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ZnS/PS复合体系的制备和性能表征 总被引:1,自引:0,他引:1
以电化学阳极氧化法制备的多孔硅(PS)为衬底,用脉冲激光沉积方法分别在200和300℃下制备了ZnS薄膜,得到ZnS/PS复合体系。利用X射线衍射仪(XRD)、扫描电子显微镜(SEM)、荧光分光光度计分别对ZnS/PS复合体系的晶体结构、形貌和光致发光(PL)特性进行了研究。XRD结果表明,制备的ZnS薄膜呈立方相晶体结构,沿β-ZnS(111)晶向择优取向生长,生长温度较高的样品的XRD衍射峰强度较大。SEM图像显示,生长温度较高的ZnS薄膜表面较致密平整。室温下的PL谱表明,沉积ZnS薄膜后,PS的发光峰发生蓝移。较高的生长温度下,ZnS的自激活发光强度较大,而PS的红光强度较低且峰位红移。根据三基色叠加的原理,ZnS的蓝绿光与PS的红光叠加在一起,ZnS/PS复合体系呈现出较强的白光发射,为固态白光发射器件的实现开辟了一条新的捷径。 相似文献
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用脉冲激光沉积法(PLD)在多孔硅(PS)衬底上生长ZnS薄膜,分别在300℃、400℃和500℃下真空退火。用X射线衍射(XRD)和扫描电子显微镜(SEM)研究了退火对ZnS薄膜的晶体结构和表面形貌的影响,并测量了ZnS/PS复合体系的光致发光(PL)谱和异质结的I-V特性曲线。研究表明,ZnS薄膜仅在28.5°附近存在着(111)方向的高度取向生长,由此判断薄膜是单晶立方结构的-βZnS。随着退火温度的升高,-βZnS的(111)衍射峰强度逐渐增大,且ZnS薄膜表面变得更加均匀致密,说明高温退火可以有效地促进晶粒的结合并改善结晶质量。ZnS/PS复合体系的PL谱中,随着退火温度升高,ZnS薄膜的自激活发光强度增大,而PS的发光强度减小,说明退火处理更有利于ZnS薄膜的发光。根据三基色叠加的原理,ZnS的蓝、绿光与PS的红光相叠加,ZnS/PS体系可以发射出较强的白光。但过高的退火温度会影响整个ZnS/PS体系的白光发射。ZnS/PS异质结的I-V特性曲线呈现出整流特性,且随着退火温度的升高其正向电流增加。 相似文献
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为了研究衬底多孔硅(PS)的孔隙对硫化锌/多孔硅(ZnS/PS)复合体系的光学性能和电学性质的影响,采用脉冲激光沉积方法在不同孔隙度的PS衬底上沉积了硫化锌薄膜。利用X射线衍射仪、扫描电子显微镜、荧光分光光度计和Ⅰ-Ⅴ特性曲线分别研究了PS衬底上ZnS薄膜的晶体结构、表面形貌和ZnS/PS复合体系的光学和电学性质。结果表明,沉积的ZnS薄膜呈立方相晶体结构,沿β-ZnS(111)晶向择优取向生长。随着衬底PS孔隙的增多,ZnS薄膜衍射峰的强度减小,且薄膜表面出现一些空洞和裂缝;在ZnS/PS复合体系的光致发光谱中,PS的发光相对于未沉积ZnS薄膜的PS有所蓝移,随着PS孔隙的增多,该蓝移量增大,而且在光谱中间550nm左右出现了一个新的绿光发射,归因于ZnS的缺陷中心发光。ZnS的蓝、绿光与PS的红光相叠加,整个ZnS/PS复合体系呈现出较强的白光发射。ZnS/PS异质结的Ⅰ-Ⅴ特性曲线呈现出与普通二极管相似的整流特性,在正向偏置下,电流密度较大,电压降较低;在反向偏置下,电流密度接近于0。随着衬底PS孔隙的增多,正向电流增大。该项研究结果为固态白光发射器件的实现奠定了基础。 相似文献
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WANG Cai-feng LI Qing-shan ZHANG Li-chun LV Lei QI Hong-xia 《光电子快报》2007,3(3):169-172
ZnS films were deposited on porous Si(PS) substrates with different porosities by pulsed laser deposition. The photolumi-nescence spectra of the samples were measured to study the effect of substrate porosity on luminescence properties of ZnS/porous Si composites. After deposition of ZnS films,the red photoluminescence peak of porous Si shows a slight blueshift compared with as-prepared porous Si samples. With an increase of the porosity,a green emission at about 550 nm was observed which may be ascribed to the defect-center luminescence of ZnS films,and the photoluminescence of ZnS/porous Si composites is very close to white light. Good crystal structures of the samples were observed by x-ray diffraction,showing that ZnS films were grown in preferred orientation. Due to the roughness of porous Si surface,some cracks appear in ZnS films,which could be seen from scanning electron microscope images. 相似文献
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We have investigated the mechanism of phase transformation from ZnS to hexagonal ZnO by hightemperature thermal annealing. The ZnS thin films were grown on Si(001) substrate by thermal evaporation system using ZnS powder as source material. The grown films were annealed at different temperatures and characterized by X-ray diffraction(XRD), photoluminescence(PL), four-point probe, scanning electron microscope(SEM) and energy dispersive X-ray diffraction(EDX). The results demonstrated that as-deposited ZnS film has mixed phases but high-temperature annealing leads to transition from ZnS to ZnO. The observed result can be explained as a twostep process:(1) high-energy O atoms replaced S atoms in lattice during annealing process, and(2) S atoms diffused into substrate and/or diffused out of the sample. The dissociation energy of ZnS calculated from the Arrhenius plot of 1000/T versus log(resistivity) was found to be 3.1 eV. PL spectra of as-grown sample exhibits a characteristic green emission at 2.4 eV of ZnS but annealed samples consist of band-to-band and defect emission of ZnO at 3.29 eV and 2.5 eV respectively. SEM and EDX measurements were additionally performed to strengthen the argument. 相似文献
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在Si(111)衬底上利用等离子体辅助分子束外延(P-MBE)生长氧化锌(ZnO)薄膜,研究了在不同衬底生长温度下(350~750℃)制备的ZnO薄膜的结构和光学性质.随着衬底温度的升高,样品的X射线及光致发光的半高宽度都是先变小后变大,衬底温度为550℃样品的结构及光学性质都比较好,这表明550℃为在Si(111)衬底上生长ZnO薄膜的最佳衬底温度;同时,我们还通过550℃样品的变温光致发光谱(81~300K)研究了ZnO薄膜室温紫外发光峰的来源,证明其来源于自由激子发射. 相似文献
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咔唑在Sol-Gel制备的SiO_2薄膜中的发光机理 总被引:1,自引:0,他引:1
利用溶胶-凝胶(sol-gel)工艺制备了能够发射红光的含咔唑的SiO2薄膜。测量了薄膜样品的发射谱,发现当激发波长从610nm连续减小到400nm时,样品的发射波长从760nm连续蓝移到了550nm左右。将含咔唑的SiO2薄膜溶解在乙醇中,经逐步稀释后所得溶液的发光可以从绿光变到紫光。基于它们的发射谱、激发谱和吸收谱,探讨了咔唑在SiO2薄膜中发红光的机理。结果表明,咔唑分子被紧缩在SiO2薄膜内部的微孔中,因受到挤压而使其共轭尺寸变大,从而导致咔唑的发光特性发生改变。 相似文献
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用脉冲激光沉积(PLD)方法在Si(111)和蓝宝石衬底上制备的氧化锌薄膜,在不同的退火温度和不同的退火氛围中进行了退火处理.退火温度及退火氛围对ZnO薄膜的结构和发光特性的影响用X射线衍射(XRD)谱和光致发光谱进行了表征.实验结果表明,随着退火温度的提高,ZnO薄膜的压应力减小,并向张应力转化.在不同的退火温度退火... 相似文献
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SiC/SiO_2镶嵌结构薄膜光致发光特性研究 总被引:2,自引:0,他引:2
采用 SiC/SiO_2复合靶,用射频磁控共溅射技术和高温退火的方法制备了 SiC/SiO_2纳米镶嵌结构复合薄膜,并应用傅里叶红外吸收(FTIR),X 射线衍射(XRD),扫描电镜(SEM)和光致发光(PL)实验分析了薄膜的结构、表面形貌以及光致发光性能。结果表明,样品经高温退火后在 SiO_2基质中有 SiC 纳米颗粒形成。以 280 nm 波长光激发样品薄膜表面,显示出较强的 365 nm 的紫外光发射以及 458 nm 和 490 nm 处的蓝光发射,其发光强度随退火温度从 800℃升高至 1 050℃而增强。其发光归结为薄膜中与 Si-O 相关的缺陷形成的发光中心。 相似文献
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脉冲激光沉积法制备氧化锌薄膜 总被引:7,自引:0,他引:7
ZnO是一种新型的Ⅱ-Ⅵ族半导体材料,具有优良的晶格、光学和电学性能,其显著的特点是在紫外波段存在受激发射。利用脉冲激光沉积法(PLD)在氧气氛中烧蚀锌靶制备了纳米晶氧化锌薄膜,衬底为石英玻璃,晶粒尺寸约为28-35 nm。X射线衍射(XRD)结果和光致发光(PL)光谱的测量表明,当衬底温度在100-250℃范围内时,所获得的ZnO薄膜具有c轴的择优取向,所有样品的强紫外发射中心均在378-385 nm范围内,深能级发射中心约518-558 nm,衬底温度为200℃时,得到了单一的紫外光发射(没有深能级发光)。这归因于其较高的结晶质量。 相似文献
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We report on the photoluminescent (PL) properties of ZnO thin films grown on SiO2/Si(100) substrates using low pressure metal-organic chemical vapor deposition. The growth temperature of the films was as
low as 400°C. From the PL spectra of the films at 10–300 K, strong PL peaks due to free and bound excitons were observed.
The origin of the near bandedge emission peaks was investigated measuring temperature-dependent PL spectra. In addition, the
Zn O films demonstrated a stimulated emission peak at room temperature. Upon illumination with an excitation density of 1
MW/cm2, a strong, sharp peak was observed at 3.181 eV. 相似文献
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利用ZnO微晶粉末以化学电泳法成功地在导电玻璃上制备了不同x值的紫外发光的宽禁带氧化物半导体三元化合物MgxZn1-xO薄膜.电子显微镜和X 射线衍射研究显示,薄膜由MgxZn1-xO微晶组成,薄膜中微晶大小的分散度比ZnO粉末有所减小,并更具择优取向的趋势.室温下光致发光测量给出,MgxZn 1-xO薄膜在小于380nm的紫外波段出现较强的半宽小于20nm的激子性发光峰,而且带边峰的半宽以及带边峰与杂质缺陷峰强度之比均较原始的ZnO粉末有明显改善,表明这种MgxZn1-xO薄膜具有优良的紫外发光特性. 相似文献
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HfOxNy 填充多孔Si空穴结构在室温下得到了改善的光致发光。观测到425nm处强的蓝光和690nm红的发光峰。量子限制效应和极化效应应该是产生发光峰的原因。N/O的化学配比同样影响蓝光发射。最后观测到样品具有极弱的温度淬灭效应。 相似文献
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CdS nanocrystals have been successfully grown on porous silicon (PS) by sol-gel method. The plan-view field emission scanning electron microscopy (FESEM) shows that the pore size of PS is smaller than 5 μm in diameter and the agglomerates of CdS are broadly distributed on the surface of PS substrate. With the increase of annealing time, the CdS nanoparticles grow in both length and diameter along the preferred orientation. The cross-sectional FESEM images of ZnO/PS show that CdS nanocrystals are uniformly penetrated into all PS layers and adhere to them very well. photoluminescence (PL) spectra demonstrate that the intensity of PL peak located at about 425 nm has almost no change after the annealing time increases. The range of emission wavelength of CdS/PS is from 425 nm to 455 nm and the PL intensity is decreasing with the annealing temperature increasing from 100 °C to 200 °C. 相似文献
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Photoluminescence origin of nanocrystalline SiC films 总被引:1,自引:0,他引:1
LIU Ji-wen LI Juan LI Yan-hui LI Chang-ling ZHAO Yan-ping ZHAO Jie XU Jing-jun 《光电子快报》2005,1(2):96-99
The nanocrystalline SiC films were prepared on Si then annealed at 800℃ and 1 000℃ for 30 minutes (111) substrates by rf magnetron sputtering and in a vacuum annealing system. The crystal structure and crystallization of as-annealed SiC films were determined by the Fourier transform infrared (FIR) absorption spectra and the X-ray diffraction (XRD) analysis. Measurement of photoluminescence (PL) of the nanocrystalline SiC (nc-SiC) films shows that the blue light with 473 nm and 477 nm wavelengths emitted at room temperature and that the PL peak shifts to shorter wavelength side and the PL intensity becomes stronger as the annealing temperature decreases. The time-resolved spectrum of the PL at 477 nm exhibits a bi-exponential decay process with lifetimes of 600 ps and 5 ns and a characteristic of the direct band gap. The strong blue light emission with short PL lifetimes suggests that the quantum confinement effect of the SiC nanocrystals resulted in the radiative recombination of the direct optical transitions. 相似文献
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