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1.
磷掺杂纳米硅薄膜的研制   总被引:8,自引:0,他引:8       下载免费PDF全文
用PECVD薄膜沉积方法,成功地制备了磷掺杂纳米硅(nc-Si:H(P))薄膜.用扫描隧道电镜(STM)、Raman散射、傅里叶变换红外吸收(FTIR)谱、电子自旋共振(ESR)、共振核反应(RNR)技术对掺磷纳米硅进行了结构分析,确认了样品的微结构为纳米相结构.掺磷后膜中纳米晶粒的平均尺寸d减小,一般在25—45nm之间,且排列更加有序.掺磷nc-Si:H膜具有较高的光吸收系数,光学带隙在173—178eV之间,和本征nc-Si:H相同.掺杂nc-Si:H薄膜电导率在10-1关键词:  相似文献   

2.
超细SnO2纳米晶粒带边光吸收的线度效应   总被引:1,自引:0,他引:1       下载免费PDF全文
康俊勇  S.TSUNEKAWA  A.KASUYA 《物理学报》2001,50(11):2198-2202
采用超细过滤方法,分别制备含有平均线度小于2nm的超细SnO2纳米晶粒的酸性和碱性溶胶溶液.通过动态光散射、X射线衍射和晶粒透射电子显微镜像测量,确定了SnO2晶粒的线度.对其光吸收谱测量发现,超细过滤后酸性和碱性溶胶溶液中晶粒的带边光吸收能量均有明显蓝移.分析结果表明,SnO2晶粒的线度减小是同类晶粒带边光吸收蓝移的主要原因. 关键词: 超细纳米晶粒 透射电子显微镜 带边光吸收 表面化学修饰  相似文献   

3.
采用螺旋波等离子体化学气相沉积技术以N2/SiH4/H2为反应气体制备了镶嵌有纳米非晶硅颗粒的氢化氮化硅薄膜,通过改变N2流量实现了薄膜从红到蓝绿的可调谐光致发光.傅里叶红外透射和紫外-可见光吸收特性分析表明,所生长薄膜具有较高的氢含量,N2流量增加使氢的键合结构发生变化,非晶硅颗粒尺寸减小,所对应的薄膜的光学带隙逐渐增加和微观结构有序度减小.可调光致发光(PL)主要来源于纳米硅颗粒的量子限制效应发光,随N2流量增加,PL的谱线展宽并逐渐增强. 关键词: 傅里叶红外透射谱 光吸收谱 纳米硅粒子镶嵌薄膜 光致发光  相似文献   

4.
以金属W和Ta为热丝,采用热丝化学气相沉积 ,在250℃玻璃衬底上沉积多晶硅薄膜.研究了热丝温度、沉积气压、热丝与衬底间距等沉积参数对硅薄膜结构和光电特性的影响,在优化条件下获得晶态比Xc>90%,暗电导率σd=10-7—10-6Ω -1cm-1,激活能Ea=0.5eV,光能隙Eopt≤1.3 eV的多晶硅薄膜. 关键词: 多晶硅薄膜 热丝化学气相沉积 光电特性  相似文献   

5.
采用脉冲激光气相沉积(PLD)方法,在Si(100)晶面上制备了Co:BaTiO3纳米复合薄膜.采用X射线衍射(XRD)结合透射电镜(TEM)方法研究了两种厚度Co:BaTiO3纳米复合薄膜的晶体结构,当薄膜厚度约为30 nm时,薄膜为单一择优取向;当薄膜厚度约为100nm时,薄膜呈多晶结构.原子力显微镜(AFM)分析表明,当膜厚为30nm时,薄膜呈现明显的方形晶粒.采用紫外光电子能谱(UPS)研究了Co的价态和Co:BaTiO3纳米复合薄 关键词: 3')" href="#">BaTiO3 纳米复合薄膜 紫外光电子能谱  相似文献   

6.
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   

7.
采用射频磁控溅射技术与热退火处理制备了纳米锗镶嵌二氧化硅(nc-Ge/SiO2)复合薄膜.对薄膜的光吸收谱进行分析,得到了纳米Ge晶粒的光学带隙.单光束Z-扫描的实验结果表明薄膜具有较强的可饱和吸收特性.将薄膜作为可饱和吸收体插入LD端面抽运的Nd:YVO4激光器内,分别实现1342 nm和1064 nm激光的被动调Q,得到脉宽分别为29 ns和22 ns的脉冲序列.理论分析认为,纳米Ge晶粒形成的界面态和缺陷态对1342 nm激光产生的饱和吸收作用,是导致被动调Q的主要原因.  相似文献   

8.
刘震  王玉晓  宋瑛林  张学如 《物理学报》2013,62(16):167801-167801
利用时域有限差分方法, 研究硅薄膜上下表面周期半圆凹槽结构对于太阳光吸收的增强效应. 研究发现这种结构可以实现太阳光宽波段的光吸收增强, 通过调节SiO2表面减反层厚度和凹槽半径长度来实现薄膜太阳能电池最大的光吸收, 并实现了波长在300-1000 nm范围的太阳光吸收总能量比没有这种 结构下硅薄膜光吸收提高了约117%. 关键词: 硅薄膜 半圆凹槽 吸收增强  相似文献   

9.
采用溶胶-凝胶法制备了Eu3+掺杂的钛酸钇晶态发光薄膜。通过X射线衍射(XRD)对薄膜的结构和结晶过程进行了分析,利用荧光分光光度计对薄膜的发光性质开展了测试和研究。XRD结果表明,薄膜包含立方相YxTi1-xO1-0.5x晶粒,该晶粒属立方晶系,Fm3m(225)空间群,晶胞参数a=0.530nm,晶粒尺寸约为17nm。荧光光谱表明,Eu3+掺杂的YxTi1-xO1-0.5x薄膜显示了强的红光发射,其中Eu3+5D07F2超灵敏跃迁为最强一组。紫外氙灯、准分子激光器、汞灯等是这种发光薄膜的有效激发源。  相似文献   

10.
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   

11.
It is reported in this paper that the phenomenon of the saturated absorption of the exciton in hydrogenated nanocrystalline silicon (nc-Si:H) thin film fabricated by plasma enhanced chemical vapor deposition (PECVD) without any post-processing is observed at room temperature using pump-probe technology. This nonlinear optical absorption property is induced by the surface effect of the silicon nanoparticles in nc-Si:H thin films.  相似文献   

12.
Hydrogenated nanocrystalline silicon (nc-Si:H) thin films were fabricated by plasma enhanced chemical vapor deposition under the various negative substrate bias voltages with hydrogen as a diluent of silane. The microstructure and optical properties of nc-Si:H thin films were studied by Raman scattering spectroscopy, X-ray diffraction (XRD), transmission electron microscopy, and optical transmission spectroscopy. Raman spectra and XRD pattern reveal that applying negative bias voltages at the moderate level favors the enhancement of crystalline volume fraction, increase of crystallite sizes and decrease of residual stress. We also demonstrated that the negative direct current bias can be used to modulate the volume fraction of voids, refractive index, absorption coefficient, compactness and ordered degree of nc-Si:H films. It is found that the film deposited at −80 V shows not only high crystallinity, size of crystallite, and static index n0 but also low residual stress and volume fraction of voids. Furthermore, the microstructural evolution mechanism of nc-Si:H thin films prepared at different bias voltages is tentatively explored.  相似文献   

13.
Hydrogenated nanocrystalline silicon germanium thin films (nc-SiGe:H) is an interesting alternative material to replace hydrogenated nanocrystalline silicon (nc-Si:H) as the narrow bandgap absorber in an a-Si/a-SiGe/nc-SiGe(nc-Si) triple-junction solar cell due to its higher optical absorption in the wavelength range of interest. In this paper, we present results of optical, structural investigations and electrical characterization of nc-SiGe:H thin films made by hot-wire chemical vapor deposition (HW-CVD) with a coil-shaped tungsten filament and with a disilane/germane/hydrogen gas mixture. The optical band gaps of a-SiGe:H and nc-SiGe:H thin-films, which are deposited with the same disilane/germane/hydrogen gas mixture ratio of 3.4 : 1.7 : 7, are about 1.58 eV and 2.1 eV, respectively. The nc-SiGe:H thin film exhibits a larger optical absorption coefficient of about 2–4 in the 600–900 nm range when compared to nc-Si:H thin film. Therefore, a thinner nc-SiGe:H layer of ∼500 nm thickness may be sufficient for the narrow bandgap absorber in an a-Si based multiple-junction solar cell. We enhanced the transport properties as measured by the photoconductivity frequency mixing technique. These improved alloys do not necessarily show an improvement in the degree of structural heterogeneity on the nanometer scale as measured by smallangle X-ray scattering. Decreasing both the filament temperature and substrate temperature produced a film with relatively low structural heterogeneity while photoluminescence showed an order of magnitude increase in defect density for a similar change in the process.   相似文献   

14.
利用等离子体增强化学气相沉积技术研制出了优质稳定的氢化非晶-纳米晶两相结构硅薄膜.薄膜的光电导率相对于器件质量的非晶硅有两个数量级的提高;光敏性也较好,光、暗电导比可以达到104,此外薄膜的光电导谱具有更宽的长波光谱响应.更为重要 的是薄膜的光致退化效应远小于典型的非晶硅薄膜,在光强为50mW/cm2的卤钨灯光 照24h后,光电导的衰退小于10%.这种薄膜优良的光电性能源于薄膜中的非晶母体的存在使其在 光学跃迁中的动量选择定则发生松弛,因而具有大的光学吸收系数和 关键词: 非晶硅 微结构 光致变化  相似文献   

15.
The amorphous silicon nanoparticles (Si NPs) embedded in silicon nitride (SiNx) films prepared by helicon wave plasma-enhanced chemical vapor deposition (HWP-CVD) technique are studied. From Raman scattering investigation, we determine that the deposited film has the structure of silicon nanocrystals embedded in silicon nitride (nc-Si/SiNx) thin film at a certain hydrogen dilution amount. The analysis of optical absorption spectra implies that the Si NPs is affected by quantum size effects and has the nature of an indirect-band-gap semiconductor. Further, considering the effects of the mean Si NP size and their dispersion on oscillator strength, and quantum-confinement, we obtain an analytical expression for the spectral absorbance of ensemble samples. Gaussian as well as lognormal size-distributions of the Si NPs are considered for optical absorption coefficient calculations. The influence of the particlesize-distribution on the optical absorption spectra was systematically studied. We present the fitting of the optical absorption experimental data with our model and discuss the results.  相似文献   

16.
李同锴  徐征  赵谡玲  徐叙瑢  薛俊明 《物理学报》2017,66(19):196801-196801
采用射频等离子体增强化学气相沉积技术,利用二氧化碳(CO_2)、氢气(H_2)、硅烷(SiH_4)和乙硼烷(B_2H_6)作为气源,制备出一系列p型氢化硅氧薄膜.利用拉曼光谱、傅里叶变换红外光谱和暗电导测试,研究了不同二氧化碳流量对薄膜材料结构和光电特性的影响,获得了从纳米晶相向非晶相转变的过渡区P层.研究表明:随着二氧化碳流量从0增加到1.2 cm~3·min~(-1),拉曼光谱的峰值位置从520 cm~(-1)逐渐移至480 cm~(-1).材料红外光谱表明,随着二氧化碳流量的增加,薄膜中的氧含量逐渐增加,氢键配置逐渐由硅单氢键转换为硅双氢键.P层SiO:H薄膜电导率从3S/cm降为8.3×10~(-6)S/cm.所有p型SiO:H薄膜的光学带隙(Eopt)都在1.82—2.13 eV之间变化.在不加背反射电极的条件下,利用从纳米晶相向非晶相转变的过渡区P层作为电池的窗口层,且在P层和I层之间插入一定厚度的缓冲层,制备出效率为8.27%的非晶硅薄膜电池.  相似文献   

17.
Boron-doped nanocrystalline silicon thin films for solar cells   总被引:1,自引:0,他引:1  
This article reports on the structural, electronic, and optical properties of boron-doped hydrogenated nanocrystalline silicon (nc-Si:H) thin films. The films were deposited by plasma-enhanced chemical vapour deposition (PECVD) at a substrate temperature of 150 °C. Crystalline volume fraction and dark conductivity of the films were determined as a function of trimethylboron-to-silane flow ratio. Optical constants of doped and undoped nc-Si:H were obtained from transmission and reflection spectra. By employing p+ nc-Si:H as a window layer combined with a p′ a-SiC buffer layer, a-Si:H-based p-p′-i-n solar cells on ZnO:Al-coated glass substrates were fabricated. Device characteristics were obtained from current-voltage and spectral-response measurements.  相似文献   

18.
By using the plasma enhanced chemical vapor deposition(PECVD) technique, amorphous silicon oxide films containing nanocrystalline silicon grain(nc-Si O x:H) are deposited, and the bonding configurations and optical absorption properties of the films are investigated. The grain size can be well controlled by varying the hydrogen and oxygen content,and the largest size is obtained when the hydrogen dilution ratio R is 33. The results show that the crystallinity and the grain size of the film first increased and then decreased as R increased. The highest degree of crystallinity is obtained at R = 30.The analyses of bonding characteristics and light absorption characteristics show that the incorporation of hydrogen leads to an increase of overall bonding oxygen content in the film, and the film porosity first increases and then decreases. When R = 30, the film can be more compact, the optical absorption edge of the film is blue shifted, and the film has a lower activation energy.  相似文献   

19.
Hydrogenated nanocrystalline silicon (nc-Si:H) thin films were deposited using HW-CVD technique at various deposition pressures. Characterisation of these films from Raman spectroscopy revealed that nc-Si:H thin films consist of a mixture of two phases, crystalline phase and amorphous phase containing small Si crystals embedded therein. We observed increase in crystallinity in the films with increase in deposition pressure whereas the size of Si nanocrystals was found ∼2 nm over the entire range of deposition pressure studied. The FTIR spectroscopic analysis showed that with increasing deposition pressure the predominant hydrogen bonding in the films shifts from, Si-H to Si-H2 and (Si-H2)n complexes and the hydrogen content in the films was found in the range 6.2-9.3 at% over the entire range of deposition pressure studied. The photo and dark conductivities results also indicate that the films deposited with increasing deposition pressure get structurally modified. It has been found that the optical energy gap range was between 1.72 and 2.1 eV with static refractive index between 2.85 and 3.24. From the present study it has been concluded that the deposition pressure is a key process parameter to induce the crystallinity in the Si:H thin films using HW-CVD.  相似文献   

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