• Journal of the Korean Vacuum Society
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• v.10 no.1
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• pp.57-60
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• 2001

We prepared uniform CdS nanowire arrays ways with lengths up to 5 $\mu\textrm{m}$ and diameters as small as 20 nm by electrochemically depositing the semiconductor directly into the pores of anodic alumina films from an electrolyte containing $CdCl_2$ and S in dimethyl sulfoxide. The nanowire arrays were characterized by scanning electron microscopy and X-ray diffraction. The deposited materials are composed mainly of hexagonal CdS with (100) preferential orientation.

• Journal of Sensor Science and Technology
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• v.10 no.6
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• pp.328-337
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• 2001

The stochiometric mix of evaporating materials for the $CdGa_2Se_4$ single crystal thin films was prepared from horizontal furnace. To obtain the single crystal thin films, $CdGa_2Se_4$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the Hot Wall Epitaxy (HWE) system. The source and substrate temperature were $630^{\circ}C$ and $420^{\circ}C$, respectively. The crystalline structure of single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of $CdGa_2Se_4$ single crystal thin films measured from Hall effect by van der Pauw method are $8.27{\times}10^{17}cm^{-3}$, $345\;cm^2/V{\cdot}s$ at 293 K, respectively. From the photocurrent spectrum by illumination of perpendicular light on the c-axis of the $CuInSe_2$ single crystal thin film, we have found that the values of spin orbit splitting ${\Delta}So$ and the crystal field splitting ${\Delta}Cr$ were 106.5 meV and 418.9 meV at 10 K, respectively. From the photoluminescence measurement on $CdGa_2Se_4$ single crystal thin film, we observed free excition ($E_x$) existing only high quality crystal and neutral bound exiciton ($D^{\circ}$, X) having very strong peak intensity. Then, the full-width-at -half-maximum(FWHM) and binding energy of neutral donor bound excition were 8 meV and 13.7 meV, respectivity. By Haynes rule, an activation energy of impurity was 137 meV.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2006.11a
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• pp.253-254
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• 2006

We have manufactured CdS and Cd(Cu)S thin films by chemical bath deposition(CBD) process, and examined the effects of $NH_4Cl$ and TEA. The addition of $NH_4Cl$ remarkably enhanced the film thickness of CdS, however, TEA slightly decreased the film thickness. The thickness of CdS film prepared from the aqueous solution of 0.003 M $CdSO_4$ 0.00008 M $CuSO_4$, 1.3M NH3, 0.03 M $SC(NH_2)_2$ and 0.0009 M $NH_4Cl$ was 210 nm and resistivity of that was $1.2{\times}10^3{\Omega}cm$.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.481-481
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• 2013

Chemical bath deposition (CBD) 기술에 의해 slide glass 기판 위에 CdS 박막을 적층 형성하였다. 적층된 박막들은 CdCl2와 thiorea (H2NCSNH2)를 증류수와 혼합 시dipping의 온도 조건, pH 조건, 시간 및 횟수를 달리하여 균일한 표면이 형성되도록 하였다. 적층된 박막은 $200^{\circ}C$ 이상의 고온에서 annealing하여 결정화하였다. 적층한 박막은 결정화 요인들을 XRD, FE-SEM, AFM, EDX, UV-Vis spectroscopy를 통해 조사하였다. 형성된 박막은 포토레지스터로 활용될 가능성을 조사하였다.

• Bulletin of the Korean Chemical Society
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• v.26 no.7
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• pp.1025-1026
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• 2005

• Transactions on Electrical and Electronic Materials
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• v.13 no.4
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• pp.196-199
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• 2012

CdS thin film was prepared on glass substrate by chemical bath deposition in an alkaline solution. The optical properties of CdS thin film were investigated using spectroscopic ellipsometry. The real (${\varepsilon}_1$) and imaginary (${\varepsilon}_2$) parts of the complex dielectric function ${\varepsilon}(E)={\varepsilon}_1(E)+i{\varepsilon}_2(E)$, the refractive index n(E), and the extinction coefficient k(E) of CdS thin film were obtained from spectroscopic ellipsometry. The normal-incidence reflectivity R(E) and absorption coefficient ${\alpha}(E)$ of CdS thin film were obtained using the refractive index and extinction coefficient. The critical points $E_0$ and $E_1$ of CdS thin film were shown in spectra of the dielectric function and optical constants of refractive index, extinction coefficient, normal-incidence reflectivity, and absorption coefficient. The dispersion of refractive index was analyzed by the Wemple-DiDomenico single-oscillator model.

• Electrical & Electronic Materials
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• v.5 no.1
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• pp.71-80
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• 1992

CdS박막을 5*$10^{-7}$Torr의 초기 진공하에서 CdS source 온도를 800~1100.deg.C로 하고 기판 온도를 100~200.deg.C로 하여 corning 7059 glass 기판위에 0.6~1.2.mu.m의 두께로 진공증착 방법으로 제조하였다. CdS soruce 온도와 기판온도가 증착된 CdS 박막의 미세구조와 결정구조 및 전기적, 광학적 성질에 미치는 영향을 알아 보았다. 기판을 가열하지 않은 경우는 source 온도가 증가할수록 전기비저항과 광투과도가 낮게 나타났다. Source 온도를 1100.deg.C로 고정하였을 경우 기판의 온도에 따라 전기비저항값과 광투과도값은 증가하였으며 optical band gap도 증가하였다. Soruce 온도가 1100.deg.C이고 기판온도가 190.deg.C일때 전기비저항값은 2*$10^{6}$ohm-cm였고 광투과도는 band gap 이상의 파장에서 80% 이상의 값을 가졌다. 증착된 CdS박막의 결정구조는 모두 hexagonal structure를 가지며 source 온도가 낮을수록 기판온도가 높을수록 C축으로 방향성있게 성장하였다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 1992.05a
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• pp.46-49
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• 1992

Cadmium sulfide thin films were deposited on glass substrate by Chemical Mist Deposition from solutions containing equimolar (0.1M) cadmium chloride and thiourea [(NH$_2$)$_2$CS] at a mist velocity of 1.6m/sec. Substrate temperatures were ranged between 200$^{\circ}C$ and 400$^{\circ}C$. The microstructure and semiconducting property of the films were investigated using SEM, X-ray diffraction, UV transmittance measurement and four point probe method. All the films have hexagonal structure and diffraction patterns indicate that the intensity of (112) and (101) reflections increase with increasing substrate temperature, whereas (002) reflection substrate temperature, whereas(002) reflection decrease for substrate temperatures between 250$^{\circ}C$ and 350$^{\circ}C$. The films prepared at lower temperature have a significant number of pinholes due probably to entrapped gaseous reaction. Optical transmittance of the films deposited at 350$^{\circ}C$ was about 75%. Optical bandgap of the films were 2.43eV regardless of substrate temperature. The dark resistivity of the films decreased with increasing substrate temperature up to 300$^{\circ}C$ and increased with further increasing substrate temperature. The films were photosensitive and had dark-to-light resistivity ratios of about 10 at room temperature for a white-light photoexcitation intensity of 50mw/$\textrm{cm}^2$.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2001.11b
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• pp.167-170
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• 2001

The stochiometric mix of evaporating materials for the $CdGa_{2}Se_{4}$ single crystal thin films was prepared from horizontal furnace. To obtain the single crystal thin films, $CdGa_{2}Se_{4}$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the Hot Wall Epitaxy (HWE) system. The source and substrate temperature were $630^{\circ}C$ and $420^{\circ}C$, respectively. The crystalline structure of single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of $CdGa_{2}Se_{4}$ single crystal thin films measured from Hall effect by van der Pauw method are $8.27{\times}10^{17}cm^{-3},345cm^{2}/V{\cdot}s$ at 293 K, respectively. From the photocurrent spectrum by illumination of perpendicular light on the c-axis of the $CuInSe_{2}$ single crystal thin film, we have found that the values of spin orbit splitting $\Delta$ So and the crystal field splitting $\Delta$Cr were 106.5 meV and 418.9 meV at 10 K, respectively. From the photoluminescence measurement on $CdGa_{2}Se_{4}$ single crystal thin film, we observed free excition (Ex) existing only high Quality crystal and neutral bound exiciton $(D^{0},X)$ having very strong peak intensity. Then, the full-width-at-half-maximum(FWHM) and binding energy of neutral donor bound excition were 8 meV and 13.7 meV, respectivity. By Haynes rule, an activation energy of impurity was 137 meV.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2001.11a
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• pp.167-170
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• 2001

The stochiometric mix of evaporating materials for the CdGa$_2$Se$_4$ single crystal thin films was prepared from horizontal furnace. To obtain the single crystal thin films, CdGa$_2$Se$_4$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the Hot Wall Epitaxy (HWE) system. The source and substrate temperature were 630$^{\circ}C$ and 420$^{\circ}C$, respectively. The crystalline structure of single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of CdGa$_2$Se$_4$ single crystal thin films measured from Hall erect by van der Pauw method are 8.27x10$\^$17/ cm$\^$-3/, 345 $\textrm{cm}^2$/V$.$s at 293 K, respectively. From the Photocurrent spectrum by illumination of perpendicular light on the c-axis of the CuInSe$_2$ single crystal thin film, we have found that the values of spin orbit splitting ΔSo and the crystal field splitting ΔCr were 106.5 meV and 418.9 meV at 10 K, respectively. From the photoluminescence measurement on CdGa$_2$Se$_4$ single crystal thin film, we observed free excition (E$\_$X/) existing only high quality crystal and neutral bound exiciton (D$\^$0/,X) having very strong peak intensity. Then, the full-width-at-half-maximum(FWHM) and binding energy of neutral donor bound excision were 8 meV and 13.7 meV, respectivity. By Haynes rule, an activation energy of impurity was 137 meV,