共查询到18条相似文献,搜索用时 15 毫秒
1.
J. C. Swartz B. Siegel A. D. Morrison H. Lingertat 《Journal of Electronic Materials》1974,3(2):309-326
In preliminary work to adapt the edge-defined, film-fed growth (EFG) process to GGG, a number of 1 cm wide × 0.5 mm thick
ribbon crystals were obtained. Most of the crystals contained longitudinal thermal stress patterns and associated dislocation
arrays. Also evident were occasional arrays of microvoids just under the external surface. In one case where the thermal stresses
were avoided, the crystal quality appeared to be sufficient for use in magnetic bubble devices. Off-stoichiometric inclusions
on the gallia-rich side were eutectic structures of gallia and garnet and on the gadolinia-rich side were an unidentified
gadolinium-rich compound. Lattice parameter measurements of the EFG crystals show that the effective distribution coefficients
are much higher than those for the Czochralski growth method.
B. Siegel is now with Man Labs., Cambridge, Mass., and H. Lingertat is now with GTE Laboratory, Waltham, Mass. 相似文献
2.
Li Xiaoting Wang Tao Wang Jingwei Wang Yiding Yin Jingzhi Sai Xiaofeng Gao Hongkai Zhang Zhiyong 《半导体学报》2005,26(12):2298-2302
采用自制的低压金属有机化学气相淀积设备,用三甲基镓、三甲基铟作为III族源,三甲基锑和砷烷作为V族源在(100)面GaSb和GaAs单晶衬底上分别外延生长了InAsSb材料. 用X射线双晶衍射、原子力显微镜、扫描电镜和电子探针能谱仪等对材料特性进行了表征,研究了生长温度、V/III比、过渡层等生长参数对外延层质量的影响. 获得了与GaSb衬底晶格失配度为0.4%的表面光亮且晶体质量较好的InAs0.85Sb0.15外延层. 相似文献
3.
After each process of a chemical etching, heat-cleaning, melt-back, or soaking in HC1, the substrate surface of GaSb was characterized
by the Auger electron spectroscopy with a simultaneous Ar sputtering to reveal oxide layer structures. An optimum treatment
process of GaSb surfaces for low temperature LPE growth of AlGaSb was established. Uniform growth of epitaxial AlGaSb on GaSb
is demonstrated for a wide temperature range(from 500‡C to as low as 250‡C). 相似文献
4.
The liquidus curves in the Cu-Sb-S system near CuSbS2 composition and between CuSbS2 and Sb2S3 were determined by cooling arrests of seeded melts. CuSbS2 melts congruently at 552.25 ± 0.14°C and a eutectic occurs between CuSbS2 and Sb2S3 at 490 ± 5°C and 0.72 ± 0.05 mole fraction Sb2S3. No additional phases appear on the liquidus surface in this portion of the Cu-Sb-S system. Crystals of CuSbS2 were grown from the stoichiometric composition using the Bridgman Stockbarger method. At room temperature, the band gap of
CuSbS2 is 0.28 eV; however below 80K, a drop in resistivity suggests the appearance of a new phase. Measurements of photo current
suggest that the band gap of the low temperature phase is greater than 0.58 eV. 相似文献
5.
Pascal F. Delannoy F. Bougnot J. Gouskov L. Bougnot G. Grosse P. Kaoukab J. 《Journal of Electronic Materials》1990,19(2):187-195
The growth of GaSb by MOVPE and itsn-type doping using a dimethyltellurium dopant source are investigated. The results of growth rate, morphology and Te incorporation
as a function of growth parameters are given. Increasing growth temperature and V/III reactant ratio were found to reduce
the Te incorporation. The lowest Hall carrier concentrations obtained at room-temperature, onp-type andn-type MOVPE GaSb are respectively:p
H= 2.2 × 1016cm−3 with a Hall mobility ofμ
H= 860 cm2/V.s andn
H= 8.5 × 1015cm−3 withμ
H= 3860 cm2/V.s. Furthermore, Hall mobilities as high as 5000 cm2/V.s were measured onn-type GaSb samples. 相似文献
6.
By using a two-temperature annealing technique to reduce native defect concentrations we have achieved carrier concentrations
as low as 5. 6 x l015 cm-3 in bulk single crystals of PbS. Hall coef-ficient, electrical resistivity, thermoelectric power, infrared absorption coefficient,
and CO2 laser transmission scan measure-ments were carried out for various samples in the carrier con-centration range from 5. 6
x l015 cm-3 to 4. 8 x 1018 cm-3. The low-temperature carrier concentration data were analyzed using a quantitative theory for the native defect concentrations
as a function of the sulfur vapor pressure. Calculations based on this theory yield good agreement with experiment for intrinsic
carrier concentration and defect equilibrium coefficient values of 5.5 x 1017 cm-3 and 5. 0 x 1017 cm-3, respectively, at 600°C.
This work was sponsored by the Department of the Air Force. 相似文献
7.
Capacitance and Hall effect measurements in the temperature range 10-300 K were performed to evaluate the deep and shallow
level characteristics of Si-doped n-AlxGa-xAs layers with 0 × 0.4 grown by molecular beam epitaxy. For alloy compositions × 0.3 the overall trap concentration was found
to be less than 10−2 of the carrier concentration. In this composition range the transport properties of the ternary alloy are comparable to those
of n-GaAs:Si except for lower electron mobibities due to alloy scattering. With higher Al content one dominant electron trap
determines the overall electrical properties of the material, and in n-Al0.35Ga0.65As:Si the deep trap concentration is already of the order of the free-carrier concentration or even higher. For the composition
× = 0.35 ± 0.02 the influence of growth temperature and of Si dopant flux intensity on the deep trap concentration, on shallow
and deep level activation energy, and on carrier freeze-out behaviour was studied and analyzed in detail. Our admittance measurements
clearly revealed that the previously assumed deepening of the shallow level in n-Alx Ga1-x As of alloy composition close to the direct-indirect cross-over point does actuallynot exist. In this composition range an increase of the Si dopant flux leads to a reduction of the thermal activation energy
for electron emission from shallow levels due to a lowering of the emission barrier by the electric field of the impurities.
The increasing doping flux also enhances the concentration of the dominant electron trap strongly, thus indicating a participation
of the dopant atoms in the formation of deep donor-type (D,X) centers. These results are in excellent agreement with the model
first proposed by Lang et al. for interpretation of deep electron traps in n-Alx Ga1-x grown by liquid phase epitaxy. 相似文献
8.
Tl3InSe4 single crystal has been successfully prepared by the Bridgman crystal growth technique. The crystal that is reported for the first time is found to be of tetragonal structure with lattice parameters of a=0.8035 and c=0.6883 nm. The electrical resistivity and Hall effect measurements on the crystal revealed a conductivity type conversion from p- to n-type at a critical temperature of 283 K. The electron to hole mobility ratio is found to be 1.10. The analysis of the temperature-dependent electrical resistivity, Hall coefficient and carrier concentration data reveals the extrinsic type of conduction with donor impurity levels that behave as acceptor levels when are empty. The data analysis allowed the calculation of the hole and the electron effective masses as 0.654m0 and 0.119m0, respectively. In addition, the temperature-dependent Hall mobility in the n-region is found to be limited by the electron–phonon short-range interactions scattering with an electron–phonon coupling constant of 0.21. 相似文献
9.
Single crystal of the ternary semi-conductor AgInSe2 has been grown by Bridgman technique. The AgInSe2 crystal crystallizes in the tetragonal chalcopyrite structure. Using melt temperature oscillation method polycrystalline charge was synthesized. The synthesized charge was subjected to powder X-ray diffraction analysis. Thermal property of AgInSe2 was analyzed using differential scanning calorimetry (DSC) technique. The melting and solidification temperature is 777 °C and 761 °C respectively. The synthesized polycrystalline charge was employed to grow AgInSe2 single crystals. The grown crystal was confirmed by single crystal X-ray diffraction. The crystal exhibits 60% transmission in the Infrared region. The stoichiometric composition of AgInSe2 was confirmed by Energy dispersive X-ray analysis (EDAX). The electrical properties of the crystal were studied by Hall Effect measurements and photoconductivity. 相似文献
10.
K. L. Hess P. D. Dapkus H. M. Manasevit T. S. Low B. J. Skromme G. E. Stillman 《Journal of Electronic Materials》1982,11(6):1115-1137
An analytical study of the impurities in trimethylgallium (TMGa) and subsequent correlation of the effect of these impurities
on resulting GaAs films grown by metalorganic chemical vapor deposition (MOCVD) is presented. The effects of using fractional
distillation techniques to improve the quality of TMGa and to help isolate and identify major source impurities in TMGa is
detailed. Photothermal ionization data are presented which show the residual donor species present and their relative concentrations
in the epitaxial layers. Correlations of the residual donor concentrations with TMGa preparation are made. It is demonstrated
that high purity GaAs with μ77 K ≈ 125,000 cm2/V-sec can be grown by MOCVD using repurified trimethylgallium and arsine source materials.
Work supported in part by the U.S. Naval Research Laboratory on Contract No. N00173-80-C-0066. 相似文献
11.
应用中频感应提拉法生长了掺杂浓度高达 5 0at. %的Yb∶YAG晶体 ,研究了室温下Yb∶YAG晶体的吸收和发射光谱特性以及荧光寿命 ,在 939nm和 96 9nm处存在Yb3 + 离子的 2个吸收带 ,能与InGaAs激光二极管(LD)有效耦合 ,适合激光管二极抽运。其荧光主峰位于 10 32nm附近 ,Yb∶YAG晶体的荧光寿命为 390 μs。比较了高掺杂与低掺杂Yb∶YAG晶体的光谱参数 ,指出高掺杂Yb∶YAG晶体是一种很有前景的高功率激光增益介质 相似文献
12.
采用熔剂-坩埚下降法生长了91%Pb(Zn1/3Nb2/3)O3-9%PbTiO3(PZNT91/9)(摩尔分数)弛豫铁电单晶,PbO助熔剂摩尔分数控制在50%左右。所得晶体被PbO助熔剂包裹,将其浸泡在热HNO3中1~2天即可除去PbO。晶体呈浅黄色,具有明显的结晶学生长面。晶体沿(001)面切出数片,晶片质量明显好于通气Bridgman法生长的PZNT单晶。偏光显微镜可观察到71°、90°、180°畴或微畴区。晶片极化条件为:垂直于C面施加1kV/mm的电场并保持10~15min。 相似文献
13.
高质量镁铝尖晶石单晶生长的研究 总被引:3,自引:0,他引:3
对制作微波延迟线用镁铝尖晶石单晶生长进行了研究,采用原料配比为MgO:Al2O3=1:1(mol),通过化学反应间接合成MgAl2O4多晶料,使用铱坩埚盛料,选用中频感应加热,在氩气中用提拉法以及合适的温场和最佳工艺参数,生长了出了高质量的镁铝尖晶石单晶,其性能达到微波器件使用要求。 相似文献
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设计了一种用于买现低损耗、近零超平坦色散特性的光子晶体光纤结构,这种结构光纤包层空气孔层数少,内三层空气孔直径相同,制作过程简单;应用多极法研究了此结构PCF各个参数特别是最外层空气孔直径对色散和损耗特性的影响,通过优化结构,设计出了在1.3μm至1.65μm波长范围内色散绝对值小于0.5ps/(nm.km),1.55μm处损耗为4.5dB/km的低损耗近零超平坦色散光子晶体光纤。 相似文献