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1.
We report on the successful growth of β-Ga2O3 single crystals using the Czochralski method. Model calculations show that the gas phase consists of Ga2O, GaO or Ga independent of the ratio of oxygen and Ar or N2. We find that for growing single crystals the evaporation has to be suppressed by a finite amount of oxygen. A CO2/Ar gas atmosphere was found to meet this requirement.  相似文献   

2.
Large-size single crystals of β-Ga2O3 with 1 inc in diameter have been grown by the floating zone technique. The stable growth conditions have been determined by the examination of the crystal structure. Wafers have been cut and fine polished in the (1 0 0), (0 1 0) and (0 0 1) planes. These were highly transparent in the visible and near UV, as well as electrically conductive, indicating the potential use of β-Ga2O3 as a substrate for optoelectic devices operating in the visible/near UV and with vertical current flow.  相似文献   

3.
作为宽禁带半导体材料的一员,结构稳定的β-Ga2O3具有比SiC和GaN更宽的禁带宽度和更高的巴利加优值,近年来受到科研人员的广泛关注。本文采用射频(RF)磁控溅射法在C面蓝宝石衬底上生长β-Ga2O3薄膜,探究溅射过程中衬底加热温度的影响。溅射完成后通过高温退火处理提升薄膜质量,研究衬底加热温度和后退火温度对氧化镓薄膜晶体结构和表面形貌的影响。利用X射线衍射(XRD)、原子力显微镜(AFM)等测试手段对β-Ga2O3薄膜晶体结构、表面形貌等进行分析表征。实验结果表明,随着衬底加热温度的升高,β-Ga2O3薄膜表面粗糙度逐渐降低,薄膜晶体质量得到显著提升;在氧气气氛中进行后退火,合适的后退火温度有利于氧化镓薄膜重新结晶、增大晶粒尺寸,能够有效修复薄膜的表面态和点缺陷,对于改善薄膜晶体质量有明显优势。  相似文献   

4.
The single-crystalline β-wollastonite (β-CaSiO3) nanowires were prepared via a simple hydrothermal method, in the absence of any template or surfactant using cheap and simple inorganic salts as raw materials. Xonotlite [Ca6(Si6O17)(OH)2] nanowires were first obtained after hydrothermal treatment at a lower temperature of 200 °C for 24 h, and after being calcinated at 800 °C for 2 h, xonotlite nanowires completely transformed into β-wollastonite nanowires and the wire-like structure was preserved. The synthesized β-wollastonite nanowires had a diameter of 10–30 nm, and a length up to tens of micrometers, and the single-crystalline monoclinic parawollastonite structured β-wollastonite was identified by XRD with the space group of P21/a and cell constants of a=15.42 Å, b=7.325 Å, c=7.069 Å and β=95.38°. A possible growth mechanism of β-wollastonite nanowires was also proposed. The advantages of this method for the nanowire synthesis lie in the high yield, low temperature and mild reaction conditions, which will allow large-scale production at low cost.  相似文献   

5.
利用等离子增强原子层沉积技术(PEALD)在c面蓝宝石衬底上制备了氧化镓(Ga2O3)薄膜,研究了退火气氛(v(N2)∶v(O2)=1∶1(体积比)、空气和N2)及退火时间对Ga2O3薄膜晶体结构、表面形貌和光学性质的影响。研究结果表明,退火前的氧化镓处于亚稳态,不同退火气氛下退火后晶体结构发生明显改变,而且退火气氛中N2比例增加有利于Ga2O3重结晶。在N2气氛下退火达到30 min,薄膜结构已由亚稳态转变成择优取向的β-Ga2O3。而且表面形貌分析表明,退火30 min后表面形貌开始趋于稳定,表面晶粒密度不再增加。另外实验样品在 400~800 nm的平均透射率几乎是100%,且光吸收边陡峭。采用N2气氛退火,对于富氧环境下沉积的Ga2O3更利于薄膜表面原子迁移,以及择优取向Ga2O3重结晶。  相似文献   

6.
Without the use of any extra surfactant or template, γ-MnOOH single crystalline nanowires were synthesized directly through the hydrothermal reaction between KMnO4 and toluene in distilled water at 180 °C for 24 h; and β-MnO2 single crystalline nanowires could be obtained just by calcination of the γ-MnOOH nanowires in air at 280 °C for 5 h. The as-prepared γ-MnOOH and β-MnO2 nanowires were characterized by X-ray powder diffraction, atomic absorption spectroscopy, Fourier transformed infrared spectroscopy, scanning electron microscope, transmission electron microscope, high-resolution transmission electron microscope and selected area electron diffraction.  相似文献   

7.
11B (I=3/2) MAS NMR in the binary glass system xV2O5–B2O3 (x=0.053, 0.43) and the ternary glass system xV2O5–B2O3–PbO (0.1x1.5) has been investigated at room temperature. In the xV2O5–B2O3 glasses, one NMR line due to BO3 unit was observed. Meanwhile in the xV2O5–B2O3–PbO, two NMR lines which arise from BO3 and BO4 units were detected, where the appearance of BO4 units is produced by the presence of PbO. From the computer-simulation of the 11B NMR central transition line (m=−1/2↔1/2), the quadrupole parameters (e2qQ/h and η) for BO3 units in xV2O5–B2O3, and those for BO3 and BO4 units in xV2O5–B2O3–PbO were obtained as a function of x. As the V2O5 content increases in xV2O5–B2O3–PbO, the e2qQ/h and η values of the BO3 associated resonance are found to slightly decrease and increase, respectively. Meanwhile, the e2qQ/h and η values of BO4 associated resonance in xV2O5–B2O3–PbO are found to slightly increase and decrease, respectively. By comparing the intensities of the total transitions (m=−3/2↔−1/2,m=−1/2↔1/2, and 1/2↔3/2) for the 11B NMR line of BO3 and BO4 units contained in xV2O5–B2O3–PbO with those of respective standard samples of 0.053V2O5–B2O3 and NaBH4, the quantitative fractions of BO3 and BO4 in xV2O5–B2O3–PbO were obtained as a function of x.  相似文献   

8.
采用自主设计搭建的雾化辅助化学气相沉积系统设备,开展了Ga2O3薄膜制备及其特性研究工作。通过X射线衍射研究了沉积温度、系统沉积压差对Ga2O3薄膜结晶质量的影响。结果表明,Ga2O3在425~650 ℃温度区间存在物相转换关系。随着沉积温度从425 ℃升高至650 ℃,薄膜结晶分别由非晶态、纯α-Ga2O3结晶状态向α-Ga2O3、β-Ga2O3两相混合结晶状态改变。通过原子力显微镜表征探究了生长温度对Ga2O3薄膜表面形貌的影响,从475 ℃升高至650 ℃时,薄膜表面粗糙度由26.8 nm下降至24.8 nm。同时,高分辨X射线衍射仪测试表明475 ℃、5 Pa压差条件下的α-Ga2O3薄膜样品半峰全宽仅为190.8″,为高度结晶态的单晶α-Ga2O3薄膜材料。  相似文献   

9.
Indium oxide (In2O3) nanobelts have been fabricated by thermal evaporation of metallic indium powders with the assistance of Au catalysts. The as-synthesized nanobelts are single-crystalline In2O3 with cubic structure, and usually tens of nanometers in thickness, tens to hundreds of nanometers in width, and several hundreds of micrometers in length. The room temperature photoluminescence spectrum of In2O3 nanobelts features a broad emission band at 620 nm, which could be attributed to oxygen deficiencies in the as-synthesized belts. The formation of In2O3 nanobelts follows a catalyst-assistant vapor—liquid–-solid growth mechanism, which enables the controlled growth of individual belts on predetermined sites.  相似文献   

10.
《Journal of Non》2003,330(1-3):128-141
The electrical and dielectric properties for three series of MoO3–Fe2O3–P2O5 and one series of SrO–Fe2O3–P2O5 glasses were measured by impedance spectroscopy in the frequency range from 0.01 Hz to 3 MHz and over the temperature range from 303 to 473 K. It was shown in Part I that the MoO3 is incorporated into phosphate network and the structure/properties are strongly influenced by the overall O/P ratio. The Fe2O3 content and Fe(II)/Fetot ratio in these glasses have significant effects on the electrical conductivity and dielectric permittivity. With decreasing Fe2O3 content in MoO3–Fe2O3–P2O5 glasses with O/P at 3.5 the dc conductivity, σdc(ω) decreases for two orders of magnitude, which indicates that the conductivity for these glasses depends on Fe2O3 and is independent of the MoO3 content. Also, the dielectric properties such as (ω), (ω) and σac(ω) and their variation with frequency and temperature indicates a decrease in relaxation intensity with increase in the concentration of MoO3. On the other hand, the dc conductivity for MoO3–Fe2O3–P2O5 glasses with O/P > 3.5 increases with the substitution of MoO3 which has been explained by an increase in the number of non-bridging oxygens and formation of Fe–O–P bonds that are responsible for formation of small polarons. The increase in the dielectric permittivity, (ω) with increasing MoO3 content is attributed to the increase in the deformation of glass network with increasing bonding defects. For SrO–Fe2O3–P2O5 glasses the conductivity and dielectric permittivity remained constant with increasing SrO.  相似文献   

11.
Ga2O3是一种新兴的宽带隙半导体,在电力和射频电子系统中具有潜在的应用前景。前期研究以β-Ga2O3为主,并且已经对β-(AlxGa1-x)2O3/Ga2O3异质结构中的二维电子气(2DEG)进行了理论计算,本文主要研究ε-(AlxGa1-x)2O3作为势垒层对ε-(AlxGa1-x)2O3/ε-Ga2O3异质结电子输运性质的影响,首先介绍了ε-(AlxGa1-x)2O3/ε-Ga2O3异质结的结构和性质,分析计算了由于ε-(AlxGa1-x)2O3/ε-Ga2O3异质结的自发极化和压电极化所产生的极化面电荷密度,以及极化对2DEG浓度产生的影响,接着分析了在不同Al摩尔组分下,ε-(AlxGa1-x)2O3势垒层厚度与合金无序散射、界面粗糙度散射和极性光学声子散射之间的关系。最后通过计算得出结论:界面粗糙度散射和极性光学声子散射对ε-(AlxGa1-x)2O3/ε-Ga2O3异质结的电子输运性质有重要影响,合金无序散射对异质结的输运性质影响较小;2DEG浓度、合金无序散射、界面粗糙度散射和极性光学声子散射的电子迁移率强弱由ε-(AlxGa1-x)2O3势垒层的厚度和Al摩尔组分共同决定。  相似文献   

12.
We investigated the dependence of the Y2O3 film growth on Si surface at initial growth stage. The reflection high-energy electron diffraction, X-ray scattering, and atomic force microscopy showed that the film crystallinity and morphology strongly depended on whether Si surface contained O or not. In particular, the films grown on oxidized surfaces revealed significant improvement in crystallinity and surface smoothness. A well-ordered atomic structure of Y2O3 film was formed on 1.5 nm thick SiO2 layer with the surface and interfacial roughness markedly enhanced, compared with the film grown on the clean Si surfaces. The epitaxial film on the oxidized Si surface exhibited extremely small mosaic structures at interface, while the film on the clean Si surface displayed an island-like growth with large mosaic structures. The nucleation sites for Y2O3 were provided by the reaction between SiO2 and Y at the initial growth stage. The SiO2 layer known to hinder crystal growth is found to enhance the nucleation of Y2O3, and provides a stable buffer layer against the silicide formation. Thus, the formation of the initial SiO2 layer is the key to the high-quality epitaxial growth of Y2O3 on Si.  相似文献   

13.
Phase relations around langasite (LGS, La3Ga5SiO14) were studied on the basis of phase assemblage observed during calcination and crystallization process of samples of various compositions in the ternary system La2O3–Ga2O3–SiO2. A ternary compound of apatite structure, La14GaxSi9–xO39–x/2 was found for the first time. Crystallization of this compound was observed in the cooling process of molten samples of stoichiometric LGS as well as LGS single crystal, demonstrating that LGS is an incongruent-melting compound. A phase diagram was established primarily based on the crystallization sequence in the cooling process.  相似文献   

14.
In this study, single-crystal γ-MnO2 nanowires have been successfully synthesized at room temperature in the absence of catalysts or templates, the diameter was found to be ca. 10–20 nm and the characteristic lengths up to several micrometers. The crystal phase of nanowires was confirmed by XRD and TEM measurements. Further, a dissolution– condensation–recrystallization process was proposed for the formation of nanowires under the room temperature condition.  相似文献   

15.
K. Hirao  T. Komatsu  N. Soga 《Journal of Non》1980,40(1-3):315-323
Mössbauer absorption measurements have been made at room temperature on 57Fe in iron sodium silicate glasses containing 3–15 mol% Fe2O3 and various iron alkali silicate crystals in order to study the state of iron in these glasses. The spectra of all the glasses gave one doublet with a quadrupole splitting varying from 0.73–0.78 mm s−1, while those of Na2O · Fe2O3 · 4 SiO2 and 5 Na2O · Fe2O3 · 8 SiO2 crystals showed much smaller quadrupole splitting, 0.28 mm s−1 and 0.10 mm s−1, respectively, and an asymmetrical doublet of much narrower linewidth. When sodium was replaced by other alkali metals of larger size, such as K and Cs, in MFeSi2O6 and MFeSi3O8 crystals, the quadrupole splitting became wider and approached to 0.73 mm s−1. Such a variation was not observed for glasses. These results suggest that a larger number of non-identical sites exist in iron sodium silicate glasses than in the corresponding crystals.  相似文献   

16.
近年来,宽禁带半导体材料β-Ga2O3越来越多地受到关注,在材料制备、掺杂、刻蚀等方面都有广泛研究。射频磁控溅射是常用的β-Ga2O3薄膜制备方法之一,后退火处理往往是提高薄膜质量的关键工艺步骤。本文研究后退火工艺中退火温度和退火气氛对射频磁控溅射在C面蓝宝石基底上制备得到的β-Ga2O3薄膜材料的影响。X射线衍射和原子力显微镜表征结果表明:在氮气气氛下退火,退火温度为1 000 ℃时得到的β-Ga2O3薄膜质量较优;相同的温度下,氧气气氛退火比氮气气氛退火更有利于提升薄膜的结晶性能、降低表面粗糙度;在氧气气氛下,1 000 ℃退火得到的薄膜质量相对比900 ℃退火得到的薄膜质量好。  相似文献   

17.
The MoS2 nanowires with diameters of 4 nm and lengths of 50 nm were synthesized by a hydrothermal method using 0.36 g MoO3 and 1.8 g Na2S as precursors in 0.4 mol/l HCl solution at 260°C. The products are characterized by XRD, XPS, TEM, HTEM and BET. Results show that the as-prepared MoS2 nanowires consist of 1–10 sulfide layers with BET surface areas of 107 m2/g. The possible reaction route and the formation mechanism of the MoS2 nanowires are discussed. The effects of exterior conditions such as pH value, temperature, concentration of precursors and additives on the particle size and morphology of MoS2 crystallites were investigated.  相似文献   

18.
Solid solutions of NdxLa2−xcaB10O19 with different Na3+ concentration have been synthesized by substituting Nd 3+ for La3+ in La2CaB10O19 Powder X-ray diffraction analysis shows that Nd3+ is easy to incorporate into the crystal. Single crystal ndxLa2−xCaB10O19 (NLCB) in centimeter size has been grown by Kyropoulos method. The crystal has strong absorption around 580nm and 805nm. The fluorescence spectra indicate that there is an energy transition at 1.06μm. And the SHG of NLCB is about the twice as that of KDP. These favorable features make NLCB a candidate for laser NLO multifunctional materials.  相似文献   

19.
A novel approach for preparation of red-emitting europium-doped yttrium oxide phosphor (Y2O3:Eu) by using the bicontinuous cubic phase (BCP) process was reported in this paper. The BCP system was composed of anionic surfactant sodium bis(2-ethylhexyl)sulfosuccinate (AOT) and aqueous yttrium nitrate/europium nitrate solution. Energy dispersive spectrometer analysis revealed the homogeneous precipitation occurred in the BCP structure. Thermogravimetric analysis measurements indicated the precursor powder was europium-doped yttrium hydroxide, Y1−xEux(OH)3. Scanning electron microscopy micrographs showed the precursor powder had a primary size about 30 nm and narrow size distribution. After heat treatment in furnace above 700 °C for 4 h, high crystallinity Y2O3:Eu phosphors was obtained. However, the primary size of particles grew to 50–200 nm and the dense agglomerates with a size below 1 μm were formed. X-ray diffraction patterns indicated the crystal structure of precursor powders and Y2O3:Eu phosphors were amorphous and body-centered cubic structure, respectively. The photoluminescence analysis showed that the obtained Y2O3:Eu phosphor had a strong red emitting at 612 nm and the quenching started at a Eu concentration of 10 mol%. This study indicated that the BCP process could be used to prepare the highly efficient oxide-based phosphors.  相似文献   

20.
The La L1 and L3 XANES and L3 EXAFS have been investigated for the series of glasses 10K2O---50SiO2---x La2O3 (x = 1, 5, 10) and (10 − x)K2O---40SiO2−(x/3)La2O3 (x = 7.5, 5, 2.5) and model compounds La2O3, LaAlO3, LaPO4, La2NiO4, La2CuO4 and La(OH)3. An edge resonance at 25 eV above the L1 edge in the glass spectra is concentration-dependent, decreasing in intensity with increasing lanthanum concentration. The 2s → nd forbidden transition increases with La2O3 concentration, indicating a reduction in the ‘average’ site symmetry of the first coordination shell of La. Mapping X(k) space, which is a new and promising technique, was employed to extract bond distance, coordination number and thermal parameters from the EXAFS. By this method, one calculates the complete X(k) space a function of all physically reasonable values of the adjusted parameters in all possible combinations. The advantage in this method is the assurance of a global minimum. Bond lengths were comparable to those obtained by Fourier transforming the phase corrected EXAFS. The values are 2.42 Å (± 0.03 Å) for La---O. The coordination numbers (N ≤ 7 ± 1.5) were derived by mapping and comparison to the published structures for other La compounds. X(k) mapping is compared with least-squares fitting the data, and the correlation between the Debye-Waller factor and coordination number is also discussed.  相似文献   

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