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31.
Evolution of the structural and optical properties of silver oxide films with different stoichiometries deposited by direct-current magnetron reactive sputtering
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Nitrogen doping of silver oxide(AgxO) film is necessary for its application in transparent conductive film and diodes because intrinsic AgxO film is a p-type semiconductor with poor conductivity.In this work,a series of AgxO films is deposited on glass substrates by direct-current magnetron reactive sputtering at different flow ratios(FRs) of nitrogen to O2.Evolutions of the structure,the reflectivity,and the transmissivity of the film are studied by X-ray diffractometry and sphectrophotometry,respectively.The specular transmissivity and the specular reflectivity of the film decreasing with FR increasing can be attributed to the evolution of the phase structure of the film.The nitrogen does not play the role of an acceptor dopant in the film deposition. 相似文献
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陷光是改善薄膜太阳电池光吸收进而提高其效率的关键技术之一. 以非晶硅(α-Si)薄膜太阳电池为例,设计了一种新的复合陷光结构:在Ag背电极与硅薄膜之间制备一维Ag纳米光栅,并通过保形生长在电池前表面沉积织构的减反膜. 采用有限元数值模拟方法,研究了该复合陷光结构对电池光吸收的影响,并对Ag纳米光栅的结构参数进行了优化. 模拟结果表明:该复合陷光结构可在宽光谱范围内较大地提高太阳电池的光吸收;当Ag纳米光栅的周期P为600 nm,高度H为90 nm,宽度W为180 nm时,在AM1.5光谱垂直入射条件下α-Si薄膜电池在300–800 nm波长范围内总的光吸收较无陷光结构的参考电池提高达103%,其中在650–750 nm长波范围内的光子吸收率提高达300%以上. 结合电场强度分布,对电池在各个波段光吸收提高的物理机制进行了分析. 另外,该复合陷光结构的引入,还较大地改善了非晶硅电池对太阳光入射角度的敏感性.
关键词:
非晶硅太阳电池
陷光
银纳米光栅
数值模拟 相似文献
35.
采用水热法在普通载玻片上热解醋酸锌生成的ZnO种子层上制备ZnO纳米棒, 采用 X射线衍射仪、扫描电镜、分光光度计等测试手段详细研究了醋酸锌热解温度对 ZnO纳米棒的结构和光学性质的影响. 结果表明: 纳米棒的结晶质量、端面尺寸、宏观应力和透射率与醋酸锌热解温度有密切关系. 随着热解温度的增加, ZnO纳米棒具有的c轴择优取向性先增强后减弱, 拉应力先减小后增大, 可见光区的平均透射率先增大后减小. 热解温度为350 ℃时, ZnO纳米棒c轴择优取向性最强, 拉应力最小, 平均透射率最大. 端面尺寸诱导的表面散射 是影响ZnO纳米棒可见光区平均透射率的主要机制.
关键词:
醋酸锌
水热法
ZnO纳米棒 相似文献
36.
Microcrystalline silicon (μc-Si:H) thin films with and without boron doping are deposited using the radio-frequency plasma-enhanced chemical vapour deposition method. The surface roughness evolutions of the silicon thin films are investigated using ex situ spectroscopic ellipsometry and an atomic force microscope. It is shown that the growth exponent β and the roughness exponent α are about 0.369 and 0.95 for the undoped thin film, respectively. Whereas, for the boron-doped μc-Si:H thin film, β increases to 0.534 and α decreases to 0.46 due to the shadowing effect. 相似文献
37.
Effects of the sputtering power on the crystalline structure and optical properties of the silver oxide films deposited using direct-current reactive magnetron sputtering
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This paper reports that a series of silver oxide (AgxO) films are deposited on glass substrates by direct-current reactive magnetron sputtering at a substrate temperature of 250 oC and an oxygen flux ratio of 15:18 by modifying the sputtering power (SP). The AgxO films deposited apparently show a structural evolution from cubic biphased (AgO + Ag2O) to cubic single-phased (Ag2O), and to biphased (Ag2O + AgO) structure. Notably, the cubic single-phased Ag2O film is deposited at the SP = 105 W and an AgO phase with <220> orientation discerned in the AgxO films deposited using the SP > 105 W. The transmissivity and reflectivity of the AgxO films in transparent region decrease with the increase the SP, whereas the absorptivity inversely increases with the increase of the SP. These results may be due to the structural evolution and the increasing film thickness. A redshift of the films' absorption edges determined in terms of Tauc formula clearly occurs from 3.1 eV to 2.73 eV with the increase of the SP. 相似文献
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采用分子动力学方法模拟不同压强下液态InGaAs的快速凝固过程,并采用双体分布函数、键角分布函数、配位数统计以及可视化等方法,从微观结构的不同层面分析了压强对凝固过程微观结构的影响机制。结果表明:对于InGaAs体系,压强对最近邻和次近邻的原子排布都有影响,但对次近邻原子排列的影响更为明显,通过次近邻原子键角的调整,使得原子排列更加紧密,体系的短程有序度增强。在原子的配位数结构上,随着压强的增加,部分三配位向四配位发生转变,从而使整个体系达到致密的结构。 相似文献
39.
The high deposition of microcrystalline silicon thin film by very high frequency plasma enhanced
chemical vapour deposition and the fabrication of solar cells
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This paper reports that the intrinsic microcrystalline silicon ($\mu
$c-Si:H) films are prepared with plasma enhanced chemical vapour
deposition from silane/hydrogen mixtures at 200\du\ with the aim to
increase the deposition rate. An increase of the deposition rate to
0.88\,nm/s is obtained by using a plasma excitation frequency of
75\,MHz. This increase is obtained by the combination of a higher
deposition pressure, an increased silane concentration, and higher
discharge powers. In addition, the transient behaviour, which can
decrease the film crystallinity, could be prevented by filling the
background gas with Hchemical vapour deposition,
plasma deposition, solar cells, crystallinity Program supported by the State Key
Development Program for Basic Research of China (Grant No
2006CB202601), and Basic Research Project of Henan Province in China
(Grant No 072300410140). 7280N, 7830G, 8115H This paper reports that the intrinsic microcrystalline silicon ($\mu
$c-Si:H) films are prepared with plasma enhanced chemical vapour
deposition from silane/hydrogen mixtures at 200\du\ with the aim to
increase the deposition rate. An increase of the deposition rate to
0.88\,nm/s is obtained by using a plasma excitation frequency of
75\,MHz. This increase is obtained by the combination of a higher
deposition pressure, an increased silane concentration, and higher
discharge powers. In addition, the transient behaviour, which can
decrease the film crystallinity, could be prevented by filling the
background gas with Hchemical vapour deposition,
plasma deposition, solar cells, crystallinity Program supported by the State Key
Development Program for Basic Research of China (Grant No
2006CB202601), and Basic Research Project of Henan Province in China
(Grant No 072300410140). 7280N, 7830G, 8115H This paper reports that the intrinsic microcrystalline silicon ($\mu
$c-Si:H) films are prepared with plasma enhanced chemical vapour
deposition from silane/hydrogen mixtures at 200\du\ with the aim to
increase the deposition rate. An increase of the deposition rate to
0.88\,nm/s is obtained by using a plasma excitation frequency of
75\,MHz. This increase is obtained by the combination of a higher
deposition pressure, an increased silane concentration, and higher
discharge powers. In addition, the transient behaviour, which can
decrease the film crystallinity, could be prevented by filling the
background gas with Hchemical vapour deposition,
plasma deposition, solar cells, crystallinity Program supported by the State Key
Development Program for Basic Research of China (Grant No
2006CB202601), and Basic Research Project of Henan Province in China
(Grant No 072300410140). 7280N, 7830G, 8115H This paper reports that the intrinsic microcrystalline silicon ($\mu
$c-Si:H) films are prepared with plasma enhanced chemical vapour
deposition from silane/hydrogen mixtures at 200\du\ with the aim to
increase the deposition rate. An increase of the deposition rate to
0.88\,nm/s is obtained by using a plasma excitation frequency of
75\,MHz. This increase is obtained by the combination of a higher
deposition pressure, an increased silane concentration, and higher
discharge powers. In addition, the transient behaviour, which can
decrease the film crystallinity, could be prevented by filling the
background gas with Hchemical vapour deposition,
plasma deposition, solar cells, crystallinity Program supported by the State Key
Development Program for Basic Research of China (Grant No
2006CB202601), and Basic Research Project of Henan Province in China
(Grant No 072300410140). 7280N, 7830G, 8115H This paper reports that the intrinsic microcrystalline silicon ($\mu
$c-Si:H) films are prepared with plasma enhanced chemical vapour
deposition from silane/hydrogen mixtures at 200\du\ with the aim to
increase the deposition rate. An increase of the deposition rate to
0.88\,nm/s is obtained by using a plasma excitation frequency of
75\,MHz. This increase is obtained by the combination of a higher
deposition pressure, an increased silane concentration, and higher
discharge powers. In addition, the transient behaviour, which can
decrease the film crystallinity, could be prevented by filling the
background gas with H$_{2}$ prior to plasma ignition, and selecting
proper discharging time after silane flow injection. Material
prepared under these conditions at a deposition rate of 0.78\,nm/s
maintains higher crystallinity and fine electronic properties. By
H-plasma treatment before i-layer deposition, single junction $\mu
$c-Si:H solar cells with 5.5{\%} efficiency are fabricated. 相似文献
40.