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1.
Thin organic films were deposited on silicon oxide surfaces with golden interdigitated electrodes (interelectrode gap was 2 μm), and the film resistivities were measured in dark and under white light illumination. The compounds selected for the measurements include molecules widely used in solar cell applications, such as polythiophene (PHT), fullerene (C60), pyrelene tetracarboxylic diimide (PTCDI) and copper phthalocyanine (CuPc), as well as molecules potentially interesting for photovoltaic applications, e.g. porphyrin-fullerene dyads. The films were deposited using thermal evaporation (e.g. for C60 and CuPc films), spin coating for PHT, and Langmuir-Schaeffer for the layer-by-layer deposition of porphyrin-fullerene dyads. The most conducting materials in the series are films of PHT and CuPc with resistivities 1.2 × 103 Ω m and 3 × 104 Ω m, respectively. Under light illumination resistivity of all films decreases, with the strongest light effect observed for PTCDI, for which resistivity decreases by 100 times, from 3.2 × 108 Ω m in dark to 3.1 × 106 Ω m under the light.  相似文献   

2.
In this work we report on the capability of polarized Raman spectroscopy to investigate the structure of thin organic films. Diindenoperylene (DIP) thin films on (1 × 1)‐rutile(110) were prepared via organic molecular beam deposition (OMBD). Raman spectra of DIP thin films showed several strong Raman modes in the wavenumber region from 1200 to 1650 cm−1. The Ag mode at 1284 cm−1 shows two contributions, thereby indicating the coexistence of at least two DIP film structures. Polarized Raman spectroscopy was applied to characterize the molecular orientation and the dominance of the σ‐configuration (i.e. upright standing DIP molecules) was found. Copyright © 2009 John Wiley & Sons, Ltd.  相似文献   

3.
蒋益明  谢亨博  郭峰  刘平  李劲 《物理学报》2005,54(12):5769-5773
采用真空热蒸发方法在玻璃基板上蒸镀不同厚度的Ag/TCNQ(7,7,8,8-tetracyanoquinodimethane)双层膜.通过固体化学反应扩散,最终形成Ag-TCNQ络合物.利用透射光谱表征,研究了双层膜中的传质规律.按电子隧穿条件满足与否分别建立了隧穿模型和非隧穿模型对体系传质过程进行了理论分析,理论分析与实验结果相符.  相似文献   

4.
Polarization‐dependent Raman microscopy is a powerful technique to perform both structural and chemical analyses with submicron spatial resolution. In conventional Raman microscopy, the polarization measurements are limited only in the direction parallel to the sample plane. In this work, we overcome the limit of conventional measurements by controlling the incident polarization by a spatially modulated waveplate. In this method, the polarization perpendicular to the sample surface (z‐polarization) can be detected together with the parallel polarization (xy‐polarization). Because of this unique polarization control, our Raman microscope has the ability to image the molecular orientation, together with the molecular analysis. Here, we have investigated thin films of pentacene molecules that are widely studied as an organic semiconductor material. The orientations of pentacene molecules are imaged with a spatial resolution of 300 nm. Our results clearly indicate that the lamellar grains show the lower tilt angles compared to the neighboring islands, which has not been proved in conventional methods. The substrate effects and the thickness dependence of the film are also studied. These results provide knowledge about the relationship between the devise performance and the film structures, which is indispensable for future device exploitations. Copyright © 2012 John Wiley & Sons, Ltd.  相似文献   

5.
彭静  徐智谋  王双保  董泽华 《物理学报》2011,60(5):57702-057702
本文采用2-辛酸钡(Ba(C8H15O2)2)和3-甲基丁基醋酸盐(CH3COOC2H4CH(CH3)2-)为基的特殊前驱体溶液,在硅和石英基片上低温制备Ba0.7Sr0.3TiO3 (BST0.7)薄膜.性能测试结果表明,厚度约为214 nm的非晶BST0.7薄膜的光学带隙能和折射率分别为4.27 eV和n=1.94.薄膜在可见光和近红外区域的消光系数远远低于多晶BST薄膜,约为10-3数量级.激发波长为450 nm时,在室温环境下非晶BST0.7薄膜在波长520—610 nm处发出强烈的可见光,峰值为540—570 nm,而结晶态的BST0.7薄膜则无发光现象. 关键词: 钛酸锶钡 非晶薄膜 金属有机分解法 光学性能  相似文献   

6.
从自旋扩散方程和欧姆定律出发研究了铁磁层到有机半导体的自旋注入,得到了系统的电流自旋极化率。有机半导体中的载流子为自旋极化子和不带自旋的双极化子,极化子比率在有机半导体内随输运距离变化。通过计算发现匹配的铁磁和有机半导体电导率有利于自旋注入;通过调节界面电阻自旋相关性,电流自旋极化率可获得很大程度提高;极化子比率衰减速率对有机半导体电流自旋极化率具有非常重要的影响。  相似文献   

7.
A 10-nm-thick molybdenum tri-oxide(MoO3) thin film was used as the interconnector layer in tandem organic lightemitting devices(OLEDs).The tandem OLEDs with two identical emissive units consisting of N,N-bis(naphthalen-1-yl)N,N-bis(phenyl)-benzidine(NPB) /tris(8-hydroxyquinoline) aluminum(Alq3) exhibited current efficiency-current density characteristics superior to the conventional single-unit devices.At 20 mA/cm2,the current efficiency of the tandem OLEDs using the interconnector layers of MoO3 thin film was about 4.0 cd/A,which is about twice that of the corresponding conventional single-unit device(1.8cd/A).The tandem OLED showed a higher power efficiency than the conventional single-unit device for luminance over 1200cd/m2.The experimental results demonstrated that a MoO3 thin film with a proper thickness can be used as an effective interconnector layer in tandem OLEDs.Such an interconnector layer can be easily fabricated by simple thermal evaporation,greatly simplifying the device processing and fabrication processes required by previously reported interconnector layers.A possible explanation was proposed for the carrier generation of the MoO3 interconnector layer.  相似文献   

8.
阐明了金刚石薄膜电致发光研究的重要意义.综述了金刚石薄膜电致发光现象研究的进展情况,指出目前该方面研究中存在的问题,并提出了进一步提高金刚石薄膜蓝区电致发光强度的可能途径.  相似文献   

9.
陈达  黄仕华 《中国物理 B》2016,25(11):117701-117701
Si-rich SiO_x and amorphous Si clusters embedded in SiO_x films were prepared by the radio-frequency magnetron cosputtering method and high-temperature annealing treatment.The threshold resistance switching behavior was achieved from the memory mode by continuous bias sweeping in all films,which was caused by the formation of clusters due to the local overheating under a large electric field.Besides,the Ⅰ-Ⅴ characteristics of the threshold switching showed a dependence on the annealing temperature and the SiO_x thickness.In particular,formation and rupture of conduction paths is considered to be the switching mechanism for the 39 nm-SiO_x film,while for the 78 nm-SiO_x film,adjusting of the Schottky barrier height between insulator and semiconductor is more reasonable.This study demonstrates the importance of investigation of both switching modes in resistance random access memory.  相似文献   

10.
Anodization of sputtered NiTi thin films has been studied in 1 M acetic acid at 23 °C for different voltages from 2 to 10 V. The morphology and cross-sectional structures of the untreated and anodized surfaces were investigated by field emission scanning electron microscopy (FE-SEM). The results show that increasing anodization voltage leads to film surface roughening and unevenness. It can be seen that the thickness of the anodized layer formed on the NiTi surface is in the nanometer range. The corrosion resistance of anodized thin films was studied by potentiodynamic scan (PDS) and impedance spectroscopy (EIS) techniques in Hank's solution at 310 K (37 °C). It was shown that the corrosion resistance of the anodized film surface improved with increasing voltage to 6 V. Anodization of austenitic sputtered NiTi thin films has also been studied, in the same anodizing conditions, at 4 V. Comparison of anodized sputtered NiTi thin films with anodized austenitic shape memory films illustrate that the former are more corrosion resistant than the latter after 1 h immersion in Hank's solution, which is attributed to the higher grain boundary density to quickly form a stable and protective passive ?lm.  相似文献   

11.
We report on a forest-like-to-desert-like pattern evolution in the growth of an organic thin film observed by using an atomic force microscope. We use a modified diffusion limited aggregation model to simulate the growth process and are able to reproduce the experimental patterns. The energy of electric dipole interaction is calculated and determined to be the driving force for the pattern formation and evolution. Based on these results, single crystalline films are obtained by enhancing the electric dipole interaction while limiting effects of other growth parameters.  相似文献   

12.
研究了接触效应对有机薄膜晶体管性能的影响.首先在n型重掺杂Si片上制备了以MOO3修饰的Al电极为源漏电极的Pentacene基OTFTs(organic thin film transistors),器件场效应迁移率μef达到0.42 cm2/V ·s,阈值电压VT为-9.16 V,开关比4.7×103.通过中间探针法,对器件电势分布做了定性判断 关键词: 有机薄膜晶体管 场效应迁移率 接触效应 电荷漂移  相似文献   

13.
高质量纳米ZnO薄膜的光致发光特性研究   总被引:3,自引:4,他引:3       下载免费PDF全文
报道了利用低压-金属有机物化学气相沉积技术生长纳米ZnS薄膜,然后,将ZnS薄膜在氧气中于800℃温度下进行热氧化制备高质量纳米ZnO薄膜.x射线衍射结果表明,纳米ZnO薄膜具有六角纤锌矿多晶结构.室温下观察到一束强的紫外(3.26 eV) 光致发光和很弱的深能级发射.根据激子峰的半高宽度与温度的关系确定了激子-纵向光学声子(LO)的耦合强度(ГLO).由于量子限域效应使ГLO减少较多. 关键词: 光致发光 热氧化 激子 纳米ZnO薄膜  相似文献   

14.
ZnO thin films were deposited on the Si(100) substrate by rf sputtering using a 99.999% pure commercially bought and a home made target under 100 W power. The home made ZnO target, including 1–2% tungsten, was synthesized via solid state reaction. Thin films were deposited under a flow of 70% argon and 30% O2 gas mixture followed by post-deposition annealing under 1 Torr oxygen atmosphere. Both deposition and post-deposition annealing were done at 420±1 °C. The structural analyses show that the films were in the [0002] preferred direction and that W atoms are bound to the oxygen atoms by replacing the Zn host atoms. Although no specific change was observed in the magnetic properties as a result of W doping, significant changes in the electrical properties were observed, as determined by the longitudinal and transversal magneto-electrical measurements. It was found that the W impurities induce better insulating properties due to lower carrier concentration and higher resistivity values. On the other hand, the enhanced positive magnetoresistivity and the existence of polarized spin currents, which were not specific for pure ZnO thin films, were observed in W doped ZnO films below 10 K.  相似文献   

15.
窦兆涛  任俊峰  王玉梅  原晓波  胡贵超 《物理学报》2012,61(8):88503-088503
基于自旋扩散漂移方程,考虑到电场的影响及有机半导体中特殊的载流子电荷自旋关系, 对一个简单的T型结构有机自旋器件模型进行了理论研究,得出了此有机器件的电流自旋 极化放大率表达式.研究表明,器件中极化子比率、电场和电流密度都会影响器件的电流 自旋极化放大率,通过调节此有机器件的电场和极化子比率可以获得较大的电流自旋 极化放大率.  相似文献   

16.
利用反射式高能电子衍射(RHEED)、X射线衍射(XRD)和X射线吸收近边结构谱(XANES)等技术研究了在950 ℃条件下Si(111)衬底上共蒸发分子束外延方法制备的Mn掺杂SiC磁性薄膜的结构特征.RHEED结果表明,生长的Mn掺杂SiC薄膜为立方结构.XRD和XANES结果表明,在Mn掺杂量为0.5%和18%的样品中,Mn原子均是与SiC半导体介质中的Si原子反应生成镶嵌在SiC基体中的Mn4Si7化合物颗粒,并未观察到在SiC晶格中有替代式或间隙式的M  相似文献   

17.
文娟辉  杨琼  曹觉先  周益春 《物理学报》2013,62(6):67701-067701
基于密度泛函理论的第一性原理并结合非平衡格林函数, 探讨了应变对 BaTiO3 铁电薄膜漏电流的影响规律.研究表明,压应变能有效地抑制BaTiO3 铁电薄膜漏电流, 特别是当压应变为4%时,其漏电流相对无应变状态降低了近10 倍.通过考察体系的透射系数和电子态密度发现: 一方面压应变状态下铁电隧道结的透射几率要比张应变时小,特别是在费米面附近;另一方面随着张应变过渡至压应变时,价带的位置逐渐向低能区移动而导带向高能区移动,导致了其带隙的增大, 从而有效抑制了漏电流. 本研究为寻找抑制铁电薄膜漏电流,提高铁电薄膜及铁电存储器的性能提供合适的方法. 关键词: 铁电薄膜 双轴应变 漏电流 第一性原理  相似文献   

18.
杨桦  冯中沛  林泽丰  胡卫  秦明阳  朱北沂  袁洁  金魁 《物理学报》2018,67(20):207416-207416
在铁基超导体中,FeSe具有最简单的晶体结构和化学组成,而且其超导转变温度具有较大的调控空间,因此适合作为超导机理研究和应用的载体.高质量样品的研制是物性研究和器件应用的前提,本文系统地研究了利用激光脉冲沉积技术制备FeSe薄膜的工艺条件,在多种衬底上成功地制备出高质量的β-FeSe薄膜,并首次实现了超导临界转变温度从小于2 K到14 K的连续调控,这为FeSe超导机理研究提供了样品支持.为探究FeSe薄膜超导电性变化的起因,从β-FeSe超导电性与晶格常数c正相关出发,基于简单的费米面填充假设,第一性原理计算可以很好地解释晶格常数c的变化规律,但该假设并不能完全符合角分辨光电子能谱实验给出的电子结构演变过程.因此β-FeSe薄膜的超导电性、晶格结构和电子结构三者之间的关系还有待澄清,该问题的解决将为FeSe超导机理研究提供重要的线索,而上述系列高质量的β-FeSe薄膜样品恰好能为该问题的研究提供理想的载体.本文根据实验和已有的相关研究结果,详细介绍了FeSe薄膜的脉冲激光沉积制备及其优化,以期为后续的薄膜研究应用提供参考.  相似文献   

19.
A numerical model is developed to describe the leakage characteristics in ferroelectric thin films under ionizing radiation. The trap-controlled space-charge-limited conduction mechanism is modified by considering radiation-induced charge carriers and changes in the relative dielectric constant. The effect of dose rate is related to the changes in the carrier mobility. Numerical simulation using this model reveals a radiation hardness of 10 Mrad(Si) for barium strontium titanate (BST) thin films at a constant dose rate of 10 Krad(Si)/s. Differences in the leakage behavior under radiation for different conduction regions are also discussed. This model provides a useful tool in predicting the leakage behavior under ionizing radiation and estimating the radiation hardness for ferroelectric materials.  相似文献   

20.
通过扫描电镜和X射线衍射对SiO2衬底上生长并五苯和酞菁铜薄膜的表面形貌进行表征,并得到在SiO2衬底上生长的并五苯薄膜是以岛状结构生长,其大小约为100nm,且薄膜有较好的结晶取向,呈多晶态存在. 酞菁铜薄膜则没有表现出明显的生长机理,其呈非晶态存在. 还对通过掩膜的方法制作得以酞菁铜和并五苯为有源层的顶栅极有机薄膜晶体管的特性进行了研究. 有源层的厚度为40nm,绝缘层SiO2的厚度为250nm,器件的沟道宽长比(W/关键词: 有机薄膜晶体管 并五苯薄膜 酞菁铜薄膜 μEF)')" href="#">场效应迁移率(μEF)  相似文献   

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