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1.
Au/SiO2纳米复合薄膜的微结构及光吸收特性研究   总被引:3,自引:2,他引:3       下载免费PDF全文
用多靶磁控溅射技术制备了Au/SiO2纳米多层薄膜.利用透射电子显微镜以及吸收光谱对Au/SiO2复合薄膜的微观结构、表面形貌及光学性能进行了表征和测试.研究结果表明:单层Au/SiO2薄膜中Au沉积时间小于10s时,分散在SiO2中的Au颗粒随Au的沉积时间的延长而增大;当沉积时间超过10s后,Au颗粒的尺寸几乎不随沉积时间变化,但Au颗粒的形状由网络状结构变为薄膜状结构.[Au(t1)SiO2(600)]×5多层薄膜在540-560nm波长附近有明显的表面等离子共振吸收峰,且吸收峰的强度随Au的沉积时间增加而增强.基于修正后的Maxwell-Garnett (M-G)有效媒质理论,讨论了金属颗粒的形状对等离子共振吸收峰的峰位和强度的影响.模拟的吸收光谱与实验吸收光谱形状、趋势及吸收峰位相符合.  相似文献   

2.
利用多靶磁控溅射技术制备了Au/SiO2纳米颗粒分散氧化物多层复合薄膜.研究了在保持Au单层颗粒膜沉积时间一定时薄膜厚度一定、变化SiO2的沉积时间及SiO2的沉积时间一定而改变薄膜厚度时,多层薄膜在薄膜厚度方向的微观结构对吸收光谱的影响.研究结果表明:具有纳米层状结构的Au/SiO2多层薄膜在560 nm波长附近有明显的表面等离子共振吸收峰,吸收峰的强度随Au颗粒的浓度增加而增强,在Au颗粒浓度相同的情况下,复合薄膜 关键词: 2纳米复合薄膜')" href="#">Au/SiO2纳米复合薄膜 多靶磁控溅射 吸收光谱 有效介质理论  相似文献   

3.
对用真空蒸发技术制备的Ag-MgF2复合纳米金属陶瓷薄膜(Ag的质量分数为0.15、0.20、0.30)的微结构及吸收光谱特性进行了研究。微结构分析表明薄膜由平均粒径约18nm的fcc-Ag纳米晶粒嵌埋于主要呈非晶态的MgF2基体中所组成。对吸收光谱的研究表明,Ag纳米微粒的表面离子共振吸收峰出现在λ=412nm-417nm波段范围内。随着Ag组分增加,吸收峰强度下降,呈现轻微红移并且逐渐宽化。  相似文献   

4.
介绍了几种计算纳米金属颗粒镶嵌于陶瓷基体中而形成的复合纳米金属陶瓷薄膜渗透阈的理论方法,分析了理论方法中所运用模型的特点及其精度.并将Landauer有效介质理论和Priou渗透阈理论应用于Ag-MgF2复合纳米金属陶瓷薄膜的渗透阈计算,所得值分别为0.08和0.14(Ag的体积分数),按Priou渗透阈理论计算的结果与实验结果相符.最后讨论了影响复合金属陶瓷薄膜体系渗透阈的主要因素. 关键词: 2复合纳米金属陶瓷薄膜')" href="#">Ag-MgF2复合纳米金属陶瓷薄膜 渗透阈理论 渗透阈  相似文献   

5.
Au/SiO2纳米多层薄膜的制备及其性质表征   总被引:2,自引:2,他引:2       下载免费PDF全文
利用多靶磁控溅射技术制备了Au/SiO2纳米颗粒分散氧化物多层复合薄膜.研究了在保持Au单层颗粒膜沉积时间一定时薄膜厚度一定、变化SiO2的沉积时间及SiO2的沉积时间一定而改变薄膜厚度时,多层薄膜在薄膜厚度方向的微观结构对吸收光谱的影响.研究结果表明:具有纳米层状结构的Au/SiO2多层薄膜在560nm波长附近有明显的表面等离子共振吸收峰,吸收峰的强度随Au颗粒的浓度增加而增强,在Au颗粒浓度相同的情况下,复合薄膜光学吸收强度随薄膜厚度的增加而增强.但当金属颗粒的浓度增加到一定程度时,金属颗粒相互接触,没有观察到纳米层状结构,薄膜不显示共振吸收峰特征.用修正后的M-G(Maxwell-Garnett)理论对吸收光谱进行了模拟,得到了与实验一致的结果.  相似文献   

6.
安蕾 《物理实验》2004,24(4):44-47
采用复合靶共溅射法制备了(Au,Si)/SiO2复合纳米颗粒薄膜样品,并对其荧光谱作了测量.在理论上分别计算了在强限域效应下和弱限域效应下Si纳晶吸收光谱的峰值位置与晶粒尺寸之间的关系,并采用Drude理论计算了Au/SiO2复合体系的吸收峰的峰值位置与微粒尺寸的关系.给出了(Au,Si)/SiO2体系复合薄膜共振吸收峰的位置随Au和Si的掺杂浓度比和微粒尺寸的相关特征.  相似文献   

7.
为提高VO2薄膜的热致变色性能,采用纳米结构和复合结构二者相结合的方法,通过磁控溅射技术先在玻璃衬底上制备高(002)取向ZnO薄膜,再在ZnO层上室温沉积钒金属薄膜,最后经热氧化处理获得纳米结构VO2/ZnO复合薄膜.利用变温拉曼光谱观察分析了VO2/ZnO薄膜相变前后的晶格畸变和键态的演变过程,讨论了薄膜的结构与热致红外开关特性和相变温度的内在关系.结果显示,与相同条件获得的同厚度的单层VO2薄膜相比,纳米VO关键词: ZnO 2')" href="#">VO2 纳米复合薄膜 热致变色 拉曼光谱  相似文献   

8.
(Au,Ag)/Si复合纳米颗粒薄膜的微结构与光谱特性   总被引:3,自引:1,他引:3       下载免费PDF全文
采用复合靶共溅射方法制备了(Au,Ag)/Si复合纳米颗粒薄膜,分别采用Maxwell-Garnett理论和微分有效媒质(DEM)理论计算了Ag/Si复合薄膜的吸收光谱,实验测量结果与DEM理论计算更接近,讨论了(Au,Ag)/Si体系复合薄膜共振吸收峰宽化的微观机制. 关键词:  相似文献   

9.
通过溶胶凝胶(sol-gel)法分别在玻璃衬底上制备了ZnO纳米薄膜和ZnO-SiO2纳米复合薄膜,并利用紫外-可见光分光光度计对薄膜的光学性能进行了分析.可见光-紫外透射谱显示,随着ZnO溶胶浓度从0.7mol/L降低到0.006mol/L,制备的ZnO薄膜从只出现一个380nm(对应的光学禁带宽度为3.27eV)左右的吸收边到在380和320nm(对应的光学禁带宽度为3.76eV)左右各出现一个吸收边,并且随着ZnO溶胶浓度的降低,在380—320nm波段内的透过率明显提高.而Z 关键词: 纳米ZnO 2复合薄膜')" href="#">ZnO-SiO2复合薄膜 溶胶凝胶法 透射率  相似文献   

10.
汪昌州  朱伟玲  翟继卫  赖天树 《物理学报》2013,62(3):36402-036402
采用磁控二靶(Ga30Sb70和Sb80Te20)交替溅射方法制备了新型Ga30Sb70/Sb80Te20纳米复合多层薄膜, 对多层薄膜周期中Ga30Sb70层厚度对相变特性的影响进行了研究. 结果表明, 多层薄膜的结晶温度可以通过周期中Ga30Sb70层厚度进行调节, 且随着Ga30Sb70层厚度的增加而升高. Ga30Sb70/Sb80Te20纳米复合多层薄膜的光学带隙随Ga30Sb70层厚度的增加而增大. 采用皮秒激光脉冲抽运光探测技术研究了多层薄膜的瞬态结晶动力学过程, 利用不同能量密度的皮秒激光脉冲可以实现Ga30Sb70/Sb80Te20多层薄膜非晶态和晶态的可逆转变.  相似文献   

11.
赵翠华  张波萍  尚鹏鹏 《中国物理 B》2009,18(12):5539-5543
Nano metal-particle dispersed glasses are the attractive candidates for nonlinear optical material applications.Au/SiO 2 nano-composite thin films with 3 vol% to 65 vol% Au are prepared by inductively coupled plasma sputtering.Au particles as perfect spheres with diameters between 10 nm and 30 nm are uniformly dispersed in the SiO 2 matrix.Optical absorption peaks due to the surface plasmon resonance of Au particles are observed.The absorption property is enhanced with the increase of Au content,showing a maximum value in the films with 37 vol% Au.The absorption curves of the Au/SiO 2 thin films with 3 vol% to 37 vol% Au accord well with the theoretical optical absorption spectra obtained from Mie resonance theory.Increasing Au content over 37 vol% results in the partial connection of Au particles,whereby the intensity of the absorption peak is weakened and ultimately replaced by the optical absorption of the bulk.The band gap decreases with Au content increasing from 3 vol% to 37 vol % but increases as Au content further increases.  相似文献   

12.
Au/SiO2 nanocomposite films were fabricated on Si (111) substrates by radio frequency (RF) magnetron sputtering technique and annealing at different temperature for 20 min (mode A) and at 1000 °C for different annealing time (mode B). The nanocomposite films were characterized by scanning electron microscopy (SEM), X-ray diffraction (XRD) and photoluminescence (PL). SEM results demonstrate that the size of Au crystallites in mode A first increases and then decreases, on increasing annealing temperature, according to the results of XRD spectra. Analysis of PL spectra in mode B shows that the intensity of the emission peak at 440 nm and 523 nm early increases and late decreases, with increasing annealing time at 1000 °C. The origin of the emission peak at around 440 nm was related to the size and quantity of Au particles and one of the emission peak at around 523 nm was related to the nanostructure of films in agreement with SEM imagines. Experimental results indicated that morphology, microstructure and luminescence of Au/SiO2 nanocomposite films showed close affinity with annealing temperature and annealing time.  相似文献   

13.
孙兆奇  蔡琪  宋学萍 《中国物理》2006,15(4):859-865
The microstructure and optical absorption of Au-MgF2 nanoparticle cermet films with different Au contents are studied. The microstructural analysis shows that the films are mainly composed of the amorphous MgF2 matrix with embedded fcc Au nanoparticles with a mean size of 9.8-21.4nm. Spectral analysis suggests that the surface plasma resonance (SPR) absorption peak of Au particles appears at λ=492-537nm. With increasing Au content, absorption peak intensity increases, profile narrows and location redshifts. Theoretical absorption spectra are calculated based on Maxwell-Garnett theory and compared with experimental spectra.  相似文献   

14.
Ge/SiO_2 and Si/SiO_2 films were deposited using the two-target alternation magnetron sputtering technique. The Au/Ge/SiO_2/p-Si and Au/Si/SiO_2/p-Si structures were fabricated and their electroluminescence (EL) characteristics were comparatively studied. Both Au/Ge/SiO_2/p-Si and Au/Si/SiO_2/p-Si structures have rectifying property. All the EL spectra from the two types of the structure have peak positions around 650-660 nm. The EL mechanisms of the structures are discussed.  相似文献   

15.
Au/SiO2 nanocomposite films were prepared on Si wafers by cosputtering of SiO2 and gold wires. Au/Si atomic ratios in Au/SiO2 nanocomposite films were varied from 0.53 to 0.92 by controlling the length of gold wire to study the evolution of the crystallization of gold, the size of Au/SiO2 nanocomposite particles, and the optical properties of as-deposited Au/SiO2 nanocomposite films. An X-ray photoelectron spectroscopy reveals that Au exists as a metallic phase in the bulk of SiO2 matrix. Dome-shaped Au/SiO2 nanocomposite particles and both Au (1 1 1) and (2 0 0) planes were observed in a field-emission scanning electron microscopy and X-ray diffraction studies respectively. With an ultraviolet-visible, absorption peaks of Au/SiO2 nanocomposite films were observed at 525 nm.  相似文献   

16.
孙小飞  魏长平  李启源 《物理学报》2009,58(8):5816-5820
以AgNO3,HAuCl4和正硅酸乙酯为主要原料,利用溶胶-凝胶法和旋涂技术,通过热处理和紫外光辐射还原得到了不同nAg/nAu(1∶0,2∶1,1∶2,0∶1)的Ag-Au合金/SiO2复合薄膜.从扫描电子显微镜和X射线衍射谱的结果可以看出得到的薄膜均匀性好,复合薄膜中合金颗粒的尺寸为10 nm左右.利用紫外-可见分光光谱仪研究了复合薄膜的光吸收性能,结果表明,随着nAg/nAu的降低,吸收峰的位置也由最初的Ag纳米粒子的等离子共振吸收峰430 nm附近,逐渐红移到Au纳米粒子的等离子共振吸收峰605和880 nm附近.从光吸收谱可以看出,nAgnAu=2∶1和1∶2的两个样品分别在515,730 nm附近和550,730 nm附近出现表面等离子共振吸收峰.这表明Au-Ag合金固溶体的形成. 关键词: 2')" href="#">Ag-Au合金/SiO2 紫外辐射 光吸收性能  相似文献   

17.
Au/SiO2 nanocomposite films were prepared by radio frequency sputtering technique and annealing. The above nanocomposite films were characterized by scanning electron microscopy (SEM), X-ray diffraction (XRD), and atomic force microscopy (AFM). The surface of the nanocomposite films was uniform with the particle diameter of 100-300 nm. The size of Au crystallites increased on increasing annealing time. The luminescent behavior of the nanocomposite films was characterized by photoluminescence (PL) with different excitation wavelengths. Two emission peaks at around 525 nm and 560 nm were observed with the excitation wavelength at 325 nm. An intensive emission peak at around 325 nm was observed with the excitation wavelength at 250 nm, which is related to the defective structure of the amorphous SiO2 layer because of oxygen deficiency, and could be applied to many fields, such as ultraviolet laser and ultraviolet detector.  相似文献   

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