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多晶硅薄膜

多晶硅薄膜的相关文献在1973年到2022年内共计820篇,主要集中在无线电电子学、电信技术、物理学、电工技术 等领域,其中期刊论文219篇、会议论文87篇、专利文献236164篇;相关期刊101种,包括材料导报、功能材料、太阳能学报等; 相关会议45种,包括第13届中国光伏大会、第十一届中国光伏大会暨展览会、中国硅酸盐学会特种玻璃分会第三届全国特种玻璃会议等;多晶硅薄膜的相关文献由1189位作者贡献,包括许颖、田雪雁、赵淑云等。

多晶硅薄膜—发文量

期刊论文>

论文:219 占比:0.09%

会议论文>

论文:87 占比:0.04%

专利文献>

论文:236164 占比:99.87%

总计:236470篇

多晶硅薄膜—发文趋势图

多晶硅薄膜

-研究学者

  • 许颖
  • 田雪雁
  • 赵淑云
  • 黄宇华
  • 黄飚
  • 孟志国
  • 熊绍珍
  • 郭海成
  • 龙春平
  • 卢景霄
  • 期刊论文
  • 会议论文
  • 专利文献

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    • 路爽; 张一凡
    • 摘要: 高温沉积方法制备多晶硅薄膜太阳电池具有电池效率高、制备成本低等优势,在光伏太阳能电池领域具有良好的发展前景。介绍了不同材料衬底制备高温沉积法制备多晶硅太阳能光伏薄膜的方法,介绍了多晶硅薄膜太阳能电池的基本特点和制备工艺的技术要点,并综述了当前多晶硅薄膜太阳能电池面临的重点以及相关的前沿研究领域的最新进展。
    • 柴甜甜
    • 摘要: 众所周知,能源驱动城市发展,然而随着传统能源日渐枯竭以及全球环境污染逐日加剧,人类迫切需要寻找新型可再生能源以驱动城市发展.因此,发展可再生能源已成为我国能源结构转型和缓解气候恶化的关键途径.科学研究表明,太阳能发电是一种清洁可再生的能源利用方案,具有"取之不尽,用之无竭"的优点.目前已商用化的晶体硅太阳能电池的光电转化效率最高,但受材料纯度和制备工艺的限制,晶体硅太阳能电池很难在提高光电转化效率的同时降低生产成本.于是,硅基薄膜太阳能电池的问世无疑是一道曙光——薄膜太阳能电池只需几微米的吸光层就能实现高效率光电转换,可以在降低生产成本的同时提高光电转化效率,具有生产成本低、硅材消耗少、光电转换效率高的无可比拟优势.
    • 郑春生; 刘德杰; 曾磊
    • 摘要: 多晶硅薄膜在集成电路制造以及半导体器件制造等相关领域中有着非常广泛的应用价值,制备工艺近年来发展速度不断加快,使得多晶硅薄膜在相关行业领域中的应用前景更为广阔.本文即以化学气相沉积法为重点,针对多晶硅薄膜的制备工艺与反应原理进行了分析,并简要介绍了多晶硅薄膜的应用与发展前景,望能够引起业内有关人员的重视与关注.
    • 郑春生1; 刘德杰2; 曾磊2
    • 摘要: 多晶硅薄膜在集成电路制造以及半导体器件制造等相关领域中有着非常广泛的应用价值,制备工艺近年来发展速度不断加快,使得多晶硅薄膜在相关行业领域中的应用前景更为广阔。本文即以化学气相沉积法为重点,针对多晶硅薄膜的制备工艺与反应原理进行了分析,并简要介绍了多晶硅薄膜的应用与发展前景,望能够引起业内有关人员的重视与关注。
    • 王帅; 刘敏; 潘岭峰; 张紫辰; 王晓峰; 杨富华
    • 摘要: Compared with amorphous silicon thin film,polysilicon thin film has higher electron mobility and shows better electrical properties in the device.The method of preparing polycrystalline silicon thin film by pulsed laser crystallization of amorphous silicon thin film has the advantages of low thermal budget,little influence on the substrate and low cost.An experiment about laser crystallization of amorphous silicon thin films was carried out by using 532nm solid state nanosecond laser.To solve the problem of nonuniform effect when using Gaussian beam crystallization of amorphous silicon thin film,the circular Gauss beam was transformed into a linear flat top beam based on the beam shaping system.Then the effect of single pulse energy density,pulse number and thickness of amorphous silicon thin film on the crystallization of amorphous silicon thin film was investigated.The experimental results show that,linear flat top beam show better uniformity about laser crystallization of amorphous silicon thin film.For the 100nm amorphous silicon thin film crystal,with the increase of energy density,the grain becomes larger,until the surface is thermally damaged,and the largest grain size is about 1 μm × 500nm.And as the number of pulses increases,the surface roughness tends to decrease,and the minimum surface roughness is 2.38 nm.For 20 nm uhra-thin amorphous silicon film,only when the energy density is between 134mJ/cm2 and 167mJ/cm2,and the number of pulses is more than or equal to 8,the obvious crystallization effect can be observed.%多晶硅薄膜比非晶硅薄膜具有更高的电子迁移率,在器件中表现出更优良的性能,脉冲激光结晶非晶硅薄膜制备多晶硅薄膜的方法具有热积存小、对衬底影响小、成本低等优点.使用532 nm固体纳秒激光器进行了非晶硅薄膜激光结晶实验,为了解决直接使用高斯光束结晶时因光斑能量分布带来的结晶效果不均匀,首先基于光束整型系统将圆形的高斯光束整型成为线性平顶光束,而后研究单脉冲能量密度、脉冲个数、非晶硅薄膜厚度对结晶效果的影响.结果表明,线性平顶光束用于非晶硅薄膜结晶具有更好的均匀性,对于100 nm非晶硅薄膜,随着能量密度的增加,晶粒逐渐变大,直到表面出现热损伤,最大晶粒尺寸约为1 μm×500 nm.随着脉冲个数的增加,表面粗糙度有减小的趋势,观察到的最小粗糙度约为2.38 nm.对于20nm超薄非晶硅薄膜,只有当能量密度位于134 mnJ/cm2和167 mJ/cm2之间、脉冲个数大于或等于八个时才能观察到明显的结晶效果.
    • 王思源; 王宙; 付传起; 骆旭梁; 张英利
    • 摘要: 采用脉冲激光沉积法(PLD)制备磷掺杂多晶硅薄膜,研究磷掺杂分数对多晶硅薄膜压阻性能的影响.结果表明,随着磷掺杂分数增大,多晶硅薄膜的应变系数先增大后减小.在磷掺杂分数为0.3%(质量分数)时,电阻横向应变系数的绝对值达到最大,为24.3,电阻纵向应变系数的绝对值达到最大,为12.6.横向电阻应变的非线性在1%~2.5%之间,电阻的温度系数为0.05%/°C,应变系数的温度系数为-0.06%/°C.%In this paper,the polycrystalline silicon thin film was prepared on a quartz glass substrate by the PLD(pulsed laser deposition)method,and the effect of phosphorus content on piezoresistive properties of polycrystalline silicon thin film was studied. The results show that with the increase of phosphorus content,the gauge factor of polycrystalline silicon thin film showed a trend of decrease after the first increase.When the phosphorus doping fraction was 0.3wt%,the maximum gauge factors of longitudinal and transverse were 12.6 and 24.3. The nonlinearity of transverse was 1%—2.5%,the temperature coefficient of resistance and the temperature coefficient of gauge factor were 0.05%/°C and -0.06%/°C.
    • 邓幼俊; 艾斌
    • 摘要: 多晶硅薄膜已广泛应用于平板显示、微机电系统和集成电路等领域,在太阳电池和平板系统领域也有着巨大的应用前景.由于多晶硅薄膜存在晶界,晶界内的晶体缺陷和悬挂键会向带隙中引入界面态,界面态一方面会束缚载流子并形成势垒阻碍载流子的传输,另一方面会作为有效复合中心加重载流子的复合,因此,多晶硅薄膜上制备的器件的性能要低于与之对应的单晶硅薄膜器件的性能.为了从理论上阐明暗场和光照条件下多晶硅薄膜的电学性质,人们已发展了各种理论模型.此外,为了确定晶界界面态在带隙中的分布,人们已发展出分析法和计算机模拟两种方法.本文将简要概述人们在多晶硅薄膜电学输运理论和晶界界面态分布确定方法等方面的主要研究进展,以期对从事多晶硅薄膜或多晶半导体输运性质研究的科研工作者有所参考和启发.%Polycrystalline silicon (poly-Si) thin films have been widely used in flat panel displays,MEMS(micro-electro-mechanical system) and integrated circuits,and also have great application prospects in other areas such as solar cells and SOP (system on panel).Since there exist grain boundaries (GBs) in poly-Si thin films,the crystal defects and dangling bonds in GB regions would introduce interface states in the band gap.On the one hand,the interface states would trap carriers thus creating barriers against carrier transportation,on the other hand,they could act as effective recombination centers to strengthen the recombination.Therefore,the performance of devices fabricated on poly-Si thin films is generally worse than that on single-crystal silicon thin films.To give a theoretical explanation on the electrical properties of poly-Si thin films under the dark and illumination conditions,various theoretical models have been proposed.In addition,two kinds of ways including analytical method and computer simulation have been developed to determine the energy distribution of interface states in the band gap.This article will briefly review the major research progress in electrical transport theory of poly-Si films and methods for determining the distribution of the interface states,so that researchers engaging in investigation on transport properties of poly-Si thin films or polycrystalline semiconductors could get some reference and inspiration.
    • 王健; 揣荣岩
    • 摘要: 多晶硅薄膜具有良好的压阻特性,晶粒结构和掺杂浓度决定其压阻特性.一般通过调节掺杂浓度改变压阻参数,但现有的多晶硅薄膜压阻系数与掺杂浓度的理论关系和适用范围不够全面.为了完善多晶硅薄膜压阻理论,基于多晶硅纳米薄膜隧道压阻模型,以及硅价带和空穴电导质量随应力改变的机理,提出了一种p型多晶硅薄膜压阻系数算法.该算法分别求取了晶粒中性区和复合晶界区的压阻系数π11,π12和π44的理论公式,据此可以计算任意择优晶向排列多晶硅的纵向和横向压阻系数.根据材料的结构特性,求取了p型多晶硅纳米薄膜和普通多晶硅薄膜应变因子,绘制了应变因子与掺杂浓度的关系曲线,与测试结果比较,具有较好的一致性.因此,该算法全面和准确,对多晶硅薄膜的压阻特性的改进和应用具有重要意义.%The polysilicon thin film piezoresistors are widely used in semiconductor pressure sensors. The polysilicon thin film has good piezoresistance properties, which are determined by the grain structure and doping concentration. The gauge factor of the polysilicon thin film is usually modified according to the relationship between gauge factor and doping concentration. The polysilicon thin films are classified into common polysilicon thin films and polysilicon nanofilms ac-cording to their thickness. The common polysilicon thin film thickness is more than 0.3 μm, which has good temperature characteristic, but its piezoresistance coefficient is small. However, the polysilicon nanofilm thickness is less than 0.1 μm, which has good temperature characteristic and high piezoresistance coefficient. The existing piezoresistance theory of the common polysilicon thin film cannot explain reasonably the experimental result of polysilicon nanofilm piezoresistance. Therefore, the tunneling piezoresistance model and an algorithm for the p-type polysilicon nanofilm piezoresistance coef-ficient were established in 2006. However, this algorithm presents an incomplete fundamental piezoresistance coefficient. In order to improve the polysilicon thin film piezoresistance theory, based on the tunneling piezoresistance model and the mechanism of silicon and the valence band hole conductivity mass with the change of stress, a novel algorithm for the piezoresistance coefficient of the p-type polysilicon thin film is presented. The theoretical formulas for three fundamental piezoresistance coefficientsπ11,π12 andπ44 of the grain neutral and grain boundary regions, are presented respectively. With these formulas for the coefficients, the longitudinal and transverse piezoresistance coefficients for arbitrary crystal direction texture polysilicon can be obtained. According to the structure characteristics, the gauge factors of the p-type polysilicon nanofilm and the common polysilicon thin film are calculated, and then the longitudinal and transverse gauge factors are plotted each as a function of doping concentration, which are compared with the experimental results. Ac-cording to the experimental results of the polysilicon nanofilm, the grain size is L=30 nm, the grain crystal directions are randomly distributed. The trap density in grain boundary region is Nt=1013 cm-2, the Young's modulus of elastic diaphragm is Y = 1.69 × 1011 Pa, the Poisson ratio of elastic diaphragm is ν = 0.062, the grain boundary width isδ=1 nm, and the thickness is 80 nm. The comparison indicates that the gauge factor average error between calculation and experiment is 0.5 times less than the average experimental difference between the maximum and the minimum for each doping concentration. For the common polysilicon thin film, according to the experimental results, its grain size L is 135 nm, thickness is 400 nm, the orientations of crystal grain neutral region are [311], [111] and [110] in the ratio of 49:31:20, i.e., 〈311〉:〈111〉:〈110〉=49:31:20, and the gauge factor calculated result is also good agreement with the experimental result. Therefore, the proposed algorithm is comprehensive and accurate, which is applicable to the p-type common polysilicon film and the polysilicon nanofilm.
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