luoroethylene(PTFE) are known as low dielectric c constant (>2.0) materials. However, their $\alpha$)Or thermal stability and low adhesive fa$\pi$e have h hindered 야1리ru뚱 as IMD ma따"ials. 1 The concept of a plasma processing a찌Jaratus with 비gh density plasma at low pressure has r received much attention for deposition because films made in these plasma reactors have many a advantages such as go여 film quality and gap filling profile. High ion flux with low ion energy in m the high density plasma make the low contamination and go어 $\sigma$'Oss피lked ftlm. Especially the h helicon plasma reactor have attractive features for ftlm deposition 야~au똥 of i앙 high density plasma p production compared with other conventional type plasma soun:es. I In this pa야Jr, we present the results on the low dielectric constant fluorocarbonated-SiOF film d밑JOsited on p-Si(loo) 5 inch silicon substrates with 00% of 0dFTES gas mixture and 20% of Ar g gas in a helicon plasma reactor. High density 띠asma is generated in the conventional helicon p plasma soun:e with Nagoya type ill antenna, 5-15 MHz and 1 kW RF power, 700 Gauss of m magnetic field, and 1.5 mTorr of pressure. The electron density and temperature of the 0dFTES d discharge are measUI벼 by Langmuir probe. The relative density of radicals are measured by optic허 e emission spe따'Oscopy(OES). Chemical bonding structure 3I피 atomic concentration 따'C characterized u using fourier transform infrared(FTIR) s야3띠"Oscopy and X -ray photonelectron spl:’따'Oscopy (XPS). D Dielectric constant is measured using a metal insulator semiconductor (MIS;AVO.4 $\mu$ m thick f fIlmlp-SD s$\sigma$ucture. A chemical stoichiome$\sigma$y of 야Ie fluorocarbina$textsc{k}$영-SiOF film 따~si야영 at room temperature, which t the flow rate of Oz and FTES gas is Isccm and 6sccm, res야~tvely, is form려 야Ie SiouFo.36Co.14. A d dielec$\sigma$ic constant of this fIlm is 2.8, but the s$\alpha$'!Cimen at annealed 5OOt: is obtain려 3.24, and the s stepcoverage in the 0.4 $\mu$ m and 0.5 $\mu$ m pattern 킹'C above 92% and 91% without void, res야~tively. res야~tively.

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