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1.
Cu2O-ZnO异质结具有成本低廉、环境友好及制备方法多样等优点,在太阳能电池领域有很好的应用前景。Cu2O薄膜的高电阻率和低载流子浓度是制约其效率提高的主要原因。本文采用磁控溅射法,在qV(Ar)∶qV(O2)=90∶0.3时得到单相p型Cu2O薄膜,电阻率为88.5Ω·cm,霍尔迁移率为16.9 cm2·V-1·s-1,载流子浓度为4.19×1015cm-3。并结合Cu2O-ZnO异质结能带结构的研究,对Cu2O-ZnO异质结太阳能电池今后的研究提出了一些建议。  相似文献   

2.
利用湿化学法在FTO玻璃基底上制备了高度规整的ZnO纳米棒阵列(ZnO NRAs),以此为衬底,采用磁控溅射法在ZnO NRAs表面沉积Cu_2O薄膜。分别用X射线衍射仪、X射线光电子能谱、扫描电镜、光致光谱、紫外可见分光光度计和电化学工作站对样品的物相、形貌、吸收光谱、光电性能进行了表征,用甲基橙(MO)模拟有机物废水研究复合材料的光催化性能。结果表明:ZnO纳米棒为六方纤锌矿结构,其直径约为80~100 nm,长约2~3μm,棒间距约100~120 nm。立方晶系的Cu_2O颗粒直径约为100~300 nm,形成致密膜层并紧密覆盖在ZnO NRAs表面上,构成ZnO/Cu_2O异质结纳米阵列(ZnO/Cu_2O HNRAs)结构。与纯ZnO NRAs和Cu_2O相比,ZnO/Cu_2O HNRAs在可见光范围内的吸收显著增强,吸收波长向可见光方向偏移。ZnO/Cu_2O HNRAs的载流子传递界面的电荷转移速度快,有效促进了光生电子和空穴的分离。在紫外-可见光照射65 min后,ZnO/Cu_2O HNRAs的降解效率为94%,分别是纯ZnO NRAs和Cu_2O的18倍和1.7倍。  相似文献   

3.
陈新亮  陈莉  周忠信  赵颖  张晓丹 《物理学报》2018,67(11):118401-118401
介绍了近年来低成本Cu_2O/ZnO氧化物异质结太阳电池方面的研究进展.应用于光伏器件的吸收层材料Cu_2O是直接带隙半导体材料,天然呈现p型;其原材料丰富,且对环境友好.Cu_2O/ZnO异质结太阳电池结构主要有平面结构和纳米线/纳米棒结构.纳米结构的Cu_2O太阳电池提高了器件的电荷收集作用;通过热氧化Cu片技术获得的具有大晶粒尺寸平面结构Cu_2O吸收层在Cu_2O/ZnO太阳电池应用中展现出了高质量特性.界面缓冲层(如i-ZnO,a-ZTO,Ga_2O_3等)和背表面电场(如p~+-Cu_2O层等)可有效地提高界面处能级匹配和增强载流子输运.10 nm厚度的Ga_2O_3提供了近理想的导带失配,减少了界面复合;Ga_2O_3非常适合作为界面层,其能够有效地提高Cu_2O基太阳电池的开路电压V_(oc)(可达到1.2 V)和光电转换效率.p~+-Cu_2O(如Cu_2O:N和Cu_2O:Na)能够减少器件中背接触电阻和形成电子反射的背表面电场(抑制电子在界面处复合).利用p型Na掺杂Cu_2O(Cu_2O:Na)作为吸收层和Zn_(1-x)Ge_x-O作为n型缓冲层,Cu_2O异质结太阳电池(器件结构:MgF_2/ZnO:Al/Zn_(0.38)Ge_(0.62)-O/Cu_2O:Na)光电转换效率达8.1%.氧化物异质结太阳电池在光伏领域展现出极大的发展潜力.  相似文献   

4.
采用简单的两步水热法合成了不同In2O3质量比的In2O3/ZnO异质结复合材料.通过X射线衍射仪(XRD)、紫外-可见分光光度计(UV-vis)和扫描电子显微镜(SEM)对复合材料的结构、形貌和性能进行了表征.同时还使用UV-vis分光光度计测试了异质结降解罗丹明B(RhB)的光催化活性.实验结果表明,与纯ZnO和In2O3相比,In2O3的引入将ZnO的吸收光谱扩展到可见光区域,从而提高了其光生电子和空穴的分离.此外,In2O3/ZnO异质结在可见光照射对RhB具有较高的光催化活性.5 wt%-In2O3/ZnO异质结对RhB的降解率为84.3%,且具有良好的光催化稳定性.In2O3/ZnO异质结复合材料在有机染料废水的降解中有更广阔的应用前景.  相似文献   

5.
利用直流反应溅射方法在p型Si衬底上生长掺Al的n型ZnO薄膜,测量了由n型ZnO薄膜和p型Si衬底组成的异质结在黑暗和光照条件下的I-V特性,结果表明该异质结具有优良的整流特性,而且在光照条件下的反向电流迅速增大并很快趋于饱和.通过测量ZnO薄膜的光电流和异质结的光电压的光谱响应,初步分析了异质结的光电转换机理.测量结果显示,在入射光波长为380nm时光电流强度明显下降,反映出光电流与ZnO薄膜禁带宽度的密切关系;同时还发现,在与ZnO禁带宽度相对应的波长前后所产生的光生电压方向相反.推测这一现象与异质结的能带结构密切相关. 关键词: ZnO薄膜 异质结 光电转换 光谱响应  相似文献   

6.
通过溶胶-凝胶结合静电纺丝过程制备了In2O3/CuO纳米异质结。XRD和Raman光谱的研究表明,随着前驱物中Cu/In比例的增加,CuO相的含量逐渐增加。吸收光谱研究表明,随着CuO含量的增加,复合纳米结构的可见光吸收明显增强。光催化实验研究结果表明,In2O3/CuO纳米异质结具有比单一相的In2O3和CuO更强的光催化性能,其主要来源于异质结所导致的增强的光生电子和空穴的分离效率。  相似文献   

7.
利用等离子体增强化学气相沉积(PECVD)技术,在ZnO/ZnMgO异质结构上制备SiO2作为栅绝缘层,采用光刻与腐蚀工艺制备ZnO/ZnMgO异质结场效应管。电学性能测试及计算结果表明器件栅压调控作用明显。发现栅端漏电流对器件性能造成一定影响。在低温条件下,栅绝缘层产生钝化,从而能够改善器件的性能。  相似文献   

8.
毕文杰  杨爽  周静  金伟  陈文 《物理学报》2023,(16):273-283
水产品的新鲜度极大地影响着人类的生命及身体健康,水产品在存放过程中会释放出以三甲胺为代表的胺类气体,通过检测这类气体的浓度可以监控水产品的新鲜度.本文以具有优良气体敏感性能的MoO3纳米带作为基体,通过引入Cu3Mo2O9纳米颗粒制备Cu3Mo2O9/MoO3复合材料,具有非常好的三甲胺气体敏感性能、快速响应/恢复时间及长期稳定性.结果表明,采用这种复合材料制备的气敏元件在50—240℃,质量分数为5×10-6时对三甲胺气体的响应可达到Rair/Rgas=13.9,最小检测极限的体积分数为2×10-7.分布在MoO3纳米带表面的Cu3Mo2O9颗粒与基体形成异质结界面,利用Cu3Mo2O...  相似文献   

9.
在室温下,通过溶液法在Cu衬底上制备了CuO纳米线,然后采用溶剂热法在CuO纳米线表面生长ZnO纳米颗粒以构建CuO/ZnO复合纳米线异质结构.利用扫描电镜、透射电镜、X射线衍射仪和X射线光电子能谱分析了样品的形貌、结构和元素组成.结果显示CuO/ZnO复合纳米线由ZnO纳米颗粒和CuO纳米线组成.在模拟太阳光照射下,...  相似文献   

10.
作为一类重要的光电极材料,α-Fe2O3在太阳能转化方面有着潜在的应用前景.但是,光生电子空穴对的再复合导致α-Fe2O3的光电量子产率很低.为了抑制光生电子空穴对的再复合,提高α-Fe2O3的光电量子产率,采用Spin-coating方法在透明导电玻璃FTO(SnO2:F)衬底上制备了SrTiO3/α-Fe2O3异质结薄膜光电极,并对该光电极进行了XRD、SEM、紫外-可见透射光谱的表征.在三电极光电化学测试系统中对薄膜的光电流-电压特性、入射光子电流转化效率(Incident photon to current efficiency,IPCE)对波长的依赖性进行了表征.在相同的Xe灯照射条件下,SrTiO3/α-Fe2O3异质结光电极的光电流及IPCE值大于单一的SrTiO3、α-Fe2O3各自的光电流及IPCE值,这与理论预测的结论一致.  相似文献   

11.
We report on the photovoltaic properties of Lao.7Sro.3MnO3//ZnO heterojunction fabricated by pulsed laser deposition methods. Nanosecond photovoltaic pulses are observed in this junction in the wavelength range from ultraviolet-visible to infrared. A qualitative explanation is presented, based on an analysis of the photovoltaic signals of p-n heterojunction.  相似文献   

12.
用电化学沉积法制备ZnO/Cu2O异质p-n结   总被引:1,自引:1,他引:1  
由于P型ZnO的制备仍然存在一定的困难,限制了ZnO在光电方面的应用,尤其是在发光二极管和激光器的实际应用,目前利用P型的透明半导体氧化物与n型ZnO制备异质p-n结,成为新的研究热点。选择P型导电Cu2O与ZnO制备出异质p-n结。Cu2O是一种典型的P型半导体材料,禁带宽度为2.1eV,可见光范围的吸收系数较高。首次利用电化学沉积的方法制备了ZnO/Cu2O异质p-n结,研究了电沉积ZnO,Cu2O的生长机制和ZnO/Cu2O异质结的结构、光学和电学特性。  相似文献   

13.
ZnO, Zn0.95Mn0.05O and Cu2O nanocrystals are synthesized. Excitonic lines in absorption spectra of these materials are detected. In photoluminescence and photoluminescence excitation spectra of Zn0.95Mn0.05O the dangling bond hybrid (DBH) state is found. It has splitted out from the top of the valence band due to the hybridization between d-states of the Mn impurity and the p-states of oxygen.  相似文献   

14.
To establish the nature of 0.7 and 0.9 μ-emission bands in cuprous oxide their excitation spectra, excitation spectra of free carriers cyclotron resonance and magneto-optic polarization adn intensity spectra have been investigated. On the basis of these data it was concluded that the bands are caused by relaxed excitons, localized near oxygen and copper vacancies.  相似文献   

15.
N-ZnO/p-Si heterojunctions are prepared by sputtering deposition of intrinsic ZnO films on p-Si substrates. Thicknesses of ZnO films are altered by varying the deposition time from I h to 3h. The electrical properties of these structures are analysed from capacitance-voltage (C V) and current-voltage (I-V) characteristics performed in a dark room. The results demonstrated that all the samples show strong rectifying behaviour. Photovoltaie property for the samples with different thicknesses of ZnO films are investigated by measuring open circuit voltage and short circuit current. It is found that photovoltages are kept to be almost constant of 320 m V along with the thickness while photoeurrents changing a lot. The variation mechanism of the photovoltade effect as a function of thickness of ZnO films is investigated.  相似文献   

16.
17.
Two series of Mn-doped Cu2O diluted-magnetic-semiconductor thin films were prepared by radio-frequency (RF) magnetron sputtering. One is prepared at different deposition temperature with the same Mn doping concentration; the other is deposited at the same temperature but with varying Mn concentration. They were used to find out the ferromagnetic-order zone for the Mn-doped Cu2O systems. Most of the samples show high (1 1 1) orientation, except low doping concentration (<6 at%). No impurities were found by X-ray diffraction and electron diffraction measurement. The doped Mn ions substituted Cu ions in the Cu2O lattice and there were about 1.5% cation vacancies. The grains shown in the transmission electron microscopy (TEM) images for all the samples were tiny, i.e. just 5 nm in diameter. A rough phase diagram for the ferromagnetic order existing in the Mn-doped Cu2O thin films was given with varying Mn doping concentration and deposition temperature.  相似文献   

18.
A first-principles investigation of cuprite crystals (Cu2O and Ag2O) has been performed. For Cu2O, the calculated frequencies at the Γ point of the Brillouin zone are in very good agreement with the experimental frequencies. For Ag2O, the presence of Eu and F2u vibrational modes with negative frequencies indicates a low temperature phase transition, in agreement with recent high resolution X-ray and neutron diffraction measurements. The energy scanning along these two modes shows a double-well potential, within which only the Ag atoms vibrate. As a result, the origin of the phase transition can be attributed to displacive disorder of the Ag atoms.  相似文献   

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