• Title/Summary/Keyword: Semiconductor doped glass

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Double Texturing of Glass Substrate and ZnO : Al Transparent Electrode Surfaces for High Performance Thin Film Solar Cells (고성능 박막태양전지를 위한 유리 기판 및 산화 아연 투명 전극의 2중 구조 표면 조직화 공정 연구)

  • Kang, Dong-Won
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.66 no.8
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    • pp.1230-1235
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    • 2017
  • We studied surface texture-etching of glass substrate by using reactive ion etching process with various working pressure (0.7~9.0 mT). With the increase in the pressure, a haze parameter, which means diffusive transmittance/total transmittance, was increased in overall wavelength regions, as measured by spectrophotometer. Also, atomic force microscopy (AFM) study also showed that the surface topography transformed from V-shaped, keen surface to U-shaped, flattened surface, which is beneficial for nanocrystalline silicon semiconductor growth with suppressing defective crack formation. The texture-etched ZnO:Al combined with textured glass exhibited pronounced haze properties that showed 60~90 % in overall spectral wavelength regions. This promising optical properties of double textured, transparent conducting substrate can be widely applied in silicon thin film photovoltaics and other optoelectronic devices.

Single Crystal Growth and Magnetic Properties of Mn-doped Bi2Se3 and Sb2Se3

  • Choi, Jeong-Yong;Lee, Hee-Woong;Kim, Bong-Seo;Choi, Sung-Youl;Choi, Ji-Youn;Cho, Sung-Lae
    • Journal of Magnetics
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    • v.9 no.4
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    • pp.125-127
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    • 2004
  • We have grown Mn-doped $Bi_2Se_3$ and $Sb_2Se_3$ single crystals using the temperature gradient solidification method. We report on the structural and magnetic propertis of Mn-doped $Bi_2Se_3$ and $Sb_2Se_3$ compound semi-conductors. The lattice constants of several percent Mn-doped $Bi_2Se_3$ and $Sb_2Se_3$ were slightly smaller than those of the un-doped samples due to the smaller Mn atomic radius ($1.40 {\AA}$) than those of Bi ($1.60 {\AA}$) and Sb ($1.45 {\AA}$). Mn-doped $Bi_2Se_3$ and $Sb_2Se_3$ showed spin glass and paramagnetic properties, respectively.

Fabrication of oxide semiconductor thin film gas sensor array (산화물 반도체 박막 가스센서 어레이의 제조)

  • 이규정;김석환;허창우
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.4 no.3
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    • pp.705-711
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    • 2000
  • A thin film oxide semiconductor micro gas sensor array which shows only 60 mW of power consumption at an operating temperature of $300^{\circ}C$ has been fabricated using microfabrication and micromachining techniques. Excellent thermal insulation of the membrane is achieved by the use of a double-layer structure of $0.1\mum\; thick\; Si_3N_4 \;and\; 1 \mum$ thick phosphosilicate glass (PSG) prepared by low-pressure chemical-vapor deposition (LPCVD) and atmospheric-pressure chemical-vapor deposition (APCVD), respectively. The sensor array consists of such thin film oxide semiconductor sensing materials as 1 wt.% Pd-doped $SnO_2,\; 6 wt.% A1_2O_3-doped\; ZnO,\; WO_3$/ and ZnO. Baseline resistances of the four sensing materials were found to be stable after the aging for three days at $300^{\circ}C$. The thin film oxide semiconductor micro gas sensor array exhibited resistance changes usable for subsequent data processing upon exposure to various gases and the sensitivity strongly depended on the sensing layer materials.

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Fabrication and yield improvement of oxide semiconductor thin film gas sensor array (산화물 반도체 박막 가스센서 어레이의 제조 및 수율 개선)

  • 이규정;류광렬;허창우
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.6 no.2
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    • pp.315-322
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    • 2002
  • A thin film oxide semiconductor micro gas sensor array which shows only 60㎽ of power consumption at an operating temperature of 30$0^{\circ}C$ has been fabricated using microfabrication and rnicrornachining techniques. Excellent thermal insulation of the membrane is achieved by the use of a double la! or structure of 0.1${\mu}{\textrm}{m}$ thick Si$_3$N$_4$ and 1${\mu}{\textrm}{m}$ thick phosphosilicate glass(PSG) prepared by low pressure chemical vapor deposition(LPCVD) and atmospheric-pressure chemical-vapor deposition(APCVD), respectively. The sensor way consists of such thin film oxide semiconductor sensing materials as 1wt.% Pd-doped SnO$_2$, 6wt.% AI$_2$O$_3$-doped ZnO, WO$_3$ and ZnO. The thin film oxide semiconductor micro gas sensor array exhibited resistance changes usable for subsequent data processing upon exposure to various gases and the sensitivity strongly depended on the sensing layer materials. Heater Part of the sensor structure has been modified in order to improve the process yield of the sensor, and as a result of modified heater structure improved process yield has been achieved.

Sputtered ZTO as a blocking layer at conducting glass and $TiO_2$ Interfaces in Dye-Sensitized Solar Cells (GZO/ZTO 투명전극을 이용한 DSSC의 광전 변환 효율 특성)

  • Park, Jaeho;Lee, Kyungju;Song, Sangwoo;Jo, Seulki;Moon, Byungmoo
    • 한국신재생에너지학회:학술대회논문집
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    • 2011.11a
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    • pp.53.2-53.2
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    • 2011
  • Dye-sensitized solar cells(DSSCs) have been recognized as an alternative to the conventional p-n junction solar cells because of their simple fabrication process, low production cost, and transparency. A typical DSSC consists of a transparent conductive oxide (TCO) electrode, a dye-sensitized oxide semiconductor nanoparticle layer, liquid redox electrolyte, and a Pt-counter electrode. In dye-sensitized solar cells, charge recombination processes at interfaces between coducting glass, $TiO_2$, dye, and electrolyte play an important role in limiting the photon-to-electron conversion efficiency. A layer of ZTO thin film less than ~200nm in thickness, as a blocking layer, was deposited by DC magnetron sputtering method directly onto the anode electrode to be isolated from the electrolyte in dye-sensitized solar cells(DSCs). This is to prevent the electrons from back-transferring from the electrode to the electrolyte ($I^-/I_3^-$). The presented DSCs were fabricated with working electrode of Ga-doped ZnO glass coated with blocking ZTO layer, dye-attached nanoporous $TiO_2$ layer, gel electrolyte and counter electrode of Pt-deposited GZO glass. The effects of blocking layer were studied with respect to impedance and conversion efficiency of the cells.

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Characterization of Al Doped ZnO Thin Films Prepared by RF Magnetron Sputtering Under Various Substrate Temperatures

  • Kim, Deok Kyu;Kim, Hong Bae
    • Applied Science and Convergence Technology
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    • v.23 no.5
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    • pp.279-283
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    • 2014
  • Al doped ZnO thin films have been deposited by a RF magnetron sputtering technique from a ZnO (2 wt.% $Al_2O_3$) target onto glass substrates heated at temperature ranging from RT to $400^{\circ}C$. X-ray diffraction analysis shows that the deposits have a preferential growth along the c-axis of a hexagonal structure. The full with at half maximum decreases from 0.45 to $0.43^{\circ}$ in the studied temperature range. The root main square surface roughness increases with substrate temperature from 1.89 to 2.67 nm. All films are transparent up to 80% in the visible wavelength range and the adsorption edge is red-shifted with substrate temperature from RT to $400^{\circ}C$. The sheet resistance increases from 92 ohm/sq to 419 ohm/sq when the deposition temperature increases from RT to $400^{\circ}C$. The increment of sheet resistance is caused by lowered carrier concentration resulting from an increase in surface roughness.

Effects of Different Dopants(B, AI, Ga, In) on the Properties of Transparent conducting ZnO Thin Films (B, Al, Ga, In의 도핑물질이 투명 전도성 ZnO 박막의 특성에 미치는 영향)

  • No, Young-Woo;Cho, Jong-Rae;Son, Se-Mo;Chung, Su-Tae
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.21 no.3
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    • pp.242-248
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    • 2008
  • The structural, optical and electrical properties of ZnO films doped with 1.5 at% of 3A materials(B, Al, Ga, In) were studied by sol-gel process. The films were found to be c-axis (002) oriented hexagonal structure on glass substrate, when post heated at 500 $^{\circ}C$. The surface of the films showed a uniform and nano size microstructure and the crystalline size of doped films decreased. The lattice constants of ZnO:B/Al/Ga increased than that of ZnO, while ZnO:In decreased. All the films were highly transparent(above 90 %) in the visible region. The energy gaps of ZnO:B/Al/Ga were increased a little, but that of ZnO:In was not changed. The resistivities of ZnO:Al/Ga/In were less than 0.1 $\Omega$cm. All the films showed a semiconductor properties in the light or temperature, however ZnO:In was less sensitive to it. A figure of merit of ZnO:In had the highest value of 0.025 $\Omega^{-1}$ in all samples.

Electrical and Optical Properties of Ga-doped SnO2 Thin Films Via Pulsed Laser Deposition

  • Sung, Chang-Hoon;Kim, Geun-Woo;Seo, Yong-Jun;Heo, Si-Nae;Huh, Seok-Hwan;Chang, Ji-Ho;Koo, Bon-Heun
    • Journal of the Korean institute of surface engineering
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    • v.44 no.4
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    • pp.144-148
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    • 2011
  • $Ga_2O_3$ doped $SnO_2$ thin films were grown by using pulsed laser deposition (PLD) technique on glass substrate. The optical and electrical properties of these films were investigated for different doping concentrations, oxygen partial pressures, substrate temperatures, and film thickness. The films were deposited at different substrate temperatures (room temperature to $600^{\circ}C$). The best opto-electrical properties is shown by the film deposited at substrate temperature of $300^{\circ}C$ with oxygen partial pressure of 80 m Torr and the gallium concentration of 2 wt%. The as obtained lowest resistivity is $9.57{\times}10^{-3}\;{\Omega}cm$ with the average transmission of 80% in the visible region and an optical band gap (indirect allowed) of 4.26 eV.

Structural, Optical, and Electrical Properties of IGZO Thin Film Sputtered with Various RF Powers (RF 파워 변화에 따른 IGZO 박막의 구조적, 광학적, 전기적 특성)

  • Jin, Chang-Hyun;Kim, Hong-Bae
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.28 no.10
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    • pp.620-624
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    • 2015
  • We have studied structural, optical and electrical properties of In-Ga-doped ZnO (IGZO) thin films. The IGZO thin films were deposited on the corning 1737 glass by RF magnetron sputtering method. The RF power in sputtering process was varied as 30, 50, 70, and 90 W respectively. All of the IGZO thin films transmittance in the visible range (400 nm ~ 800 nm) was above 83%. XRD analysis showed the IGZO thin films amorphous structure of the thin films without any peak. And also IGZO thin film have low resistivity ($1.99{\times}10^{-3}{\Omega}cm$), high carrier concentration ($6.4{\times}10^{20}cm^{-3}$), and mobility ($10.3cm^2V^{-1}s^{-1}$). By the studies we found that IGZO transparent thin film can be used as optoelectronic material and introduced application possibility for future electronic devices.

Local structure of transparent flexible amorphous M-In-ZnO semiconductor

  • Son, L.S.;Kim, K.R.;Yang, D.S.;Lee, J.C.;Sung, N.;Lee, J.;Kang, H.J.
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.08a
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    • pp.164-164
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    • 2010
  • The impurity doped ZnO has been extensively studied because of its optoelectric properties. GIZO (Ga-In-Zn-O) amorphous oxide semiconductors has been widely used as transparent flexible semiconductor material. Recently, various amorphous transparent semiconductors such as IZO (In-Zn-O), GIZO, and HIZO (Hf-In-Zn-O) were developed. In this work, we examined the local structures of IZO, GIZO, and HIZO. The local coordination structure was investigated by the extended X-ray absorption fine structure. The IZO, GIZO and HIZO thin films ware deposited on the glass substrate with thickness of 400nm by the radio frequency sputtering method. The targets were prepared by the mixture of $In_2O_3$, ZnO and $HfO_2$ powders. The percent ratio of In:Zn in IZO, Ga:In:Zn in GIZO and Hf:In:Zn in HIZO was 45:55, 33:33:33 and 10:35:55, respectively. In this work, we found that IZO, GIZO and HIZO are all amorphous and have a similar local structure. Also, we obtained the bond distances of $d_{Ga-O}=1.85\;{\AA}$, $d_{Zn-O}=1.98\;{\AA}$, $d_{Hf-O}=2.08\;{\AA}$, $d_{In-O}=2.13\;{\AA}$.

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