• Title/Summary/Keyword: Sn doping

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The Application and Electrical, Optical Properties of $In_2O_3$: Sn Transparent Conducting Films (ITO투명도전막의 전기, 광학적 특성 및 그 응용)

  • Lee, Dong Hoon;Park, Ki Cheol;Park, Chang Bae;Kim, Ki Wan
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.23 no.4
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    • pp.498-505
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    • 1986
  • In2O3: Sn(ITO) transparent conducting films were fabricated by the electron beam evaporation method. The dependence of their electrical and optical properties on deposition conditions were examined. The optimum evaporation conditions were such that the deposition rate was 5-10\ulcornersec, oxygen partial pressure was 4x10**_4 torr, substate temperatudre was above 300\ulcorner, and SnO2 doping rate was 10 mol%. The values of sheet resistance and transmittance of the films in visible region fabricated under these optimum conditins were 12\ulcorner/ and 87-99%, respecively. And the energy conversion efficiency of the SIS solar cell fabricated using ITO was 9.16%. It is shown that the transparent conducting films can be applied to the TV camear pick-up tube and solar cell.

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Synthesis of Ni-rich NCMA Precursor through Co-precipitation and Improvement of Cycling through Boron and Sn Doping (공침법을 통한 Ni-rich NCMA 합성과 붕소와 주석 도핑을 통한 사이클 특성 향상)

  • Jeon, Hyungkwon;Hong, Soonhyun;Kim, Minjeong;Koo, Jahun;Lee, Heesang;Choi, Gyuseok;Kim, Chunjoong
    • Korean Journal of Materials Research
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    • v.32 no.4
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    • pp.210-215
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    • 2022
  • Extensive research is being carried out on Ni-rich Li(NixCoyMn1-x-y)O2 (NCM) due to the growing demand for electric vehicles and reduced cost. In particular, Ni-rich Li(NixCoyMn1-x-y-zAlz)O2 (NCMA) is attracting great attention as a promising candidate for the rapid development of Co-free but electrochemically more stable cathodes. Al, an inactive element in the structure, helps to improve structural stability and is also used as a doping element to improve cycle capability in Ni-rich NCM. In this study, NCMA was successfully synthesized with the desired composition by direct coprecipitation. Boron and tin were also used as dopants to improve the battery performance. Macro- and microstructures in the cathodes were examined by microscopy and X-ray diffraction. While Sn was not successfully doped into NCMA, boron could be doped into NCMA, leading to changes in its physicochemical properties. NCMA doped with boron revealed substantially improved electrochemical properties in terms of capacity retention and rate capability compared to the undoped NCMA.

Electrical and Optical Properties of Sb-doped SnO2 Thin Films Fabricated by Pulsed Laser Deposition (펄스레이저 공정으로 제조한 Sb가 도핑된 SnO2 박막의 전기적 및 광학적 특성)

  • Jang, Ki-Sun;Lee, Jung-Woo;Kim, Joongwon;Yoo, Sang-Im
    • Journal of the Korean Ceramic Society
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    • v.51 no.1
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    • pp.43-50
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    • 2014
  • We fabricated undoped and Sb-doped $SnO_2$ thin films on glass substrates by a pulsed laser deposition (PLD) process. Undoped and 2 - 8 wt% $Sb_2O_3$-doped $SnO_2$ targets with a high density level of ~90% were prepared by the spark plasma sintering (SPS) process. Initially, the effects of the deposition temperature on undoped $SnO_2$ thin films were investigated in the region of $100-600^{\circ}C$. While the undoped $SnO_2$ film exhibited the lowest resistivity of $1.20{\times}10^{-2}{\Omega}{\cdot}cm$ at $200^{\circ}C$ due to the highest carrier concentration generated by the oxygen vacancies, 2 wt% Sb-doped $SnO_2$ film exhibited the lowest resistivity value of $5.43{\times}10^{-3}{\Omega}{\cdot}cm$, the highest average transmittance of 85.8%, and the highest figure of merit of 1202 ${\Omega}^{-1}{\cdot}cm^{-1}$ at $400^{\circ}C$ among all of the doped films. These results imply that 2 wt% $Sb_2O_3$ is an optimum doping content close to the solubility limit of $Sb^{5+}$ substitution for the $Sb^{4+}$ sites of $SnO_2$.

Elect of Catalytic Configuration on Sensing Properties of Nano Gas Sensor (나노 가스 감지 소자의 특성에 미치는 촉매 구조의 영향)

  • Hong, Sung-Jei;Isshiki Minoru;Han, Jeong-In
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.18 no.10
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    • pp.917-923
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    • 2005
  • In this paper, effect of catalytic configuration on the sensing properties of $SnO_2$ nanoparticle gas sensitive thick film was investigated. Two types of catalytic configuration, mono and binary, were made on the $SnO_2$ nanoparticle. In case of mono catalytic system, $3 wt\%$ Pd or Pt catalyst was doped onto the $SnO_2$ nanoparticle, respectively. In case of binary catalytic system, Pd and Pt was doped simultaneously with concentration ratio of 1:2 to 2:1 onto the $SnO_2$ nanoparticle. After doping, gas sensitive thick film was printed on alumina substrate and heat-treated at 450 to $600^{\circ}C$. Gas sensing properties was evaluated using 500 to 10,000 ppm $CH_4$ gas. As a result, gas sensitive thick film with binary catalytic system showed unstable phenomena that the gas sensitivity was changed according to aging time. In contrary, the mono catalytic system showed relatively stable phenomena despite of aging time. Especially, gas sensitive thick film doped with $3 wt\%$ Pt catalyst and heat-treated at $500^{\circ}C$ showed good sensing properties such as 0.57 of $R_{3500}/R_{1000}$ and very small variation within $3.5\%$ after aging for 5 hours, and response time was very short less than 20 seconds.

Microstructure Evolution and Dielectric Characteristics of CaCu3Ti4O12 Ceramics with Sn-Substitution

  • Kim, Cheong-Han;Oh, Kyung-Sik;Paek, Yeong-Kyeun
    • Journal of the Korean Ceramic Society
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    • v.50 no.1
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    • pp.87-91
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    • 2013
  • The doping effect of Sn on the microstructure evolution and dielectric properties was studied in $CaCu_3Ti_{4-x}Sn_xO_{12}$ polycrystals. Samples were produced by a conventional solid-state reaction method. Sintering was carried out at $1115^{\circ}C$ for 2-16 h in air. The dielectric constant and loss were examined at room temperature over a frequency range between $10^2$ and $10^6$ Hz. The microstructure was found to evolve into three stages. Addition of $SnO_2$ led to an increase in density and advanced formation of abnormal grains. The formation of coarse grains with a reduced thickness of the boundary brought about an enhanced dielectric constant and a lower dielectric loss below ~1 kHz. EDS data showed the Cu-rich phase along the grain boundary, which should contribute to the improved dielectric constant according to the internal barrier layer capacitor model. After all, $SnO_2$ was an effective dopant to elevate the dielectric characteristics of $CaCu_3Ti_{4-x}Sn_xO_{12}$ polycrystals as a promoter for abnormal grain growth.

A comparative study on the flux pinning properties of Zr-doped YBCO film with those of Sn-doped one prepared by metal-organic deposition

  • Choi, S.M.;Shin, G.M.;Joo, Y.S.;Yoo, S.I.
    • Progress in Superconductivity and Cryogenics
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    • v.15 no.4
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    • pp.15-20
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    • 2013
  • We investigated the flux pinning properties of both 10 mol% Zr-and Sn-doped $YBa_2Cu_3O_{7-{\delta}}$ (YBCO) films with the same thickness of ~350 nm for a comparative purpose. The films were prepared on the $SrTiO_3$ (STO) single crystal substrate by the metal-organic deposition (MOD) process. Compared with Sn-doped YBCO film, Zr-doped one exhibited a significant enhancement in the critical current density ($J_c$) and pinning force density ($F_p$). The anisotropic $J_{c,min}/J_{c,max}$ ratio in the field-angle dependence of $J_c$ at 77 K for 1 T was also improved from 0.23 for Sn-doped YBCO to 0.39 for Zr-doped YBCO. Thus, the highest magnetic $J_c$ values of 9.0 and $2.9MA/cm^2$ with the maximum $F_p$ ($F_{p,max}$) values of 19 and $5GN/m^3$ at 65 and 77 K for H // c, respectively, could be achieved from Zr-doped YBCO film. The stronger pinning effect in Zr-doped YBCO film is attributable to smaller $BaZrO_3$ (BZO) nanoparticles (the average size ${\approx}28.4$ nm) than $YBa_2SnO_{5.5}$ (YBSO) nanoparticles (the average size ${\approx}45.0$ nm) incorporated in Sn-doped YBCO film since smaller nanoparticles can generate more defects acting as effective flux pinning sites due to larger incoherent interfacial area for the same doping concentration.

Doping Effects with $GeO_{2}$ and $SnO_{2}$ in Mn-Zn Ferrites (Mn-Zn 훼라이트의 $GeO_{2}$$SnO_{2}$ 첨가효과)

  • 최용석;유병두;김종오
    • Journal of the Korean Magnetics Society
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    • v.2 no.2
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    • pp.99-104
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    • 1992
  • The permeability vs. temperature curve, the loss factor and the microstructure of a commercial Mn-Zn ferrites were investigated by X-ray diffractometer, SEM and LCR meter, where the additives, such as $SnO_{2}$ and $GeO_{2}$, were added to the main composition. Their wt% were 0.05, 0.3 and 1.0, respectively. When the content of additives increased, the SPM (Secondary Peak Maximum) of the permeability moved from $80^{\circ}C$ to below the room temperature. This movement, without the significant change of the microstructure, is because Sn and Ge, having the different ionic radius, were soluble in the matrix. There was no variation of the permeability with the frequency up to 100 kHz. And the loss factor showed the maximum value at 10 kHz.

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Thermoelectric Properties of $Sn_zCo_3FeSb_{12}$ ($Sn_zCo_3FeSb_{12}$의 열전특성)

  • Lee, Jae-Ki;Yoon, Seok-Yeon;Jung, Jae-Yong;Lee, Jung-Il;Ur, Soon-Chul;Kim, Il-Ho
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.11a
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    • pp.126-127
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    • 2007
  • Sn-filled and Fe-doped $CoSb_3$ skutterudites were synthesized by encapsulated induction melting. Single ${\delta}$-phase was successfully obtained by subsequent annealing and confirmed by X-ray diffraction analysis. Temperature dependences of Seebeck coefficient, electrical resistivity and thermal conductivity were examined from 300 K to 700 K. The positive Seebeck coefficient confirmed the p-type conduction. Electrical resistivity increased with increasing temperature, which shows that the $Sn_zCo_3FeSb_{12}$ skutterudite is highly degenerate. Thermal conductivity was reduced by Sn-filling because the filler atoms acted as phonon scattering centers in the skutterudite lattice. Thermoelectric figure of merit was enhanced by Sn filling and its optimum filling content was considered to be z=0.3 in the $Sn_zCo_3FeSb_{12}$ system.

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Optical properties of $Ag_2CdSnSe_4$ and $Ag_2CdSnSe_4:CO^{2+}$ single crystals ($Ag_2CdSnSe_4$$Ag_2CdSnSe_4:Co^{+2}$단결정의 광학적 특성)

  • 이충일
    • Journal of the Korean Vacuum Society
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    • v.10 no.1
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    • pp.16-21
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    • 2001
  • Optical properties of $Ag_2CdSnSe_4$ and $Ag_2CdSnSe_4:Co^{+2}$ quaternary semiconductor single crystals grown by the chemical transport reaction method were investigated. The analysis of the X - ray powder diffraction measurements showed that these crystals have a wurtzite structure with lattice constants a = 4.357 $\AA$, c = 7.380 $\AA$, for $Ag_2CdSnSe_4$ and a = 4.885 $\AA$, c = 7.374 $\AA$, for $Ag_2CdSnSe_4:CO^{2+}$. The direct band gap at 298K, obtained from the optical absorption measurement, is found to be 1.21 eV for $Ag_2CdSnSe_4$ and 1.02 eV for $Ag_2CdSnSe_4:CO^{2+}$. The shrinkage of the band gap due to Co-doping is observed and is about 190 meV, We observed four absorption bands of $Co^{2+}$ ions in two near infrared regions of optical absorption spectra of $Ag_2CdSnSe_4$:$Co^{+2}$. These absorption bands were assigned as due to electronic transitions between the split energy levels of $Co^{2+}$ ions in $T_d$ crystal field under spin-orbit interactions.

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Effects of Sb doping on the Characteristis of $SnO_2$ Transparent Electrodes ($SnO_2$ 수용전극특성에 미치는 Sb첨가의 영향)

  • 이정한
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.13 no.3
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    • pp.16-21
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    • 1976
  • Transparent eloctroaes of polycrystalline till-oxide films doped with antimony are prepared on the substrate of microscopic cover g1ass by modified spray method and from SnCl4 Solution. Their electrical and optical properties are investigated in relation to the surface temperature of the substrate glass and to antimony concentration in the starting materials. The sheet.resiststrace of the film electrodes and transmittance for incandescent light depen on tile antimony concentration and surface temperature of substrates at the time of making films. The transmittance increases with decrease of sheet resistance of the film. The optimum sheet.resistance was obtianed in the case of the antimony concentration 0.6(%) approximately , and the max. transmittance was 93(%).

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