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1.
SnO2 films have been deposited on Y-stabilized ZrO2 (YSZ) (1 0 0) substrates at different substrate temperatures (500–800 °C) by metalorganic chemical vapor deposition (MOCVD). Structural, electrical and optical properties of the films have been investigated. The films deposited at 500 and 600 °C are epitaxial SnO2 films with orthorhombic columbite structure, and the HRTEM analysis shows a clear epitaxial relationship of columbite SnO2(1 0 0)||YSZ(1 0 0). The films deposited at 700 and 800 °C have mixed-phase structures of rutile and columbite SnO2. The carrier concentration of the films is in the range from 1.15×1019 to 2.68×1019 cm−3, and the resistivity is from 2.48×10−2 to 1.16×10−2 Ω cm. The absolute average transmittance of the films in the visible range exceeds 90%. The band gap of the obtained SnO2 films is about 3.75–3.87 eV.  相似文献   

2.
T. Serin  N. Serin  H. Sar?  O. Pakma 《Journal of Non》2006,352(3):209-215
This study investigated the effect of the substrate temperature on the structural, optical, morphological, and electrical properties of undoped SnO2 films prepared by a spray deposition method. The films were deposited at various substrate temperatures ranging from 300-500 °C in steps of 50 °C and characterized by different optical and structural techniques. X-ray diffraction studies showed that the crystallite size and preferential growth directions of the films were dependent on the substrate temperature. These studies also indicated that the films were amorphous at 300 °C and polycrystalline at the other substrate temperatures used. Infrared and visible spectroscopic studies revealed that a strong vibration band, characteristic of the SnO2 stretching mode, was present around 630 cm−1 and that the optical transmittance in the visible region varied over the range 75-95% with substrate temperature, respectively. The films deposited at 400 °C exhibited the highest electrical conductivity property.  相似文献   

3.
In this paper the synthesis of SnO2 nanoparticles with average particle size up to about 70 nm using SnCl22H2O and NH4OH in 1‐botanol solution by the precipitation method is reported and the inhibition of sodium dodecyl sulphate (SDS) on the SnO2 particle growth is investigated by soaking SnO2precursor in the SDS solution for 24 h. The as‐prepared SnO2and SDS modified‐SnO2 powders, then, were calcined at different temperatures and the X‐ray powder diffraction (XRD) and Fourier transform infrared spectroscopy (FT‐IR) were used to characterize the output samples. The XRD results reveal that the structure of tin‐dioxide is tetragonal rutile and the as‐prepared SnO2 nanoparticles grow with increasing the annealing temperature, while the SDS treatment prevents the particle growth under the same condition. Furthermore, the FT‐IR results indicate the formation of tin‐hydroxyl group which are then converted into tin‐dioxide with heat treatment. Further characterization of the samples by the transmission electron microscopy (TEM) and the photoluminescence (PL) spectroscopy was carried out. The room temperature PL spectra of SnO2exhibits broad and strong peak attributed to the surface defects such as oxygen vacancies and intensity of which decreases with the increase in particle size. (© 2012 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

4.
Undoped and 5%(Mn, In)-doped SnO2 thin films were deposited on Si(1 0 0) and Al2O3 (R-cut) by RF magnetron sputtering at different deposition power, sputtering gas mixture and substrate temperature. X-ray reflectivity was used to determine the films thickness (10–130 nm) and roughness (~1 nm). The combination of X-ray diffraction and Mössbauer techniques evidenced the presence of Sn4+ in an amorphous environment, for as-grown films obtained at low power and temperature, and the formation of crystalline SnO2 for annealed films. As the deposition power, substrate temperature or O2 proportion are increased, SnO2 nanocrystals are formed. Epitaxial SnO2 films are obtained on Al2O3 at 550 °C. The amorphous films are quite uniform but a more columnar growth is detected for increasing deposition power. No secondary phases or segregation of dopants were detected.  相似文献   

5.
Porous silicon (PSi) was formed at different current densities in the range of 5-60 mA/cm2 by electrochemical anodized etching in HF for different durations in the range of 10-30 min. Above this PSi structure, SnO2 films were deposited by the spin coating technique. The PSi has been characterized by X-ray diffraction studies. Peaks pertaining to PSi along with those corresponding to SnO2 are observed. Atomic force microscopic studies indicate that very fine needle like silicon nanostructures are observed which is the result of the best PSi structure formed at 30 mA/cm2. For the SnO2 covered PSi structures, larger grains are observed with uniform coverage. The PSi samples prepared at current densities above and below 30 mA/cm2 show PL spectra with asymmetric and overlapped peaks. The PL profile of thin SnO2 film coated on PSi shows a peak at 633 nm and a small hump at about 660 nm.  相似文献   

6.
Growth of tin oxide thin films using molecular beam epitaxy in a pyrolyzed nitrogen dioxide atmosphere on a titanium dioxide (1 1 0) substrate was investigated using X-ray photoelectron spectroscopy (XPS), electron diffraction, and atomic force microscopy (AFM). Properties of deposited films were studied for their dependence on substrate temperature and oxidation gas pressure. Analyses using XPS data revealed that tin atoms were fully oxidized to Sn4+ and SnO2 films were grown epitaxially in deposition conditions of substrate temperatures of 627 K or higher and NO2 pressure greater than 3×10−3 Pa. At a substrate temperature of 773 K, a smooth surface with atomic steps was visible in the SnO2 films, but above or below this temperature, fine grains with crystal facets or porous structures appeared. At pressures of 8×10−4 to 3×10−4 Pa, the randomly oriented SnO phase was dominantly grown. Further decreasing the pressure, the Sn metal phase, which was epitaxially crystallized at less than 500 K, was also grown.  相似文献   

7.
Mercuric iodide has been grown for the first time heteroepitaxially on a substrate. α-HgI2 is deposited as a single crystalline layer which is azimuthally completely oriented. The orientation of the grown layer has been confirmed with texture X-ray diffractometry, reflection powder diffractometry and Atomic Force Microscopy.  相似文献   

8.
Thin films of various thicknesses in the MIM structure have been prepared from the powder of SnO2/Sb2O3 mixed sample by the thermal evaporation technique in a vacuum of 10−5 Torr. Dielectric properties of SnO2/Sb2O3 mixed thin films have been studied with temperature starting from LNT to RT and above RT and frequency ranging from 100 Hz to 16 kHz. The activation energy for the migration of charge carriers in SnO2/Sb2O3 mixed thin films has been calculated and it is found to be 0.23 eV. The results thus obtained on dielectric properties of SnO2/Sb2O3 mixed thin films are presented and discussed.  相似文献   

9.
Optical properties of spray deposited antimony (Sb) doped tin oxide (SnO2) thin films, prepared from SnCl2 precursor, have been studied as a function of antimony doping concentration. The doping concentration was varied from 0‐4 wt.% of Sb. All the films were deposited on microscope glass slides at the optimized substrate temperature of 400 °C. The films are polycrystalline in nature with tetragonal crystal structure. The doped films are degenerate and n‐type conducting. The sheet resistance of tin oxide films was found to decrease from 38.22 Ω/□ for undoped films to 2.17 Ω/□ for antimony doped films. The lowest sheet resistance was achieved for 2 wt.% of Sb doping. To the best of our knowledge, this sheet resistance value is the lowest reported so far, for Sb doped films prepared from SnCl2 precursor. The transmittance and reflectance spectra for the as‐deposited films were recorded in the wavelength range of 300 to 2500 nm. The transmittance of the films was observed to increase from 42 % to 55 % (at 800 nm) on initial addition of Sb and then it is decreased for higher level of antimony doping. This paper investigates the variation of optical and electrical properties of the as‐deposited films with Sb doping. (© 2003 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

10.
A novel method was developed for synthesizing ultralong SnO2 zigzag belts with the assistance of CuO powder. The crystalline structure and morphology of SnO2 zigzag belts were characterized using x‐ray diffraction, scanning electron microscopy and transmission electron microscopy. The growth mechanism of the ultralong SnO2 zigzag belts and the catalytic behavior of the copper were discussed. The humidity sensor based on as‐synthesized product shows high sensitivity and fast response time due to unique structure of the SnO2 zigzag belts with large surface‐to‐volume ratio. It can be found that the resistance of the SnO2 materials decreases obviously with increasing relative humidity (RH) at room temperature (26 °C). The results demonstrate that these SnO2 nanostructures are potential to be used as effective and high performance humidity sensors. (© 2010 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

11.
Fe-doped nanosized SnO2 powders were prepared by chemical co-precipitation technique using SnCl4 and FeCl3 as starting materials and water as a carrier. Experimental results show that the grain size of Fe-doped SnO2 crystallites is smaller than 5 nm, and the particle size is smaller than 15 nm. When the calcination temperature is below 650 °C, the SnO2 crystal has tetragonal lattice structure. At higher temperature the particles become a two-phase mixture of tetragonal SnO2 and hexagonal Fe2O3 crystallites. Fe doping can obviously prevent the growth of nanosized SnO2 crystallites, and a higher Fe-doping concentration is more effective to prevent the growth of nanosized SnO2 particles when the calcination temperature is below 550 °C.  相似文献   

12.
Nanocrystalline and transparent conducting SnO2‐ ZnO films were fabricated by employing an inexpensive, simplified spray technique using a perfume atomizer at relatively low substrate temperature (360±5 °C) compared with conventional spray method. The structural studies reveal that the SnO2‐ZnO films are polycrystalline in nature with preferential orientation along the (101) plane. The dislocation density is very low (1.48×1015lines/m2), indicating the good crystallinity of the films. The crystallite size of the films was found to be in the range of 26–34 nm. The optical transmittance in the visible range and the optical band gap are 85% and 3.6 eV respectively. The sheet resistance increases from 8.74 kΩ/□ to 32.4 kΩ/□ as the zinc concentration increases from 0 to 40 at.%. The films were found to have desirable figure of merit (1.63×10–2 (Ω/□)–1), low temperature coefficient of resistance (–1.191/K) and good thermal stability. This simplified spray technique may be considered as a promising alternative to conventional spray for the massive production of economic SnO2 ‐ ZnO films for solar cells, sensors and opto‐electronic applications. (© 2010 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

13.
The influence of crucibles (Au or Pt) on the structure, electrical, dielectric and optical properties of 70TeO2·30PbCl2 glasses doped with Pr3+ added as a metal, chloride, or oxide, in concentrations of 500–1500 wt-ppm, is reported. The dc conductivity of ‘pure’ glasses prepared in Au crucibles is two orders of magnitude higher than that of those prepared in Pt crucibles. Upon doping, the dc conductivity of glasses prepared in Pt and Au crucibles increases or decreases, respectively. The static relative permittivity is equal to 33 ± 2. In the range of 640–700 nm, six photoluminescence (PL) peaks were observed, at 641.5, 647.1, 652.4, 660.8, 662.9, and 664.5 nm. In the range of 200–1200 cm−1, seven Raman scattering (RS) peaks were observed at 184, 217, 321, 468, 654, 735 cm−1, and a small peak at 650 cm−1. Both spectra were deconvoluted using symmetrical Gaussian functions. Relative intensities of PL and RS bands depend on the concentration and chemical form of Pr3+ and on the material of the crucible. However, positions of these bands are independent of these conditions.  相似文献   

14.
SnO2@carbon (SnO2@C) nanofibers (NFs) have been prepared by electrospinning method and evaluated as anodes in lithium‐ion battery half cells. XRD were carried out to provide further information about the structure of the as‐prepared NFs, and all the peaks can be readily indexed to the rutile phase SnO2 (JCPDS No. 41–1445). Electrochemical characterization by galvanostatic charge‐discharge tests shows that the NF anodes have first discharge capacities of 1375.5 mA h g−1 at 80 mA g−1current density. This excellent Li‐ion storage capability of SnO2 NFs is probably resulting from protection of amorphous carbon and the synergy arising from that the ultrafine SnO2 particles embedded in the carbon nanofiber (CNF) matrix: the nanometer‐sized SnO2@C NFs can provide not only negligible diffusion times of ions thus faster phase transitions but also enough space to buffer the volume changes during the lithium insertion and extraction reactions. The highly dispersed NFs are expected to be applied as attractive anodes for lithium‐ion batteries.  相似文献   

15.
Branched Zn-doped SnO2 nanorod clusters with tunable size and aspect ratios were prepared by a facile solvothermal process. The introduction of a small quantity of Zn2+ proved to play an important role in directing the anisotropic growth of SnO2 nanocrystals. The as-synthesized products exhibit tetragonal rutile structure and many lattice defects exist in the products. The possible growth mechanism has been proposed. These Zn-doped SnO2 nanorods exhibited unique Raman spectrum in contrast with the undoped SnO2 nanostructures. These Zn-doped SnO2 nanorods showed good sensitivities to ethanol gas, acetone gas, and benzene gas.  相似文献   

16.
《Journal of Non》2005,351(46-48):3619-3623
Tin dioxide (SnO2) nanorods have been successfully synthesized in bulk quantity by a calcining process based on annealing precursor powders in which sodium chloride, sodium carbonate, and stannic chloride were homogeneously mixed. Transmission electron microscopy shows that the as-prepared nanorods are structurally perfect and uniform, with widths of 10–25 nm, and lengths of several hundreds nanometers to a few micrometers. X-ray diffraction and energy-dispersive X-ray spectroscopy analysis indicate that the as-prepared nanorods have the same crystal structure and chemical composition found in the tetragonal rutile form of SnO2. Selected area electron diffraction and high-resolution transmission electron microscopy reveal that the as-prepared nanorods grow along the [1 1 0] crystal direction. We found that the calcined temperature has a strong influence on the size and morphology of SnO2 nanorods. The growth process of SnO2 nanorods is suggested to follow an Ostwald ripening mechanism. Our findings indicate that other nanorods or nanowires may be manipulated by using this technique, and might provide insight into the new opportunities to control materials fabrication.  相似文献   

17.
Transparent dielectric thin films of MgO has been deposited on quartz substrates at different temperatures between 400 and 600°C by a pneumatic spray pyrolysis technique using Mg(CH3COO)2·4H2O as a single molecular precursor. The thermal behavior of the precursor magnesium acetate is described in the results of thermogravimetry analysis (TGA) and differential thermal analysis (DTA). The prepared films are reproducible, adherent to the substrate, pinhole free and uniform. Amongst the different spray process parameters, the substrate temperature effect has been optimized for obtaining single crystalline and transparent MgO thin films. The films crystallize in a cubic structure and X‐ray diffraction measurements have shown that the polycrystalline MgO films prepared at 500°C with (100) and (110) orientations are changed to (100) preferred orientation at 600°C. The MgO phase formation was also confirmed with the recorded Fourier Transform Infrared (FTIR) results. The films deposited at 600°C exhibited highest optical transmittivity (>80%) and the direct band gap energy was found to vary from 4.50 to 5.25 eV with a rise in substrate temperature from 500 to 600°C. The measured sheet resistance and the resistivity of the film prepared at 600°C were respectively 1013Ω/□ and 2.06x107Ω cm. The surface morphology of the prepared MgO thin films was examined by atomic force microscopy. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

18.
ABSTRACT

TiO2:SnO2 thin films were deposited on glass substrates, by using sol gel spin coating method with different ratio (3%, 5% and 7%) at 3200 rpm, to study their effect on different properties of TiO2: SnO2 thin films. The structural and optical properties of films have studied for different ratio. These deposited films have been characterized by various methods such as X-Ray Diffraction (XRD), Ultra Visible spectroscopy. The (XRD) can be used to identify crystal structure of as deposited films. The Transmission spectra have shown the transparent and opaque parts in the visible and UV wavelengths.  相似文献   

19.
《Journal of Non》2006,352(26-27):2921-2924
Sn-doped silicate fibers exhibit extremely high photosensitivity when exposed to 248 nm KrF excimer laser. Electron micrograph probing has shown that nanoscale phase separation occurs in fibers and fiber preforms after UV exposure. This phenomenon has been observed only in SnO2-doped germanosilicate and phosphosilicate fibers and fiber preforms when the SnO2 concentration is high. At low SnO2 concentrations no phase separation has been observed. SnO2 codoped glasses are the first optical fibers to exhibit phase separation.  相似文献   

20.
We report on the Kerr signal enhancement as a result of the capping effect of SnO2 on the CoFeSiB amorphous layer. The magnetic layer was deposited by pulsed laser deposition method on Cu buffer layer and was capped by SnO2 with different thicknesses. The magnetic behavior of the samples was investigated by the Kerr effect. As the SnO2 thickness increased up to about 70 nm, the Kerr signal increased and then reduced. The results were analyzed using the formalism based on the matrix method.  相似文献   

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