• 제목/요약/키워드: ZnO doping

검색결과 316건 처리시간 0.027초

Optical characteristics of p-type ZnO epilayers doped with Sb by metalorganic chemical vapor deposition

  • Kwon, B.J.;Cho, Y.H.;Choi, Y.S.;Park, S.J.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2009년도 제38회 동계학술대회 초록집
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    • pp.122-122
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    • 2010
  • ZnO is a widely investigated material for the blue and ultraviolet solid-state emitters and detectors. It has been promoted due to a wide-band gap semiconductor which has large exciton binding energy of 60 meV, chemical stability and low radiation damage. However, there are many problems to be solved for the growth of p-type ZnO for practical device applications. Many researchers have made an efforts to achieve p-type conductivity using group-V element of N, P, As, and Sb. In this letter, we have studied the optical characteristics of the antimony-doped ZnO (ZnO:Sb) thin films by means of photoluminescence (PL), PL excitation, temperature-dependent PL, and time-resolved PL techniques. We observed donor-to-acceptor-pair transition at about 3.24 eV with its phonon replicas with a periodic spacing of about 72 meV in the PL spectra of antimony-doped ZnO (ZnO:Sb) thin films at 12 K. We also investigate thermal activation energy and carrier recombination lifetime for the samples. Our result reflects that the antimony doping can generate shallow acceptor states, leading to a good p-type conductivity in ZnO.

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N-doped ZnO 박막의 미세 구조 특성 (Nano-structural Characteristics of N-doped ZnO Thin Films)

  • 이은주;;박재돈;윤기완
    • 한국정보통신학회논문지
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    • 제13권11호
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    • pp.2385-2390
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    • 2009
  • 본 연구에서는 C-축 우선 배향 특성을 가지는 N-doped ZnO 박막을 증착하고 그 미세구조의 특성을 분석 비교하였다. ZnO박막은 $N_2O$ 가스 분위기에서 RF reactive magnetron sputtering 시스템을 사용하여 p-Si(100) 웨이퍼 위에 증착되었다. $N_2O$ 가스는 N doping source로 사용되었으며, 전체 가스 유량에 대한 $N_2O$ 가스의 비율 $N_2O/(N_2O+Ar)$과 증착 전력을 증착의 주요 공정 변수로 선택하여 다양한 가스 비율과 증착 전력에 대한 박막의 미세 구조 특성을 비교 분석하였다. 특히, Auger electron spectroscopy (AES)를 이용하여 ZnO 박막 내에 들어가 존재하는 불순물 N의 수직분포를 분석하였고, 여러 가지 증착 조건에서 제작된 ZnO 박막의 표면형상 및 미세구조 특성을 Scanning Electron Microscope (SEM)를 이용하여 분석하였다.

전기방사를 이용한 Al이 첨가된 ZnO 나노섬유의 제조 및 광학 특성평가 (Optical properties of Al doped ZnO Nanofibers Prepared by electrospinning)

  • 송찬근;윤종원
    • 한국결정성장학회지
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    • 제21권5호
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    • pp.205-209
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    • 2011
  • ZnO는 반도전성과 초전도성을 나타내며 광학적으로도 독특한 재료로 가스센서, 태양전지, 광학도파관 등 여러 방면에 널리 활용되고 있다. 본 논문에서는 이러한 ZnO에 Al을 첨가함에 따라 광학적 특성에 어떠한 영향을 미치는지 알아보기 위하여 ZnO에 Al 첨가량 변화에 따른 나노구조체를 제작하여 특성을 비교하였다. ZnO 용액은 PVP, ethanol, zinc acetate를 이용하여 Sol의 형태로 제작하였으며, Al첨가용액을 넣어 Al이 첨가된 ZnO Sol을 제작하였다. 제작된 Sol을 전기 방사법을 이용하여 나노구조체를 제조하였다. 제조된 섬유들을 각각 300, 500, $700^{\circ}C$로 열처리 한 후 나노 구조체를 XRD, XPS, SEM을 이용하여 분석하였다. 또한 TGA, DSC를 이용하여 온도변화에 따른 질량 및 열량의 변화를 측정하였다. UVvis를 이용하여 ZnO와 Al이 첨가된 ZnO의 흡광도를 측정 비교하였다.

Luminescence Properties of $Dy^{3+}-(or Tm^{3+}-)$ Doped $Ga_2O_3$ and $ZnGa_2O_4$ Phosphors

  • Ryu, Ho-Jin;Park, Hee-Dong
    • The Korean Journal of Ceramics
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    • 제3권2호
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    • pp.134-138
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    • 1997
  • $Dy^{3+}-(or Tm^{3+}-)$ doped $Ga_2O_3 \;and\; ZnGa_2O_4$ phosphors were prepared using the solid state reaction method to investigate their photoluminescent characteristics. Under 254 nm excitation, $Dy^{3+}-doped Ga2_O_3$ exhibited two emission bands of 460~505nm and 570~600nm. On the other hand, $Dy^{3+}-(or Tm^{3+}-)$ doped $ZnGa_2O_4 $phosphors exhibited a broad-band emission extending from 330 nm to 610 nm, peaking at about 430 nm(or 370 nm). In this study, an emission peak shift of nealy 50 nm towards longer wavelength region was observed with $Dy^{3+}$ doping in the $ZnGa_2O_4 $.

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Sol-gel 법으로 제작한 Ga-doped ZnO 박막의 도핑 농도와 열처리 온도가 전기적 및 광학적 특성에 미치는 효과 (Effects of Doping Concentrations and Annealing Temperatures on the Electrical and Optical Properties of Ga-doped ZnO Thin Films by Sol-gel Method)

  • 강성준;정양희
    • 한국정보통신학회논문지
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    • 제16권3호
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    • pp.558-564
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    • 2012
  • Sol-gel 법으로 Eagle 2000 유리 기판 위에 Ga 도핑 농도와 열처리 온도에 따른 GZO 박막을 제작하여, 전기적 및 광학적 특성을 조사하였다. 1 mol% Ga 이 도핑되고 $600^{\circ}C$에서 열처리한 GZO 박막에서 가장 우수한 (002) 배향성이 관찰되었다. Hall 측정 결과, Ga 도핑 농도가 증가함에 따라 segregation 효과로 인한 캐리어 농도의 감소와 비저항 값의 증가가 관찰되었다. 1 mol% Ga 이 도핑되고 $600^{\circ}C$에서 열처리한 GZO 박막에서 가장 큰 캐리어 농도($9.13{\times}10^{18}cm^{-3}$)와 가장 낮은 비저항 ($0.87{\Omega}cm$) 값을 나타내었다. 모든 박막은 가시광 영역에서 약 80 % 이상의 투과율을 보였으며, Ga 농도가 1 에서 4 mol% 로 증가함에 따라 에너지 밴드 갭이 좁아지는 Burstein-Moss 효과가 관찰되었다.

Cu 도핑된 ZnO 박막의 물성 및 SAW 소자 응용 (Characterization of Cu-doped ZnO thin film and its application of SAW devices)

  • 이진복;이혜정;신완철;서수형;박진석
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2000년도 하계학술대회 논문집 C
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    • pp.1488-1490
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    • 2000
  • ZnO:Cu thin films are deposited by using an RF magnetron co-sputtering system with Cu chips attached on ZnO target. Structural and electrical properties are analyzed as a function of deposition conditions, such as Cu chip areas, $O_2/(Ar+O_2)$ ratios, and working pressures, The results show that a higher electrical resistivity above $10^{10}$ ${\Omega}cm$ along with an excellent c-axial growth can be easily achieved by Cu-doping. SAW filters based on the ZnO:Cu films are also fabricated to estimate the electric-mechanical coupling coefficient($K^{2}_{eff}$). Higher $K^{2}_{eff}$ and lower insertion losses are observed for ZnO:Cu films, compared with those for ZnO films.

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Intermediate band solar cells with ZnTe:Cr thin films grown on p-Si substrate by pulsed laser deposition

  • Lee, Kyoung Su;Oh, Gyujin;Kim, Eun Kyu
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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    • pp.247.1-247.1
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    • 2016
  • Low-cost, high efficiency solar cells are tremendous interests for the realization of a renewable and clean energy source. ZnTe based solar cells have a possibility of high efficiency with formation of an intermediated energy band structure by impurity doping. In this work, ZnO/ZnTe:Cr and ZnO/i-ZnTe structures were fabricated by pulsed laser deposition (PLD) technique. A pulsed (10 Hz) Nd:YAG laser operating at a wavelength of 266 nm was used to produce a plasma plume from an ablated a ZnTe target, whose density of laser energy was 10 J/cm2. The base pressure of the chamber was kept at approximately $4{\times}10-7Torr$. ZnTe:Cr and i-ZnTe thin films with thickness of 210 nm were grown on p-Si substrate, respectively, and then ZnO thin films with thickness of 150 nm were grown on ZnTe:Cr layer under oxygen partial pressure of 3 mTorr. Growth temperature of all the films was set to $250^{\circ}C$. For fabricating ZnO/i-ZnTe and ZnO/ZnTe:Cr solar cells, indium metal and Ti/Au grid patterns were deposited on back and front side of the solar cells by using thermal evaporator, respectively. From the fabricated ZnO/ZnTe:Cr and ZnO/i-ZnTe solar cell, dark currents were measured by using Keithley 2600. Solar cell parameters were obtained under Air Mass 1.5 Global solar simulator with an irradiation intensity of 100 mW/cm2, and then the photoelectric conversion efficiency values of ZnO/ZnTe:Cr and ZnO/i-ZnTe solar cells were measured at 1.5 % and 0.3 %, respectively.

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Hetero-epitaxial ZnO 버퍼층이 As-doped ZnO 박막의 증착조건에 미치는 영향 (Effect of the hetero-epitaxial ZnO buffer layer for the formation of As-doped ZnO thin films)

  • 이홍찬;최원국;심광보;오영제
    • 센서학회지
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    • 제15권3호
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    • pp.216-221
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    • 2006
  • ZnO thin films prepared by PLD method exhibit an excellent optical property, but may have some problems such as incomplete surface roughness and crystallinity. In this study, undoped ZnO buffer layers were deposited on (0001) sapphire substrates by ultra high vacuum pulse laser deposition (UHV-PLD) and molecular beam epitaxy (MBE) methods, respectively. After post annealing of ZnO buffer layer, undoped ZnO thin films were deposited under different oxygen pressure ($35{\sim}350$ mtorr) conditions. The Arsenic-doped (1, 3 wt%) ZnO thin layers were deposited on the buffer layer of undoped ZnO by UHV-PLD method. The optical property of the ZnO thin films was analyzed by photoluminescence (PL) measurement. The ${\theta}-2{\theta}$ XRD analysis exhibited a strong (002)-peak, which indicates c-axis preferred orientation. Field emission-scanning electron microscope (FE-SEM) revealed that microstructures of the ZnO thin films were varied by oxygen partial pressure, Arsenic doping concentration, and deposition method of the undoped ZnO buffer layer. The denser and smoother films were obtained when employing MBE-buffer layer under lower oxygen partial pressure. It was also found that higher Arsenic concentration gave the enhanced growing of columnar structure of the ZnO thin films.

Codoped ZnO films by a co-spray deposition technique for photovoltaic applications

  • Zhou, Bin;Han, Xiaofei;Tao, Meng
    • Advances in Energy Research
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    • 제2권2호
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    • pp.97-104
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    • 2014
  • A co-spray deposition technique has been developed to bypass a fundamental limitation in the conventional spray deposition technique, i.e., the deposition of metal oxides from incompatible precursors in the starting solution. With this technique, ZnO films codoped with F and Al have been successfully synthesized, in which F is incompatible with Al. Two starting solutions were prepared and co-sprayed through two separate spray heads. One solution contained only the F precursor, $NH_4F$. The second solution contained the Zn and Al precursors, $Zn(O_2CCH_3)_2$ and $AlCl_3$. The deposition was carried out at $500^{\circ}C$ on soda-lime glass in air. A minimum sheet resistance, $55.4{\Omega}/{\square}$, was obtained for Al and F codoped ZnO films after vacuum annealing at $400^{\circ}C$, which was lower than singly-doped ZnO with either Al or F. The transmittance for the codoped ZnO samples was above 90% in the visible range. This co-spray deposition technique provides a simple and cost-effective way to synthesize metal oxides from incompatible precursors with improved properties for photovoltaic applications.

Self-textured Al-doped ZnO transparent conducting oxide for p-i-n a-Si:H thin film solar cell

  • 김도영;이준신;김형준
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2009년도 추계학술발표대회
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    • pp.50.1-50.1
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    • 2009
  • Transparent conductive oxides (TCOs) play an important role in thin-film solar cells in terms of low cost and performance improvement. Al-doped ZnO (AZO) is a very promising material for thin-film solar cellfabrication because of the wide availability of its constituent raw materials and its low cost. In this study, AZO films were prepared by low pressurechemical vapor deposition (LPCVD) using trimethylaluminum (TMA), diethylzinc(DEZ), and water vapor. In order to improve the absorbance of light, atypical surface texturing method is wet etching of front electrode using chemical solution. Alternatively, LPCVD can create a rough surface during deposition. This "self-texturing" is a very useful technique, which can eliminate additional chemical texturing process. The introduction of a TMA doping source has a strong influence on resistivity and the diffusion of light in a wide wavelength range.The haze factor of AZO up to a value of 43 % at 600 nm was achieved without an additional surface texturing process by simple TMA doping. The use of AZO TCO resulted in energy conversion efficiencies of 7.7 % when it was applied to thep-i-n a-Si:H thin film solar cell, which was comparable to commercially available fluorine doped tin oxide ($SnO_2$:F).

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