• Title/Summary/Keyword: doped ZnS

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Influence of post-annealing temperature on double layer ZTO/GZO deposited by magnetron co-sputtering

  • Oh, Sung Hoon;Cho, Sang Hyun;Jung, Jae Heon;Kang, Sae Won;Cheong, Woo Seok;Lee, Gun Hwan;Song, Pung Keun
    • Journal of Ceramic Processing Research
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    • v.13 no.spc1
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    • pp.140-144
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    • 2012
  • Ga-doped ZnO (GZO) was a limit of application on the photovoltaic devices such as CIGS, CdTe and DSSC requiring high process temperature, because it's electrical resistivity is unstable above 300 ℃ at atmosphere. Therefore, ZTO (zinc tin oxide) was introduced in order to improve permeability and thermal stability of GZO film. The resistivity of GZO (300 nm) single layer increased remarkably from 1.8 × 10-3Ωcm to 5.5 × 10-1Ωcm, when GZO was post-annealed at 400 ℃ in air atmosphere. In the case of the ZTO (150 nm)/GZO (150 nm) double layer, resistivity showed relatively small change from 3.1 × 10-3Ωcm (RT) to 1.2 × 10-2Ωcm (400 ℃), which showed good agreement with change of carrier density. This result means that ZTO upper layer act as a barrier for oxygen at high temperature. Also ZTO (150 nm)/GZO (150 nm) double layer showed lower WVTR compared to GZO (300 nm) single layer. Because ZTO has lower WVTR compared to GZO, ZTO thin film acts as a barrier by preventing oxygen and water molecules to penetrate on top of GZO thin film.

Electrical and Optical Properties of the GZO Transparent Conducting Layer Prepared by Magnetron Sputtering Technique (마그네트론 스퍼터링법으로 제작된 GZO 투명전도막의 전기적 및 광학적 특성)

  • No, Im-Jun;Kim, Sung-Hyun;Shin, Paik-Kyun;Lee, Kyung-Il;Kim, Sun-Min;Cho, Jin-Woo
    • Journal of the Korean Institute of Illuminating and Electrical Installation Engineers
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    • v.24 no.4
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    • pp.110-115
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    • 2010
  • Transparent conducting gallium-doped zinc oxide (GZO) thin films which were deposited on Corning glass substrate using an Gun-type rf magnetron sputtering deposition technology. The GZO thin films were fabricated with an GZO ceramic target (Zn : 97[wt%], $Ga_2O_3$ : 3[wt%]). The GZO thin films were deposited by varying the growth conditions such as the substrate temperature, oxygen pressure. Among the GZO thin films fabricated in this study, the one formed at conditions of the substrate temperature of 200[$^{\circ}C$], Ar flow rate of 50[sccm], $O_2$ flow rate of 5[sccm], rf power of 80[W] and working pressure of 5[mtorr] showed the best properties of an electrical resistivity of $2.536{\times}10^{-4}[{\Omega}{\cdot}cm]$, a carrier concentration of $7.746{\times}10^{20}[cm^{-3}]$, and a carrier mobility of 31.77[$cm^2/V{\cdot}S$], which indicates that it could be used as a transparent electrode for thin film transistor and flat panel display applications.

Fabrication of P-type Transparent Oxide Semiconductor SrCu2O2 Thin Films by RF Magnetron Sputtering (RF 마그네트론 스퍼터링을 이용한 p 타입 투명전도 산화물 SrCu2O2 박막의 제조)

  • Seok, Hye-Won;Kim, Sei-Ki;Lee, Hyun-Seok;Lim, Tae-Young;Hwang, Jong-Hee;Choi, Duck-Kyun
    • Korean Journal of Materials Research
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    • v.20 no.12
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    • pp.676-680
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    • 2010
  • Most TCOs such as ITO, AZO(Al-doped ZnO), FTO(F-doped $SnO_2$) etc., which have been widely used in LCD, touch panel, solar cell, and organic LEDs etc. as transparent electrode material reveal n-type conductivity. But in order to realize transparent circuit, transparent p-n junction, and introduction of transparent p-type materials are prerequisite. Additional prerequisite condition is optical transparency in visible spectral region. Oxide based materials usually have a wide optical bandgap more than ~3.0 eV. In this study, single-phase transparent semiconductor of $SrCu_2O_2$, which shows p-type conductivity, have been synthesized by 2-step solid state reaction at $950^{\circ}C$ under $N_2$ atmosphere, and single-phase $SrCu_2O_2$ thin films of p-type TCOs have been deposited by RF magnetron sputtering on alkali-free glass substrate from single-phase target at $500^{\circ}C$, 1% $H_2$/(Ar + $H_2$) atmosphere. 3% $H_2$/(Ar + $H_2$) resulted in formation of second phases. Hall measurements confirmed the p-type nature of the fabricated $SrCu_2O_2$ thin films. The electrical conductivity, mobility of carrier and carrier density $5.27{\times}10^{-2}S/cm$, $2.2cm^2$/Vs, $1.53{\times}10^{17}/cm^3$ a room temperature, respectively. Transmittance and optical band-gap of the $SrCu_2O_2$ thin films revealed 62% at 550 nm and 3.28 eV. The electrical and optical properties of the obtained $SrCu_2O_2$ thin films deposited by RF magnetron sputtering were compared with those deposited by PLD and e-beam.

비진공법을 이용한 CIGS광흡수층의 합성과 특성평가

  • Gwon, Yeong-Eun;Park, Jun-Tae;Im, Gi-Hong;Choe, Hyeon-Gwang;Jeon, Min-Hyeon
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.312.1-312.1
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    • 2014
  • Chalcopyrite계 화합물 반도체인 $Cu(InGa)Se_2$ (CIGS)는 직접천이형 에너지 밴드갭과 전파장 영역에 대하여 높은 광흡수계수($1{\times}$[10]^5/cm)를 가지므로 두께 $1{\sim}2{\mu}m$인 박막형태으로 고효율의 태양전지 제조가 가능하다. 또한, 박막공정의 저가 가능성을 나타내면서 전세계적으로 많은 연구와 관심을 받고 있고, 현재 상용화되어 있는 결정질실리콘 태양전지를 대체할만한 재료로 주목 받고 있다. 일반적으로, CIGS박막형 태양전지 구성은는 유리를 기판으로 하여 5개의 단위 박막인 Mo 후면전극, p형 반도체 CIGS 광흡수층, n형 반도체 CdS 버퍼층, doped-ZnO 상부 투명전극, $MgF_2$ 반사방지막으로 이루어진다. 이들 중에서 태양전지의 에너지 변환효율에 결정적인 영향을 미치는 구성된다. CIGS 광흡수층의 제조는 크게 진공법과 비진공방법으로 나뉜다. 현재까지 보고된 문헌에 따르면 CIGS 박막형 태양전지의 경우에 동시증발법으로 20.3%의 에너지 변환효율을 보였지만,는데, 이는 진공장비 특성상 공정단가가 높고 대면적화가 어렵다는 단점을 가진다. 따라서, 비진공법을 이용하여 광흡수층 제작하는 것이 기술적으로 진보할 여지가 크다고 볼 수 있다. 반면 현재 상용화되어 있는 결정질실리콘 태양전지를 대체할만한 방법으로 주목 받고 있는 비진공을 이용한 저가공정은 최근 15.5%의 에너지 변환효율이 보고 되었다. 비진공법에는 전계를 이용한 증착법 및 스프레이법으로 나뉘며, 이들 광흡수층 재료의 화학적 합성은 III족 원소인 In, Ga의 함량비에 따라 광흡수층의 에너지 밴드갭(1.04~1.5 eV) 조절이 가능하다. 따라서, 본 연구에서는 비진공법에 사용되는 CIGS재료의 화학적 합성조건을 변화시켜 III족 원소의 조성비 조절을 시도하였다. CIGS 분말 시료의 입자 형태와 크기를 FE-SEM을 이용하여 관찰하였고, 화합물의 성분비를 EDX 및 XRD 분석을 통해 Ga 함량에 따른 구조적 차이를 비교해 보았다.

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Influence of Post-deposition Annealing Temperature on the Properties of GZO/Al Thin Film (진공열처리 온도에 따른 GZO/Al 적층박막의 구조적, 전기적, 광학적 특성 변화)

  • Kim, Sun-Kyung;Kim, Seung-Hong;Kim, So-Young;Jeon, Jae-Hyun;Gong, Tae-Kyung;Yoon, DaeYoung;Choi, DongYong;Choi, Dong-Hyuk;Son, Dong-Il;Kim, Daeil
    • Journal of the Korean institute of surface engineering
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    • v.47 no.2
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    • pp.81-85
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    • 2014
  • Ga doped ZnO (GZO)/Al bi-layered films were deposited on the glass substrate by RF and DC magnetron sputtering and then vacuum annealed at different temperatures of 100, 200 and $300^{\circ}C$ for 30 minutes to consider the effects of annealing temperature on the structural, electrical and optical properties of the films. For all depositions, the thicknesses of the GZO and Al films were kept constant at 95 and 5 nm, respectively, by controlling the deposition time. As-deposited GZO/Al bi-layered films showed a relatively low optical transmittance of 62%, while the films annealed at $300^{\circ}C$ showed a higher transmittance of 81%, compared to the other films. In addition, the electrical resistivity of the films was influenced by annealing temperature and the lowest resistivity of $9.8{\times}10^{-4}{\Omega}cm$ was observed in the films annealed at $300^{\circ}C$. Due to the increased carrier mobility, 2.35 $cm^2V^{-1}S^{-1}$ of the films. From the experimental results, it can be concluded that increasing the annealing temperature enhanced the optical and electrical properties of the GZO/Al films.

Effect of the Concentration of Oxygen Vacancies on the Structural and Electrical Characteristics of MZO Thin Films (산소공공 농도에 따른 MZO 투명전도성 박막의 구조적 및 전기적 특성)

  • Jong Hyun Lee;Kyu Mann Lee
    • Journal of the Semiconductor & Display Technology
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    • v.22 no.1
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    • pp.18-22
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    • 2023
  • We have investigated the effect of the concentration of oxygen vacancies on the characteristics of Mo-doped ZnO (MZO) thin films for the TCO (transparent conducting oxide). For this purpose, MZO thin films were deposited by RF magnetron sputtering at different substrate temperature from room temperature to 300℃. The electrical resistivity of the MZO films decreases with increasing substrate temperature up to 100℃ and then gradually increases at higher temperatures. To investigate the influences of the ambient gases, the flow rate of oxygen and hydrogen in argon was varied from 0.1 sccm to 0.5 sccm. The MZO thin films were preferentially oriented to the (002) direction, regardless of the ambient gases used. The electrical resistivity of the MZO thin films increased with increasing O2 flow rates, whereas the electrical resistivity decreased sharply under an Ar+H2 atmosphere and was nearly the same, regardless of the H2 flow rate used. As the oxygen vacancy concentration increases, the resistivity intended to decrease. In conclusion, Oxygen vacancy affects the MZO thin film's electrical characteristics. All the films showed an average transmittance of over 80% in the visible range.

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