共查询到19条相似文献,搜索用时 31 毫秒
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报道了以正硅酸乙酯(TEOS)为源,采用等离子体增强化学汽相淀积(PECVD)技术在InP表面低温生长SiO2钝化膜。对SiO2/InP界面态进行了X射线光谱(XPS)分析和C-V特性研究。 相似文献
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夏祥;陆红波;马超;刘雪连;邱龙臻;徐苗;朱俊;张国兵 《液晶与显示》2021,36(9):1247-1254
本文探究了单体与液晶的相容性对聚合物墙表面组成的影响和表面组成对聚合物墙液晶器件光电性能的影响及其调控方法。选取与液晶相容性相差较大但表面能相近的单体,通过表面引发聚合形成与液晶分层的聚合物薄膜,洗去液晶后用反应离子刻蚀在聚合物表面刻蚀出不同深度。通过衰减全反射红外光谱和X射线光电子能谱仪表征不同深度的组分。最后利用掩模版制备聚合物墙液晶器件,并探究聚合墙表面组成对其光电性能的影响。实验结果表明:在聚合物-液晶界面处富集与液晶相容性高的聚合物组分,并且聚合光强越低,这种组分偏析效果越明显,当聚合光强较低时,聚合物表面组成中的PTFEMA组分占比为68.5%,比高光强时的多出10.6%。聚合物墙的表面组成对液晶器件的光电性能有一定的影响,当光强为10mW/cm2时器件的阈值电压为0.879V,而在70mW/cm2光强时升高到1.172V。可以利用单体与液晶的相容性差异以及光强调控聚合物墙表面组成,进而影响液晶器件的光电性能。 相似文献
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表面活性剂对聚合物分散液晶光电性能的影响 总被引:1,自引:0,他引:1
为了调控聚合物分散液晶(PDLC)中聚合物基体和液晶微滴的界面作用,降低锚定能,以聚丙烯酸甲酯(PMA)为基体,E7为分散相,并加入了不同含量的硬脂酸(SA)表面活性剂,采用聚合物诱导相分离法制备了PDLC,并对PDLC的光电性能进行了测试。研究发现,PDLC的电光性能随着SA含量的增加而改善,但当SA的含量达到一定值后,液晶微滴出现\"岛聚\"现象,光电曲线出现一个转折点。实验结果表明,表面活性剂可以调控聚合物和液晶微滴的界面作用,降低锚定能,从而改善PDLC的光电性能。 相似文献
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Au/Zn/Au/p-In P欧姆接触的界面研究 总被引:2,自引:0,他引:2
研究了离子束溅射制备的Au/Zn/Au/p-InP欧姆接触的界面特性.在480℃退火15s比接触电阻达到最小,为1.4×1 0-5 Ω·cm 2.利用俄歇电子能谱(AES)和X射线光电子能谱(XPS)研究了接触界面的冶金性质.实验结果表明,在室温下InP中的In就可以扩散到接触的表面,退火后可与Au形成合金.退火后,Zn的扩散可以在p-InP表面形成重掺杂层,从而降低接触势垒高度,减小势垒宽度,有助于欧姆接触的形成;在接触与p-InP的界面产生一个P聚集区,同时Au与InP反应生成Au2P3,其P的2p3/2电子的结合能约为129.2 eV. 相似文献
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光电探测器能将光辐照转换为电信号,是光电系统中接收端的核心部件,在国民经济、警用装备以及诸多军事领域都有着重要的应用。基于传统材料的光电探测器面临性能不够优越、单个探测器检测范围窄等问题。近年来,低维半导体和钙钛矿材料在光电探测器领域引起研究人员的广泛关注。相较单一材料,基于低维半导体/钙钛矿异质结构的光电探测器在光响应度、外量子效率、探测率以及响应时间上都有着更为优越的性能,逐渐成为研究热点。简述了光电探测器的基本性质以及钙钛矿材料常见的制备方法,进一步介绍了国内外关于低维半导体/钙钛矿异质结构光电探测器的主要研究进展,探讨了目前优化性能的主要措施,最后对发展前景进行了展望,并提出了相关建议。 相似文献
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全无机CsPbBr3钙钛矿太阳能电池中的电荷传输层与钙钛矿层界面的载流子复合是制约其光电转换效率进一步提升的关键因素。文中采用带隙和带边可调控的二维过渡金属硫族化合物(MoS2、MoSe2、WS2和WSe2)材料作为电子传输层和钙钛矿层之间的界面修饰材料和载流子传输材料,利用晶格匹配的范德华外延生长高质量的钙钛矿薄膜,同时通过界面能级补偿和势垒消减,降低钙钛矿层与电子传输层之间的界面电荷损失,促进全无机CsPbBr3钙钛矿太阳能电池器件中载流子的提取与传输,使器件光电转换效率由初始的7.94%提高到10.02%,同时开路电压从1.474 V提升至1.567 V。该研究为制备高质量的钙钛矿薄膜同时实现界面能级匹配的高性能光电器件提供了一条新途径。 相似文献
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王凯宇;白龙飞;谢丽娟;高冬宁;闫旭东;余辉;袁冬 《液晶与显示》2022,37(8):1095-1103
当前聚合物稳定液晶器件的光电响应特性尚未完全满足智能窗的实用需求。材料的自身特性是决定液晶器件性能的关键,因此本文重点研究了负性液晶材料的介电各向异性和双折射率两项核心参数对聚合物稳定液晶器件光电响应特性的影响趋势,并给出对应的最佳参数。本文采用实验和仿真相结合的研究方法,首先选用具有不同参数的负性液晶材料制备聚合物稳定液晶器件,研究分析介电各向异性对器件光电性能的影响。然后通过仿真模拟,研究负性液晶材料的双折射率对器件光电效应的影响。最后通过实验和仿真结果的综合分析得出最佳负性液晶参数。研究结果表明,介电各向异性越大,液晶分子越容易被电场驱动,液晶器件的光电性能也就越好。在固定聚合物稳定网络双折射率的情况下,当负性液晶的双折射参数为n e=1.49、n o=1.593时,可达到最优雾度。这一研究结果可为聚合物稳定液晶器件性能的优化及产业化的发展提供理论指导。 相似文献
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不同单体配比对聚合物网络及聚合物稳定胆甾相液晶器件光电性能的影响 总被引:1,自引:1,他引:0
为了调节聚合物网络与液晶分子之间的相互作用,从而改善聚合物稳定胆甾相液晶(PSCLC)的光电性能,本文采用紫外光聚合诱导相分离法(PIPS)制备了聚合物稳定胆甾相液晶,通过控制2种单体RM257与BAB6的比例来改善器件性能。随着RM257含量的减少,聚合物网络由取向排列的纤维状结构向疏松不规整的交联状结构转变,形成的聚合物网络对液晶分子的锚定作用减弱,聚合物稳定胆甾相液晶的饱和电压降低,关闭时间增大。当RM257与BAB6质量比为1:4时,聚合物稳定胆甾相液晶器件具有较好的对比度。 相似文献
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This paper describes a simple approach for reducing the contact resistances at the source/drain (S/D) contacts in solution-processed n-channel organic thin-film transistors (OTFTs). Blending poly(ethylene glycol) (PEG) into the fullerene semiconducting layer significantly improved the device performance. The PEG molecules in the blends underwent chemical reactions with the Al atoms of the electrodes, thereby forming a better organic-metal interface. Further, the rougher surface obtained after the addition of PEG could also increase the effective contact area, thereby reducing the resistance. As a result, the electrical properties of the devices were significantly improved. Unlike conventional bilayer structures, this approach allows the ready preparation of OTFTs with a low electron injection barrier at the S/D contacts. 相似文献
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《Organic Electronics》2014,15(4):858-863
The use of appropriate charge carrier transport materials in organic solar cells strongly influences the device performance. In this work, we focused on the molecular electron transport material 1,4,5,8-naphthalene-tetracarboxylic-dianhydride (NTCDA) doped by cesium carbonate (Cs2CO3). We first investigated the electrical properties of such n-type doped material as a function of the doping concentration before using it as electron transport layer (ETL) in polymer solar cells. The doped transparent ETL reduces the series resistance leading to an increased open circuit voltage. A power conversion efficiency of 3.8% was finally achieved in a device with a blend of poly(3-hexylthiophene-2,5-diyl):phenyl-C61-butyric acid methyl ester (P3HT:PCBM) as the active layer and a 5 nm-thick NTCDA:Cs2CO3 film with a molar ratio of 30% as ETL. 相似文献
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In this study, to adjust the desired molecular energy levels and bandgap energies of polymers for photovoltaic applications, a regular terpolymer structure was designed. A new regular terpolymer, poly(DPP4T-alt-TBP), containing diketopyrrolopyrrole (DPP), BT, and BP units in the repeating group was successfully synthesized. The DPP-BT monomeric unit in polymer backbone enhanced chain packing and induced a high-lying highest occupied molecular orbital (HOMO) level and the DPP-BP segment induced a deeper HOMO level. The lowest unoccupied molecular orbital (LUMO) level of the terpolymer was also controlled in a similar manner. The HOMO level of the terpolymer was similar to that of poly(DPP-alt-BP), and the energies of the LUMOs were governed by the DPP-BT unit. The polymer chain arrangement of the terpolymer on the substrate was observed to be a mix of face-on and edge-on orientations, which is a different chain arrangement mode to those shown in both poly(DPP-alt-BP) and poly(DPP-alt-BT). A TFT fabricated with poly(DPP4T-alt-TBP) had a charge carrier mobility of 0.59 cm2 V−1 s−1 and a moderately high current on/off ratio. Furthermore, a polymer solar cell containing the terpolymer and PC71BM had a power conversion efficiency of 4.54%, which is significantly higher than those of the PCEs of poly(DPP-alt-BP) and poly(DPP-alt-BT)-based solar cells with identical device configurations. 相似文献
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Kaname Kanai Masato HondaHisao Ishii Yukio OuchiKazuhiko Seki 《Organic Electronics》2012,13(2):309-319
We present an investigation of the interface between organic semiconductor films and metal substrates (organic/metal interface) using photoelectron yield spectroscopy (PYS) as the probing technique. PYS studies were conducted on the pentacene/Au, copper phthalocyanine (CuPc)/Au, and perfluorinated zinc phthalocyanine (F16ZnPc)/Au, and the results were compared with literature results obtained using conventional ultraviolet photoemission spectroscopy (UPS). PYS is advantageous for probing the electronic structure of the organic/metal interface because of the relatively long mean free path of photoexcited electrons with very low kinetic energy in PYS, which enables the detection of the photoelectrons from the metal substrate buried deep in the organic film. We demonstrate herein that the use of PYS reduces the significance of the final state effect of the electronic density surrounding the photohole at the organic molecule generated after the photoemission; this effect is known as the electric polarization effect. Although this effect has a significant influence on the results obtained using conventional UPS, the reduced influence of the final state effect in PYS makes it possible to construct an energy level diagram at the organic/metal interface with greater accuracy than can be achieved with UPS. In addition, a novel mechanism of the photoelectron detection for PYS enables us to apply PYS to very thick organic films, and therefore, PYS provides a reliable value of ionization energy for organic films without the influence of the substrate.Because the interface electronic structure has a significant influence on the carrier injection properties of organic devices, the increased reliability of the information obtained by PYS will render it very useful for the improvement of device performance as well for understanding their operation principles. 相似文献
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Noriyuki Miyata Hiroyuki IshiiYuji Urabe Taro ItataniTetsuji Yasuda Hisashi YamadaNoboru Fukuhara Masahiko HataMomoko Deura Masakazu SugiyamaMitsuru Takenaka Shinichi Takagi 《Microelectronic Engineering》2011,88(12):3459-3461
Electrical and physical characteristics of the Al2O3/InGaAs interfaces with (1 1 1)A and (1 0 0) orientations were investigated in an attempt to understand the origin of electron mobility enhancement in the (1 1 1)A-channel metal-insulator-semiconductor field-effect-transistor. The (1 1 1)A interface has less As atoms of high oxidation states as probed by X-ray photoelectron spectroscopy. The electrical measurements showed that energy distribution of the interface traps for the (1 1 1)A interface is shifted toward the conduction band as compared to that for the (1 0 0) interface. Laterally-compressed cross-section transmission electron microscopy images showed that the characteristic lengths of the interface roughness are different between the (1 1 1)A and (1 0 0) interfaces. The contributions of the Coulomb and roughness scattering mechanisms are discussed based on the experimental results. 相似文献