• Title/Summary/Keyword: S-doping

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Preparation and Characteristics of Visible-Light-Active $TiO_2-_xN_x$ Nanoparticles for Photocatalytic Activities (가시광 활성을 갖는 광촉매용 $TiO_2-_xN_x$ 나노입자의 제조 및 특성)

  • Yun, Tae-Kwan;Bae, Jae-Young
    • Journal of Korean Society of Environmental Engineers
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    • v.31 no.11
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    • pp.1019-1024
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    • 2009
  • Visible-light-active $TiO_2-_xN_x$ nanoparticles with a homogeneous anatase crystalline structure were successfully prepared through a hydrolysis of $TiCl_4$ with ammonia solution. The samples were characterized by X-ray diffraction (XRD), Transmission electron microscopy (TEM), $N_2$-sorption, and UV-vis diffuse reflectance spectra (DRS) techniques. The light absorption onset shifted from 390 nm on pure $TiO_2$ to the visible region at 530 nm on nitrogen-doped $TiO_2$. A clear decrease in the band gap was deduced from the DRS results. The photocatalytic activity was evaluated from the photodegradation of congo red solution under visible light irradiation. The photocatalyst showed the highest photocatalytic activity at an optimal value of nitrogen doping concentration. This was suggested that the nitrogen doping should have an important effects on the improvement of photocatalytic activity.

Effects of ZnO on the Piezoelectric Properties of PMS-PZT Ceramics (PMS-PZT 세라믹스의 압전특성에 미치는 ZnO의 영향)

  • Son Y.-J.;Hwang D.-Y.;Kim J.-C.;Cho K.-W.;Kim Y.-M.;Ur S.-C.;Kim I.-H.
    • Korean Journal of Materials Research
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    • v.14 no.11
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    • pp.764-768
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    • 2004
  • Perovskite Pb(Mn_{1/3}Sbu_{2/3})O_2-Pb(Zr,Ti)O_3\;(PMS-PZT) was prepared and ZnO doping effects on its piezoelectric properties were investigated. Pyrochlore phase was not identified in the PMS-PZT ceramics with $0\sim5\;mol\%$ ZnO sintered at $1100^{\circ}C$ for 2 hrs, and maximum sintered density of $7.92 g/cm^3$ was obtained. Piezoelectric charge constant and voltage constant increased to $359{\times}10^{-12}\;C/N\;and\;22.5{\times}10^{-13}\;Vm/N$, respectively, with increasing ZnO content. Mechanical quality factor reduced considerably with increasing ZnO content. When the ZnO content was 3 $mol\%$, electromechanical coupling factor and relative dielectric constant showed maximum values of $56\%$ and 1727, respectively. This should be evaluated by complicated variations of sintered density, tetragonality of lattice, grain size, and A-site vacancy generated by ZnO addition and $Zn^{2+}$ substitution.

VT-Modulation of Planar Tunnel Field-Effect Transistors with Ground-Plane under Ultrathin Body and Bottom Oxide

  • Sun, Min-Chul;Kim, Hyun Woo;Kim, Hyungjin;Kim, Sang Wan;Kim, Garam;Lee, Jong-Ho;Shin, Hyungcheol;Park, Byung-Gook
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.14 no.2
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    • pp.139-145
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    • 2014
  • Control of threshold voltage ($V_T$) by ground-plane (GP) technique for planar tunnel field-effect transistor (TFET) is studied for the first time using TCAD simulation method. Although GP technique appears to be similarly useful for the TFET as for the metal-oxide-semiconductor field-effect transistor (MOSFET), some unique behaviors such as the small controllability under weak ground doping and dependence on the dopant polarity are also observed. For $V_T$-modulation larger than 100 mV, heavy ground doping over $1{\times}10^{20}cm^{-3}$ or back biasing scheme is preferred in case of TFETs. Polarity dependence is explained with a mechanism similar to the punch-through of MOSFETs. In spite of some minor differences, this result shows that both MOSFETs and TFETs can share common $V_T$-control scheme when these devices are co-integrated.

Subthreshold Current Model for Threshold Voltage Shift Analysis in Junctionless Cylindrical Surrounding Gate(CSG) MOSFET (무접합 원통형 게이트 MOSFET에서 문턱전압이동 분석을 위한 문턱전압이하 전류 모델)

  • Jung, Hakkee
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.21 no.4
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    • pp.789-794
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    • 2017
  • Subthreshold current model is presented using analytical potential distribution of junctionless cylindrical surrounding-gate (CSG) MOSFET and threshold voltage shift is analyzed by this model. Junctionless CSG MOSFET is significantly outstanding for controllability of gate to carrier flow due to channel surrounded by gate. Poisson's equation is solved using parabolic potential distribution, and subthreshold current model is suggested by center potential distribution derived. Threshold voltage is defined as gate voltage corresponding to subthreshold current of $0.1{\mu}A$, and compared with result of two dimensional simulation. Since results between this model and 2D simulation are good agreement, threshold voltage shift is investigated for channel dimension and doping concentration of junctionless CSG MOSFET. As a result, threshold voltage shift increases for large channel radius and oxide thickness. It is resultingly shown that threshold voltage increases for the large difference of doping concentrations between source/drain and channel.

In-situ P-doped LPCVD Poly Si Films as the Electrodes of Pressure Sensor for High Temperature Applications (고온용 압력센서 응용을 위한 in-situ 인(P)-도핑 LPCVD Poly Si 전극)

  • Choi, Kyeong-Keun;Kee, Jong;Lee, Jeong-Yoon;Kang, Moon Sik
    • Journal of Sensor Science and Technology
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    • v.26 no.6
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    • pp.438-444
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    • 2017
  • In this paper, we focus on optimization of the in-situ phosphorous (P) doping of low-pressure chemical vapor deposited (LPCVD) poly Si resistors for obtaining near-zero temperature coefficient of resistance (TCR) at temperature range from 25 to $600^{\circ}C$. The deposited poly Si films were annealed by rapid thermal anneal (RTA) process at the temperature range from 900 to $1000^{\circ}C$ for 90s in nitrogen ambient to relieve intrinsic stress and decrease the TCR in the poly Si layer and get the Ohmic contact. After the RTA process, a roughness of the thin film was slightly changed but the grain size and crystallinity of the thin film with the increase in anneal temperature. The film annealed at $1,000^{\circ}C$ showed the behavior of Schottky contact and had dislocations in the films. Ohmic contact and TCR of $334.4{\pm}8.2$ (ppm/K) within 4 inch wafer were obtained in the measuring temperature range of 25 to $600^{\circ}C$ for the optimized 200 nm thick-poly Si film with width/length of $20{\mu}m/1,800{\mu}m$. This shows the potential of in-situ P doped LPCVD poly Si as a resistor for pressure sensor in harsh environment applications.

Hall 소자용 InAs 박막성장

  • 김성만;임재영;이철로;노삼규;신장규;권영수;유연희;김영진
    • Proceedings of the Korean Vacuum Society Conference
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    • 1999.07a
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    • pp.94-94
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    • 1999
  • 반도체 Hall 효과를 이용하여 자계를 검출하여 이를 전압신호로 출력하는 자기센서로는 주로 GaAs, InSb, InAs 등의 박막이 사용되고 있다. 자기센서의 응용분야가 최근에는 직류전류의 무접촉 검출, 자동차의 무접촉 회전 검출, 산업용 기계의 제어용 무접촉 위치검출 분야로 확대되고 있어 그 수요가 급증하고 있다. 이중 Hall 소자의 응용분야중 많은 활용이 기대되고 있는 자동차용 무접촉 센서는 -4$0^{\circ}C$~15$0^{\circ}C$의 온도범위에서 안정하게 작동하여야 하므로 온도 안정성이 매우 중요하다. 그러나 Hall 소자 시장의 80%를 점유하고 있는 InSb Hall 소자는 온도가 올라감에 따라 저항이 급격히 낮아지는 성질을 가지고 있으므로 10$0^{\circ}C$ 이상의 온도에서 사용하는 것이 불가능하다. 한편 InAs(에너지갭~0.18eV)는 InSb보다 에너지 갭이 크므로 고온에서도 작동이 가능하고 자계변화에 따른 출력의 직진성이 매우 좋다는 장점을 가지고 있다. 이러한 InAs Hall 소자를 실현하기 위해서 가장 중요한 것이 고품위의 InAs의 박막 성장기술이다. InAs 박막을 성장하기 위해서 사용되고 있는 기판은 GaAs이다. 그러나 GaAs 기판과 InAs 박막 사이에는 약 7% 정도의 격자부정합이 존재하기 때문에 높은 이동도를 가지는 고품위 박막을 성장시키기가 매우 어렵다. 이에 본 연구에서는 분자선에피택시 방법을 이용하여 GaAs 기판위에 고품위의 InAs 박막을 성장하는 기술을 연구하였으며, 성장된 InAs 박막의 특성을 DCX 및 Hall effect 등으로 조사하였다. InAs 박막 성장시 기판은 <0-1-1> 방향으로 2$^{\circ}$ off 된 GaAs(100)를 사용하였다. InAs 박막성장시 기판온도는 48$0^{\circ}C$로 하고 GaAs buffer 두께는 2000$\AA$로 하여 As flux 및 Si doping 농도등을 변화시켰다. 그 결과 Si doping 농도 2.21$\times$1017/am에서 10,952cm2/V.s의 이동도를 얻었다.

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Luminescence Properties of Zn2SiO4:Mn, M(M=Cr, Ti) Green Phosphors Prepared by Sol-gel Method (졸-겔법으로 제조한 Zn2SiO4:Mn, M(M=Cr, Ti) 녹색 형광체의 발광특성)

  • 안중인;한정화;박희동
    • Journal of the Korean Ceramic Society
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    • v.40 no.7
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    • pp.637-643
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    • 2003
  • In order to improve the photoluminescent properties and crystallinity, Zn$_2$SiO$_4$:Mn, M(M=Cr, Ti) phosphors were synthesized by the sol-gel method. The willemite single phase was obtained at 110$0^{\circ}C$, which is lower temperature than that of the conventional solid-state reaction (130$0^{\circ}C$). The characteristics of fired samples were obtained by a 147 nm excitation source under VUV (Vacuum Ultraviolet). To investigation the effect of co-dopant, the content of Mn and the ratio of $H_2O$ to TEOS was fixed as 2 ㏖% and 36. 1, respectively. The highest emission intensity was obtained when the concentration of Cr and Ti was 0.1 ㏖% relative to Zn$_2$SiO$_4$:Mn. While the emission intensity decrease continuously the decay time improved as increased the Cr concentration. In the case of Ti added samples, however, the emission intensity increase up to 2 ㏖% concentration.

Efficiency Improvement of $N^+NPP^+$ Si Solar Cell with High Low Junction Emitter Structure (고저 접합 에미터 구조를 갖는 $N^+NPP^+$ Si 태양전지의 효율 개선)

  • 장지근;김봉렬
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.21 no.1
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    • pp.62-70
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    • 1984
  • N+NPP+ HLEBSF (high low emitter back surface field) solar cells which have N+N high low junction in the emitter as well as N+PP+ BSF cells were designed and fabricated by using <111> oriented P type Si wafers with the resistivity of 10$\Omega$/$\textrm{cm}^2$ and the thickness of 13-15 mil. Physical parameters (impurity concentration, thickness) at each region of N+PP+ and N+NPP+ cell were made equally through same masks and simultaneous process except N region of HLEBSF cell to investigate the high low emitter junction effect for efficiency improvement. Under the light intensity of 100 mW/$\textrm{cm}^2$, total area (active area) conversion efficiency were typically 10.94% (12.16%) for N+PP+ BSF cells and 12.07% (13.41%) for N+N PP+ cells. Efficiency improvement of N+NPP+ cell which has high low emitter Junction structure is resulted from the suppression of emitter recombination current and the increasement of open circuit voltage (Voc) and short circuit current (Ish) by removing heavy doping effects occurring in N+ emitter region.

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표면변형에 따른 실리콘 태양전지의 전력변환효율 변화

  • Lee, Se-Won;O, Si-Deok;Sin, Hyeon-Uk;Jeong, Je-Myeong;Kim, Tae-Hwan;Sin, Jae-Cheol;Kim, Hyo-Jin
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.02a
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    • pp.387-387
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    • 2012
  • 결정 Si 및 비정질 Si 태양전지는 환경친화적이며 안정적인 물질로 전력변환 및 에너지 저장 장치에 중요하기 때문에 연구가 활발하게 진행되고 있다. 고효율 Si 태양전지를 제작하여 상용화하기에는 여러 가지 문제점이 있다. 공기와 비교하여 높은 굴절률을 갖고 있기 때문에 발생하는 반사를 줄이기 위해서 필요한 무반사 코팅층(Anti-reflective coating; ARC)은 주로 SiO2 와 SiNx 와 같은 유전체를 이용하여 사용하지만 이들 ARC 증착은 PECVD와 같은 진공장비를 사용하므로 제작 비용이 높아지는 단점이 있다. 나노선 또는 나노 팁과 같은 sub-wavelength 구조를 표면에 만들어 반사율을 줄이는 작업을 통해 ARC 공정비용을 감소하고 효율을 증진하는 연구가 활발히 진행되고 있다. CdS 양자점을 태양전지 표면에 형성함으로 ARC로 해결할 수 없는 단파장영역에 해당하는 부분을 줄이는 연구가 진행되었으며, 비정질의 경우 원기둥 형태의 태양전지 형태와 더불어 지름 방향으로의 PN 접합 나노로드 배열을 만들어 흡수면을 증가하여 효율을 증가한 연구도 진행되었다. 태양전지 표면의 형태를 V-groove 형태로 형성하여 입사하는 태양전지의 광밀도를 증가하는 이론적 결과도 발표되었다. 본 연구에서는 Si 태양전지의 표면변형에 따른 태양전지의 전력변환효율의 변화를 관찰하기 위하여 태양전지 표면의 texture 지름을 $3{\sim}15{\mu}m$, 간격을 $5{\sim}20{\mu}m$로 변화하고, 태양전지 표면의 나노 패턴을 2~10 nm 로 변화하여 반사율과 전력변환효율을 비교하였다. 나노와 마이크로 패턴은 각각 polystyrene nanosphere 와 photo mask를 이용하여 제작하였으며 PN junction Si 태양전지는 spin on dopant 방식으로 제작하여 성능을 조사하였다.

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Crystal growth and optical properties of near-stoichiometric $Zn:LiNbO_3$ fiber single crystal by ${\mu}-PD$ method (${\mu}-PD$ 법으로 성장시킨 near-stoichiometric 조성 $Zn:LiNbO_3$ fiber 단결정 성장 및 광손상 특성)

  • Lee, H.J.;Shur, J.W.;Shin, T.I.;Song, W.Y.;Yoon, D.H.
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.16 no.6
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    • pp.235-239
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    • 2006
  • ZnO-doped near-stoichiometric $LiNbO_3$ single crystals of $0.8{\sim}1.0mm$ diameter and $30{\sim}35mm$ length were grown by the micro-pulling down (U-PD) method. The structure of the grown crystals was confirmed by powder x-ray diffraction (XRD) patterns. Electron probe micro analysis (EPMA) showed that Zn ions were homogeneously incorporated In grown crystals. The threshold in ZnO doping level was confirmed that an abrupt change in the features of $OH^-$ absorption band as doping level reaching about 2 mol%.