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1.
吴萍  张杰  李喜峰  陈凌翔  汪雷  吕建国 《物理学报》2013,62(1):18101-018101
在室温下采用射频磁控溅射法制备了以ZnO薄膜为沟道层的薄膜晶体管(TFTs).研究表明ZnO薄膜在紫外区具有较高的吸收率,并且ZnO-TFTs对紫外光照射较为敏感.因此,进一步深入研究了ZnO-TFTs紫外光照下的输出和转移特性,结果表明,紫外光照将引起较为明显的光响应电流,且经过光照的器件在光源移除7天后,ZnO沟道层中仍能观察到残余电导现象,其原因可以归结为紫外光辐射在ZnO沟道层中引入了一定数量的氧空位施主态缺陷.  相似文献   

2.
杨帆  韦敏  邓宏  杨胜辉  刘冲 《发光学报》2014,35(5):604-607
以 ZnO:Al为底电极,Cu为顶电极,在同种工艺条件下分别制备了类电容结构的纯ZnO 阻变器件和ZnO:2%Cu阻变器件,分析比较了两种器件的典型I-V特性曲线、置位电压(VSet)和复位电压(VReset)的分布范围、器件的耐久性。结果显示,ZnO:Cu阻变器件较纯ZnO阻变器件有更大的开关比和更稳定的循环性能。另外,研究了 ZnO:Cu阻变器件的阻变机理,通过对其I-V特性曲线分析得出以下结论:ZnO:Cu阻变器件在高阻态遵循空间电荷限制电流效应,低阻态符合欧姆定律。  相似文献   

3.
综合氧化锌纳米线(ZnO NWs)的光学活性与聚苯胺(PANI)的空穴传输特性,设计并制备了一种聚合物/ZnO纳米线电致发光材料,并对其发光特性进行了研究。通过高分子络合软模板法,将有序的单晶ZnO NWs均匀生长在覆有铟锡氧化物(ITO)涂层的柔性聚乙烯对苯二甲酸乙二醇酯(PET)衬底上并嵌入PANI薄膜,获得了电致发光薄膜材料和有机/无机异质结实验器件ITO/(ZnO NWs-PANI)。有机/无机异质结器件电致发光可调,在相对低的开启电压下呈现室温蓝紫外发光,并且ZnO NWs表面覆盖PANI增加了蓝紫外发光的强度和稳定性;而无PANI的ZnO NWs阵列具有450 nm处的缺陷发射峰,这可能是电子从扩展态锌间隙Zni到价带的跃迁引起的。这些结果表明,基于PANI/ZnO纳米线的复合材料在柔性光电器件方面的应用极具潜力。  相似文献   

4.
王丽师  徐建萍  石少波  张晓松  任志瑞  葛林  李岚 《物理学报》2013,62(19):196103-196103
本文通过化学浴沉积法获得了直径约为50 nm, 长度约为250 nm的ZnO纳米棒阵列, 引入纳米ZnS对ZnO纳米棒进行表面修饰, 分别制备得到了具有ITO (indium tin oxides)/ZnO/Poly-(3-hexylthiophene) (P3HT)/Au和ITO/ZnO@ZnS/P3HT/Au结构的多层器件. 通过I-V曲线对比讨论了两种结构器件的开启电压, 串联电阻, 反向漏电流及整流比等参数, 认为包含ZnS修饰层器件的开启电压、串联电阻、反向漏电流明显降低, 整流比显著增强, 展现出更优异的电子传输性能. 光致发光光谱分析结果证实由于ZnS使ZnO纳米 棒的表面缺陷产生的非辐射复合被明显抑制, 弱化了电场激发下的载流子陷获, 改善了器件的导电特性. 关键词: ZnO纳米棒阵列 表面修饰 电流-电压特性  相似文献   

5.
氧化锌纳米颗粒薄膜的近紫外电致发光特性研究   总被引:1,自引:0,他引:1       下载免费PDF全文
高松  赵谡玲  徐征  杨一帆  刘志民  谢小漪 《物理学报》2014,63(15):157702-157702
利用溶胶-凝胶法(sol-gel method)制备了ZnO纳米颗粒薄膜(ZnO nanoparticle film),并以此为发光层制备了结构为ITO/ZnO nanoparticle/MEH-PPV/LiF/Al的电致发光器件.通过调整器件发光层厚度,对器件的发光光谱和电学特性进行测试研究,发现该器件在一定的直流电压下可以得到以ZnO近紫外(中心波长390 nm)发光为主的电致发光光谱,显示出较好的ZnO近紫外电致发光特性.对该器件的发光机理进行了一定的研究,认为该器件的发光是基于载流子隧穿.  相似文献   

6.
本文制备了基于ZnO纳米线阵列和ZnO薄膜的Ag-ZnO-Ag电导型X射线探测器件,研究了它们对X射线的响应特性.薄膜器件在100 V偏置时的响应度达到0.12μC/Gy,纳米线阵列器件在50 V偏压下的响应度达到0.17μC/Gy.器件工作机理研究表明,器件的响应过程与表面氧吸附与解吸附效应有关,氧气吸附与解吸附过程使得X射线辐照下的载流子寿命大幅度增加,从而使得器件对X射线具有较高的响应度.本文研究结果表明ZnO薄膜和纳米线阵列器件在X射线剂量测量领域具有应用前景.  相似文献   

7.
以ZnO为电子传输层PPV的发光   总被引:2,自引:0,他引:2       下载免费PDF全文
滕枫  黄宗浩 《发光学报》1997,18(4):348-350
以Ⅱ-Ⅵ族无机半导体ZnO为电子传输层,PPV为空穴传输层和发光层,得到的电致发光器件比单层PPV器件的发光亮度和效率都高.器件结构为ITO/PPV/ZnO/Al的电致发光光谱同单层PPV器件的光谱基本相同,但是启亮电压明显比单层器件低,最大亮度大约比单层器件高6倍左右,同时工作电流也比单层器件小.通过PPV层自吸收现象可判断出发光区域在PPV/ZnO界面处.电流-电压曲线表明,这种器件具有空间电荷限制电流特性,即JVn,这里n大约为2,这器件的电流主要受到空穴的限制.  相似文献   

8.
用RF-MBE在蓝宝石(0001)衬底上引入MgO和低温ZnO双缓冲层生长了ZnO薄膜,并制备了声表面波器件。在ZnO薄膜中,仅观测到(0002)面的XRD,且衍射峰增强,半高宽减小,表明ZnO薄膜c轴取向性更好,晶体结构更优。室温下自由激子吸收峰更尖锐和吸收边更陡峭以及仅观测到自由激子发光,且发光线宽变窄、发光强度变大,表明ZnO薄膜缺陷密度减小,薄膜质量提高。测得该ZnO压电薄膜的电阻率高达4×107 Ω·cm,其声表面波的速度高达5 010 m/s。  相似文献   

9.
正ZnO具有优异的紫外发光、激射、光响应等功能特性,是固态光源和电力电子、微波射频器件的理想材料之一。经过全球众多科学家的不懈研究,人们对ZnO半导体的光、电、磁及压电等特性有了深刻的理解,在紫外发光器件、紫外激光器件、紫外光电探测器件、压电器件、太阳能电池等领域的研究不断取得重要进展,特别是ZnO基透明导电膜、薄膜晶体管已经在光电子领域大规模工业应用,在环境、生物、  相似文献   

10.
室温下溅射法制备高迁移率氧化锌薄膜晶体管   总被引:11,自引:10,他引:1       下载免费PDF全文
刘玉荣  黄荷  刘杰 《发光学报》2017,38(7):917-922
为降低氧化锌薄膜晶体管(ZnO TFT)的工作电压,提高迁移率,采用磁控溅射法在氧化铟锡(ITO)导电玻璃基底上室温下依次沉积NbLaO栅介质层和ZnO半导体有源层,制备出ZnO TFT,对器件的电特性进行了表征。该ZnO TFT呈现出优异的器件性能:当栅电压为5 V、漏源电压为10 V时,器件的饱和漏电流高达2.2 m A;有效场效应饱和迁移率高达107 cm~2/(V·s),是目前所报道的室温下溅射法制备ZnO TFT的最高值,亚阈值摆幅为0.28 V/decade,开关电流比大于107。利用原子力显微镜(AFM)对NbLaO和ZnO薄膜的表面形貌进行了分析,分析了器件的低频噪声特性,对器件呈现高迁移率、低亚阈值摆幅以及迟滞现象的机理进行了讨论。  相似文献   

11.
n-ZnO/i-MgO/p-GaN异质结发光二极管   总被引:10,自引:10,他引:0       下载免费PDF全文
用等离子体辅助分子束外延的方法生长了n-ZnO/i-MgO/p-GaN异质结发光二极管。I-V测量表明其具有典型的二极管整流特性。电致发光峰位于382nm,通过与n型ZnO和p型GaN的光致发光谱比较,其发光峰位与线形都与ZnO的自由激子发射一致,表明该电致发光来自于ZnO的自由激子发射。通过Anderson模型比较了n-ZnO/i-MgO/p-GaN和n-ZnO/p-GaN异质结的能带示意图,证明了由于MgO层的插入抑制了ZnO向GaN层中的电子注入,且有利于空穴向ZnO层注入,从而实现了ZnO层中的电注入发光。  相似文献   

12.
Vertically aligned ZnO nanowires were successfully grown on the sapphire substrate by nanoparticle-assisted pulsed laser deposition (NAPLD), which were employed in fabricating the ZnO nanowire-based heterojunction structures. p-GaN/n-ZnO heterojunction light-emitting diodes (LEDs) with embedded ZnO nanowires were obtained by fabricating p-GaN:Mg film/ZnO nanowire/n-ZnO film structures. The current–voltage measurements showed a typical diode characteristic with a threshold voltage of about 2.5 V. Electroluminescence (EL) emission having the wavelength of about 380 nm was observed under forward bias in the heterojunction diodes and was intensified by increasing the applied voltage up to 30 V.  相似文献   

13.
ZnMgO/n-ZnO/ZnMgO/p-GaN异质结LED的紫外电致发光   总被引:3,自引:2,他引:1  
宿世臣  吕有明 《发光学报》2011,32(8):821-824
利用等离子体辅助分子束外延( P-MBE)技术制备了ZnMgO/n-ZnO/ZnMgO/p-GaN异质结LED.Ni/Au电极与p-GaN、In电极与ZnMgO之间都形成了良好的欧姆接触.在ZnMgO/n-ZnO/ZnMgO/p-GaN异质结器件中观察到了明显的整流特性.异质结的电致发光强度随着注入电流的增大而逐渐增强...  相似文献   

14.
Based on the easily controllable radio frequency magnetron sputtering, n-ZnO and i-MgO thin films were fabricated on p+-GaN substrate to construct heterojunctional light-emitting diodes for ultraviolet emission from the near band edge exciton recombination of ZnO. Effects of the insulator MgO layer on the electroluminescent performance of the n-ZnO/i-MgO/p+-GaN light-emitting diodes have been investigated. It was found that the light-emitting diode presented stronger near band-edge emission with blue shift emission peak under the lower working current when i-MgO layer was inserted. The fabrication process, characteristics and the mechanism were discussed in detail.  相似文献   

15.
Lu TC  Ke MY  Yang SC  Cheng YW  Chen LY  Lin GJ  Lu YH  He JH  Kuo HC  Huang J 《Optics letters》2010,35(24):4109-4111
Low-temperature electroluminescence from ZnO nanowire light-emitting arrays is reported. By inserting a thin MgO current blocking layer in between ZnO nanowire and p-GaN, high-purity UV light emission at wavelength 398 nm was obtained. As the temperature is decreased, contrary to the typical GaN-based light emitting diodes, our device shows a decrease of optical output intensity. The results are associated with various carrier tunneling processes and frozen MgO defects.  相似文献   

16.
ZnO-based heterojunction light emitting diodes (LEDs) with MgZnO barrier layer had been fabricated on the p-Si substrate by metal-organic chemical vapor deposition (MOCVD) technology. The current-voltage (I-V) characteristics exhibited a typical p-n diode behavior. Both ultraviolet (UV) and visible emissions could be detected in the electroluminescence (EL) measurement. The result was compared with the EL spectrum of n-ZnO/p-Si heterojunction LED without MgZnO barrier layer. An improved light extraction efficiency by about 31% was realized owing to the current-blocking effect of MgZnO layer. The result indicated that MgZnO barrier layer can prevent the electrons as expected and realize electron-hole recombination in ZnO layer effectively.  相似文献   

17.
X-ray photoelectron spectroscopy (XPS) was used to measure the energy discontinuity in the MgO (111)/ZnO (0002) heterostructure. The valence band offset (VBO) was determined to be 1.22±0.23 eV and a type-I heterojunction with a conduction band offset (CBO) of 3.24±0.23 eV was obtained. The discrepancy of VBO values between MgO/ZnO and ZnO/MgO heterojunctions was mainly attributed to the internal electric field induced by spontaneous polarization effect in ZnO layer.  相似文献   

18.
In this work, two types of Schottky barrier diodes (SBDs) with and without Rhodamine B interfacial layer, were fabricated and measured at room temperature in order to investigate the effects of the Rhodamine B interfacial layer on the main electrical parameters. It was seen that the barrier height (BH) value of 0.78 eV calculated for the Al/Rhodamine B/p-GaAs device was higher than the value of 0.63 eV of the conventional Al/p-GaAs Schottky diodes. It has been observed that the Rhodamine B film increases the effective BH by influencing the space charge region of GaAs. The main diode parameters such as the ideality factor (n) and zero-bias BH of SBD with Rhodamine B interfacial layer were found to be strongly temperature dependent and while the BH decreases, the ideality factor increases with decreasing temperature. It has been concluded that the temperature dependent characteristic parameters for Al/Rhodamine B/p-GaAs SBDs can be successfully explained on the basis of thermionic emission (TE) mechanism with Gaussian distribution of the barrier heights.  相似文献   

19.
Au/MgO/ZnO/MgO/Au structures have been designed and constructed in this study. Under a bias voltage, a carrier avalanche multiplication will occur via an impact ionization process in the MgO layer. The generated holes will be drifted into the ZnO layer, and recombine radiatively with the electrons in the ZnO layer. Thus obvious emissions at around 387 nm coming from the near-band-edge emission of ZnO will be observed. The reported results demonstrate the ultraviolet (UV) emission realized via a carrier multiplication process, and so may provide an alternative route to efficient UV emissions by bypassing the challenging p-type doping issue of ZnO.  相似文献   

20.
ZnO micro-prisms are prepared on the p-type and n-type Si substrates, separately. The $I$--$V$ curves analysed by AFM show that the interface junctions between the ZnO micro-prisms and the p-type substrate and between the ZnO micro-prisms and the n-type Si substrate exhibit p--n junction behaviour and ohmic contact behaviour, respectively. The formation of the p--n heterojunction and ohmic contact is ascribed to the intrinsic n-type conduction of ZnO material. Better field emission performance (lower onset voltage and larger emission current) is observed from an individual ZnO micro-prism grown on the n-type Si substrate. It is suggested that the n-Si/n-ZnO interfacial ohmic contact benefits the electron emission; while the p-Si/n-ZnO interface heterojunction deteriorates the electron emission.  相似文献   

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