Metal-Organic Chemical Vapor Deposition of Zn-In-Sn-O and Ga-In-Sn-O Transparent Conducting Oxide Thin Films

1999 ◽  
Vol 607 ◽  
Author(s):  
A. Wang ◽  
N.L. Edleman ◽  
J.R. Babcock ◽  
T.J. Marks ◽  
M.A. Lane ◽  
...  

AbstractThe metal-organic chemical vapor deposition (MOCVD) technique has been successfully applied for growth of Sn-doped transparent, conducting Zn-In-O and Ga-In-O films using Sn(acac)2, In(dpm)3, Ga(dpm)3, and Zn(dpm)2, as volatile precursors. The 25 °C electrical conductivity of the as-grown films is as high as 1030 S/cm (n-type, carrier density N = 4.5 × 1020 cm−3, mobility µ = 14.3 cm2/V•s) for the Zn-In-O series and 700 S/cm (n-type, N = 8.1 × 1019 cm−3, µ = 55.2 cm2/V•s) for the Ga-In-O series. After Sn-doping, the Zn-In-O series exhibits 25 'C electrical conductivities as high as 2290 S/cm with a higher carrier mobility, while the Ga-InO series exhibits higher electrical conductivity (3280 S/cm at 25 °C) and much higher carrier density, but with diminished mobility. All films show broader optical transparency windows than that of commercial ITO films. Reductive annealing, carried out at 400-425 °C in a flowing gas mixture of H2(4%) and N2, results in increased carrier density and mobility as high as 64.6 cm2/V•s for films without Sn doping, but lowered carrier density for the Sn-doped films. X-ray diffraction, transmission electron microscopy, micro diffraction, and high-resolution X-ray analysis show that all films with good conductivity have cubic, homogeneously doped In2O3-like crystal structures.

1997 ◽  
Vol 495 ◽  
Author(s):  
A. Wang ◽  
S. C. Cheng ◽  
J. A. Belot ◽  
R. J. Mcneely ◽  
J. Cheng ◽  
...  

ABSTRACTThis contribution reports the in situ growth of transparent, conducting GaxIn2-xO3 and ZnkIn2Ok+3 films by MOCVD (metal-organic chemical vapor deposition) techniques using In(dpm)3, Ga(dpm)3, and Zn(dpm)2 (dpm = dipivaloylmethanate) as volatile precursors. In the former series, film microstructure in the x = 0.4 – 1.0 range is predominantly cubic with 25° C electrical conductivities as high as 1300 S/cm (n-type; carrier density = 1.2 × 1020 cm−3, mobility = 68 cm2/Vs) and optical transparency in the visible region greater than that of ITO. In the latter series, films in the composition range K = 0.16 – 3.60 were studied; the microstructural systematics are rather complex. Electrical conductivities (25° C) as high as 1000 S/cm (n-type; carrier density = 3.7 × 1020 cm−3, mobility = 18.6 cm2/Vs) for K = 0.66 were measured. The optical transparency window is significantly broader than that of ITO.


2007 ◽  
Vol 515 (5) ◽  
pp. 2921-2925 ◽  
Author(s):  
Chunyu Wang ◽  
Volker Cimalla ◽  
Genady Cherkashinin ◽  
Henry Romanus ◽  
Majdeddin Ali ◽  
...  

1997 ◽  
Vol 487 ◽  
Author(s):  
Daiji Noda ◽  
Torn Aoki ◽  
Yoichiro Nakanishi ◽  
Yoshinori Hatanaka

AbstractFor epitaxial growth of compound Zn1−xCd1−XTe by metal organic chemical vapor deposition (MOCVD), it is difficult to obtain a high composition ratio x. In this study, we have adopted a remote plasma enhanced (RPE) MOCVD method for the epitaxial growth. Cd1−xZnxTe with the composition ratio x in the range of 0 to 1 has been obtained while varying the ratio of dimethylcadmium (DMCd) to diethylzinc (DEZn) from 0 to 20%. The crystallinity of the epitaxial films was about 400 to 700 arcsec FWHM defined by X ray diffiraction measurements.


2007 ◽  
Vol 515 (14) ◽  
pp. 5593-5596 ◽  
Author(s):  
R.-V. Wang ◽  
F. Jiang ◽  
D.D. Fong ◽  
G.B. Stephenson ◽  
P.H. Fuoss ◽  
...  

1999 ◽  
Vol 597 ◽  
Author(s):  
John McAleese ◽  
L. Gary Provost ◽  
Gary S. Tompa ◽  
Andrei Colibaba-Evulet ◽  
Nick G. Gulmac ◽  
...  

AbstractOver the past 30 years, the need for transparent conducting oxide coatings has been met almost exclusively by tin doped indium-oxide. As the display market advances in complexity, the demand for alternative transparent materials exhibiting high conductivity and stability has become greater. In this paper, we discuss briefly the merits of using doped ZnO as a superior transparent conducting oxide. We report here our results in scaling our ZnO MOCVD reactor technology from 5° to 12° diameter susceptors. Using Rotating Disk Reactor-Low Pressure Metal Organic Chemical Vapor Deposition, we have been able to obtain large area uniformity on multiple (14 cm × 9 cm) glass sheets per deposition run. Promising film characteristics suggest significant application in the field of flat panel displays and other optical systems may be possible.


1992 ◽  
Vol 280 ◽  
Author(s):  
Yu-neng Chang

ABSTRACTIn this report, the impact of deposition temperature variation on the evolution of film morphology and microstructure was studied. In the copper oxide metal organic chemical vapor deposition (MOCVD) process, a temperature gradient was created on the substrate surface. By using a specific design of the heating susceptor, the local temperature of the leading edge (upstream) on the substrate surface was maintained at 70°C lower than the temperature of the ending (downstream) edge. The evolution of local composition and microstructure in deposited films were analyzed by X-ray diffraction (XRD), transmission Fourier Transform Infrared Spectroscopy (FTIR), X-ray photoelectron spectroscopy (XPS), and SEM. From XPS and XRD results, Cu2O rich phase was deposited at the low temperature area, while CuO rich phase was deposited at the high temperature area. These two areas were divided by a phase intermixing (transition) zone of 40–100 ums wide. The temperature of this abrupt Cu2O->CuO deposition product transition was determined to be 390°C -400°C. As indicated by SEM results, the low temperature favorite Cu2O continuous phase, collapsed into coarse grains (with the scale of 10 urn) first, then became fine grains among channels of CuO phase, and finally diminished into the high temperature favorite CuO continuous phase. Spatially resolved XPS results also indicated that the film composition changed abruptly through the transition zone. A nucleation-growth competition mechanism, between the Cu2O rich phase and the CuO rich phase, was suggested to occur in this zone. In this model, this dynamic deposition product transition is interpreted by the temperature dependency of nucleation rates for the specific CuO phase or Cu2O phase.


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