• 제목/요약/키워드: substrate thickness

검색결과 1,911건 처리시간 0.029초

소오스-드레인 기생용량을 개선한 박막트랜지스터 제조공정 (The Fabrication of a-Si:H TFT Improving Parasitic Capacitance of Source-Drain)

  • 허창우
    • 한국정보통신학회논문지
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    • 제8권4호
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    • pp.821-825
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    • 2004
  • 본 연구는 에치스토퍼를 기존의 방식과 다르게 적용하여 수소화 된 비정질 실리콘 박막 트랜지스터의 제조공정을 단순화하고, 박막 트랜지스터의 게이트와 소오스-드레인간의 기생용량을 줄인다. 본 연구의 수소화 된 비정질 실리콘 박막 트랜지스터는 Inverted Staggered 형태로 게이트 전극이 하부에 있다. 실험 방법은 게이트전극, 절연층 , 전도층, 에치스토퍼 및 포토레지스터층을 연속 증착한다. 스토퍼층을 게이트 전극의 패턴으로 남기고, 그 위에 n+a-Si:H 층 및 NPR(Negative Photo Resister)을 형성시킨다. 상부 게이트 전극과 반대의 패턴으로 NPR층을 패터닝하여 그것을 마스크로 상부 n+a-Si:H 층을 식각하고, 남아있는 NPR층을 제거한다. 그 위에 Cr층을 증착한 후 패터닝하여 소오스-드레인 전극을 위한 Cr층을 형성시켜 박막 트랜지스터를 제조한다. 이렇게 제조하면 기존의 박막 트랜지스터에 비하여 특성은 같고, 제조공정은 줄어들며, 또한 게이트와 소오스-드레인간의 기생용량이 줄어들어 동작속도를 개선시킬 수 있다.

5.8GHz ISM대역 국부 발진기용 능동 공진 발진기 설계 및 제작 (Design and Fabrication of a Active Resonator Oscillator for Local Oscillator in ISM Band(5.8GHz))

  • 신용환;임영석
    • 한국정보통신학회논문지
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    • 제8권4호
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    • pp.886-893
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    • 2004
  • 본 논문에서는 트랜지스터를 이용해서 이득을 갖는 능동 대역 통과 필터, 부성저항 특성을 갖는 능동 공진기를 이용한 능동 공진 발진기를 설계 제작하였다. 제안된 능동 공진 발진기는 ISM 대역의 국부 발진기로 사용 가능하도록 5.5GHz의 발진주파수를 갖도록 설계하였다. 설계된 능동 공진 발진기는 유전율 3.38, 유전체 두께 0.508mm, 금속 두께 0.018mm인 기판 위에 구현하였다. 이득을 갖는 능동 대역 통과 필터를 이용한 능동 공진 발진기는 5.6GHz의 발진주파수와 -2Bm의 출력과 100kHz 옵셋에서의 위상잡음 특성은 -81dBc/Hz이다. 부성저항 특성을 갖는 능동 공진기를 이용한 능동 공진 발진기는 5.8GHZ의 발진주파수와- 4dBm의 출력과 100kHz 옵셋에서의 위상잡음 특성은 -91dBc/Hz이다.

부성저항 특성을 갖는 능동 인덕터와 능동 캐패시터를 이용한 능동 공진 발진기 설계 및 제작 (Design and Fabrication of a Active Resonator Oscillator using Active Inductor and Active Capacitor with Negative Resistance)

  • 신용환;임영석
    • 한국정보통신학회논문지
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    • 제7권8호
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    • pp.1591-1597
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    • 2003
  • 본 논문에서는 HEMT(Agilent ATF­34143)를 이용한 부성저항 특성을 갖는 능동 인덕터와 캐패시터를 이용해 능동 공진 발진기 제작에 응용하였다. 5.5GHz 대역에서 능동 인덕터는 ­25$\Omega$의 부성저항과 2.4nH의 인덕턴스를 갖고, 능동 캐패시터는 ­14$\Omega$의 부성저항과 0.35pF의 캐패시턴스를 갖도록 설계하였다. 설계된 능동 인덕터와 캐패시터를 이용 5.8GHz ISM 대역의 국부 발진기로 사용 가능한 능동 공진 발진기를 설계하였다. 애질런트사의 ADS 2002C를 이용 시뮬레이션 하였다. 설계된 발진기는 유전율 3.38, 유전체 두께 0.508mm, 금속 두께 0.018mm인 기판위에 HMIC 형태로 구현하였다. 제작된 능동 공진 발진기는 5.68GHz의 기본 발진주파수에서 ­3.6㏈m의 출력을 얻었고, 100KHz 옵셋에서 ­81㏈c1/Hz의 위상잡음 특성을 갖는다.

Plasma nitriding on chromium electrodeposit

  • Wang Liang;K.S. Nam;Kim, D.;Kim, M.;S.C. Kwon
    • 한국표면공학회:학술대회논문집
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    • 한국표면공학회 2001년도 추계학술발표회 초록집
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    • pp.29-30
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    • 2001
  • This paper presents some results of plasma nitriding on hard chromium deposit. The substrates were C45 steel and $30~50{\;}\mu\textrm{m}$ of chromium deposit by electroplating was formed. Plasma nitriding was carried out in a plasma nitriding system with $95NH_3{\;}+{\;}SCH_4$ atmosphere at the pressure about 600 Pa and different temperature from $450^{\circ}C{\;}to{\;}720^{\circ}C$ for various time. Optical microscopy and X-ray diffraction were used to evaluate the characteristics of surface nitride layer formed by nitrogen diffusion from plasma atmosphere inward iCr coating and interface carbide layer formed by carbon diffusion from substrate outward Cr coating. The microhardness was measured using microhareness tester at the load of 100 gf. Corrosion resistance was evaluated using the potentiodynamic measurement in 3.5% NaG solution. A saturated calomel electrode (SiCE) was used as the reference electrode. Fig.1 shows the typical microstructures of top surface and cross-section for nitrided and unnitrided samples. Aaer plasma nitriding a sandwich structure was formed consisting of surface nitride layer, center chromium layer and interface carbide layer. The thickness of nitride and carbide layers was increased with the increase of processing temperature and time. Hardness reached about 1000Hv after nitriding while 900Hv for unnitrided hard chromium deposit. X-ray diffraction indicated that surface nitrided layer was a mixture of $Cr_2N$ and CrN at low temperature and erN at high temperature (Fig.2). Anodic polarization curves showed that plasma nitriding can greatly improve the corrosion resistance of chromium e1ectrodeposit. After plasma nitriding, the corrosion potential moved to noble direction and passive current density was lower by 1 to 4 orders of magnitude compared with chromium deposit(Fig.3).

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ITO/p-InP 태양전지 제작 (The fabrication of ITO/p-InP solar cells)

  • 맹경호;김선태;송복신;문동찬
    • E2M - 전기 전자와 첨단 소재
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    • 제7권3호
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    • pp.243-251
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    • 1994
  • ITO(Indium Tin Oxide) film with thickness of 1500.angs. was prepared by an e-beam evaporator onto a glass and a p-type InP wafer (100) LEC grown Zn-doped p=2.3*10$\^$16/cm$\^$-3/), in which the components of ITO used for evaporation source were hot pressed pellets 1 mole% ln$\_$2/O$\_$3/+9 mole% SnO$\_$2/, and evaporated in O$\_$2/ ambient. The optimum conditions to preparation of ITO thin film were the substrate temperature of 350.deg. C, the injected oxygen pressure of 2*10$\^$-4/ torr, and the evaporation speed of 0.2-0.3.angs./sec, respectively. In these optimum conditions, the resistivity and the carrier concentration were 5.3*10$\^$-3/ .ohm.-cm, 6.5*10$\^$20/cm$\^$-3/, and the transmittance was over 80%. From the results of J-V measurements in ITO/p-InP structure solar cells, the higher pressure of injected oxygen, the more open circuit voltage. The efficiency of ITO/p-InP solar cell without the grid line contact, prepared by the optimum evaporation conditions, was 7.19%. By using the grid line contact, the efficiency, the open circuit voltage, the short circuit current density, the fill factor, the series resistance, and the shunt resistance were 8.5%, 0.47V, 29.48 mAcm$\^$-2/ , 61.35%, 3.ohm., and 26.6k.ohm., respectively.

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산소 분압비에 따른 $TiO_2$ 박막의 특성평가 (The properties of $TiO_2$ thin films by oxygen partial pressure)

  • 양현훈;임정명;박중윤;정운조;박계춘
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2003년도 춘계학술대회 논문집 센서 박막재료 반도체 세라믹
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    • pp.154-157
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    • 2003
  • $TiO_2$ thin films were fabricated by RF magnetron sputtering system at by controlling deposition times, ratios of $Ar:O_2$ partial presser ratio and substrate conditions. And the surface, cross-section morphology, microstructure, and composition ratio of the films were analyzed by FE-SEM, TEM and XPS. Besides, the optical absorption and transmittance of the $TiO_2$ films were measured by a UV-VIS-NIR Spectrophotometer, and photocatalytic properties were studied by G${\cdot}$C Analyzer & Data Analysis system. As the result, when $TiO_2$ thin film was made at deposition time of 120[min] and $Ar:O_2$ ratio of 60:40, the best structural and optical properties among many thin films could be accepted. The best results of properties were as follows: thickness; 360~370[nm), grain size; 40[nm], gap between two peak binding energy; $5.8{\pm}0.05[eV]$ ($2_{p3/2}$ peak and $2_{p1/2}$ peak of Ti was show at $458.3{\pm}0.05[eV]$ and $464.1{\pm}0.05[eV]$ respectively), binding energy; $530{\pm}0.05[eV]$, optical energy band gap; 3.4[eV].

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$Al_2Nq_4$를 발광층으로 이용한 OLED의 계면 및 발광 특성에 관한 연구 (A Study on the Interface and Luminescent Properties of OLED using $Al_2Nq_4$ as an Emitting Layer)

  • 양기성;이호식;신훈규;김두석;김정균;권영수
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2004년도 추계학술대회 논문집 전기물성,응용부문
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    • pp.215-219
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    • 2004
  • Metal-chelate derivatives have been investigated intensively as an emitting layer and recognize to have excellent electroluminescence(EL) properties. We synthesized new luminescent material, 1,4-dihydoxy-5,8-naphtaquinone $Aiq_3$ complex($Al_2Nq_4$) and investigated the electrical optical properties. OLED has potential candidates for information display with merits of thickness, low power and high efficiency. Although the OLED show a lot of advantages for information display, it has the limit of inorganic(metal)/ organic interface. In this study, the two methods are used to study the interface of metal/organic in OLED. First, we treated $O_2$ plasma on an ITO thin film by using RIE system, and analyzed the ingredient of ITO thin film according to change of the processing conditions. We used the RDS and the XPS for the ingredient analysis of the surface and bulk. We measured electrical resistivity using Four-Point-Probe and calculated sheet resistance, and ITO surface roughness was measured by using AFM. We fabricated OLED using substrate that was treated optimum ITO surface. Second, we used the buffer layer of CuPc to improve the characteristics of the interface and the hole injection in OLED. The result of the study for electrical and optical properties by using I V L T System(Flat Panel Display Analysis System), we confirmed that the electrical properties and the luminance properties were improved.

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KSTAR 토카막의 Alfvén파 RF 스펙트럼 측정을 위한 광대역 보우타이 안테나 설계 (Design of A Broadband Bowtie Antenna for RF Spectral Measurements of Alfvén-wave in the KSTAR Tokamak)

  • 우동식;김성균;김강욱;최현철
    • 센서학회지
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    • 제25권1호
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    • pp.46-50
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    • 2016
  • During KSTAR plasma experiments, torsional $Alfv\acute{e}n$ waves in the frequency of few GHz or below were detected. To understand this plasma waves during the crash of MHD instabilities, an RF spectrometer has been developed for detection of the radiated RF signals in the KSTAR Tokamak. It has the capability of broadband RF spectral measurement (50 ~ 400 MHz). To detect the broadband RF signals which are radiated from the KSTAR systems, a broadband antenna is the key feature of the RF spectrometer. In this paper, a broadband bowtie antenna for detection of $Alfv\acute{e}n$-waves in the KSTAR Tokamak is presented. Planar-type bowtie antenna is designed and fabricated on an FR4 substrate with thickness of 1.6 mm. The antenna consists of bowtie shaped balanced radiators and broadband planar balun. The antenna is designed to have an input impedance of 50 Ohm, and a taper-shaped balun is adopted for field and impedance matching between 50 Ohm transmission line to 110 Ohm feeding network of balanced radiators. The implemented antenna provides around -3 to 3 dBi of gain for the whole frequency band. The VSWR of the bowtie antenna is less than 12:1 over the frequency bandwidth of 50 to 2000 MHz.

Preparation of Nanocolumnar In2O3 Thin Films for Highly Sensitive Acetone Gas Sensor

  • Han, Soo Deok;Song, Young Geun;Shim, Young-Seok;Lee, Hae Ryong;Yoon, Seok-Jin;Kang, Chong-Yun
    • 센서학회지
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    • 제25권6호
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    • pp.383-387
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    • 2016
  • Well-ordered nanocolumnar indium oxide ($In_2O_3$) thin films have been successfully fabricated by glancing angle deposition (GAD) using an e-beam evaporator. Nanocolumnar structures have a porous and large surface area with a narrow neck between nanocolumns, which allows them to detect minute amounts of gases. The nanocolumnar $In_2O_3$ thin films were fabricated by the GAD process at five different positions, viz. top, bottom, center, left, and right in a four inch substrate holder. There was a divergence in the thickness and the base resistance of each sensor. However, all the sensors exhibited extremely high sensitivity that was greater than $10^3$ times the change in electrical resistance after being exposed to 50 ppm of acetone gas at $300^{\circ}C$. Furthermore, the nanocolumnar $In_2O_3$ sensors displayed an extremely low detection limit (1.2 ppb) in dry atmosphere as well as in high humidity (80%). We demonstrated that the GAD nanocolumnar $In_2O_3$ sensors have an enormous potential for many applications owing to their particularly simple and reliable fabrication process.

AFM을 이용한 스트렙타비딘-바이오틴 단백질 복합체의 흡착 분석 (Absorption analysis of streptavidin-biotin complexes using AFM)

  • 박지은;김동선;최호진;신장규;김판겸;임근배
    • 센서학회지
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    • 제15권4호
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    • pp.237-244
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    • 2006
  • Atomic force microscope (AFM) has become a common tool for the structural and physical studies of biological macromolecules, mainly because it provides the ability to perform experiments with samples in a buffer solution. In this study, structure of proteins and nucleic acids has been studied in their physiological environment that allows native intermolecular complexes to be formed. Cr and Au were deposited on p-Si (100) substrate by thermal evaporation method in sequence with the thickness of $200{\AA}$ and $500{\AA}$, respectively, since Au is adequate for immobilizing biomolecules by forming a self-assembled monolayer (SAM) with semiconductor-based biosensors. The SAM, streptavidin and biotin interacted each other with their specific binding energy and their adsorption was analyzed using the Bio-AFM both in a solution and under air environment. A silicon nitride tip was used as a contact tip of Bio-AFM measurement in a solution and an antimony doped silicon tip as a tapping tip under air environment. Actual morphology could also be obtained by 3-dimensional AFM images. The length and agglomerate size of biomolecules was measured in stages. Furthermore, $R_{a}$ (average of surface roughness) and $R_{ms}$ (mean square of surface roughness) and surface density for the adsorbed surface were also calculated from the AFM image.