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1.
通过反应磁控溅射在n型硅和玻璃衬底上制备了p型CuO薄膜.使用X射线衍射仪和紫外-可见光-近红外光度计研究了p型CuO薄膜的结构和光学特性,得出其平均晶粒尺寸和光学带隙分别为8 nm和1.36 eV.通过研究其电压-电流关系确定了在p型CuO薄膜和n型硅衬底之间形成了p-n结.在AM 1.5光照条件下p-CuO/n-Si电池的开路电压为0.33 V,短路电流密度为6.27 mA/cm2, 填充因数和能量转化效率分别为0.2和0.41%.  相似文献   

2.
采用射频磁控溅射法在p型自支撑金刚石衬底上制备了高度c轴取向的n型氧化锌薄膜.研究了不同的溅射功率对氧化锌薄膜质量的影响.通过半导体特性分析系统测试了氧化锌/金刚石异质结的电流-电压特性,结果显示该异质结二极管具有良好的整流特性,开启电压约为1.6 V.在此基础上制备了结型紫外光探测器,并对其光电性能进行了研究.结果表...  相似文献   

3.
CuO薄膜的三阶非线性光学特性研究   总被引:1,自引:0,他引:1       下载免费PDF全文
采用脉冲激光沉积技术在Si(100)和熔石英基片上制备了单相的CuO薄膜.通过X射线衍射仪,拉曼光谱仪,场发射扫描电镜和紫外可见光光度计对薄膜的结构,表面形貌和光学性质进行了表征. 场发射扫描电镜结果表明CuO薄膜中晶粒排列致密且分布均匀,其尺寸约为45nm.结合飞秒激光(800nm,50fs)和Z扫描方法测量了薄膜的三阶非线性光学特性,结果表明CuO薄膜具有超快的非线性光学响应且非线性折射率和非线性吸收系数均为负值,其大小分别为-3.96×10-17 m2< 关键词: CuO薄膜 Z-扫描')" href="#">Z-扫描 三阶光学非线性  相似文献   

4.
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   

5.
用化学溶液方法在宝石衬底及有LaNiO3缓冲层的Pt/TiO2/SiO2/Si衬底上制备了92%Pb(Mg1/3 Nb2/3)O3-8%PbTiO3(PMNT)薄膜,X射线衍射测试结果表明:在有LaNiO3缓冲层的Pt/TiO2/SiO2/Si衬底上制备的PMNT薄膜几乎是纯钙钛矿相,且薄膜呈现(110)择优取向.通过对Pt/TiO2/SiO2/Si衬底上的PMNT薄膜在2.5-12.6μm波长范围内的红外椭圆偏振光谱测试,并拟合得到了PMNT薄膜在2.5-12.6μm波长范围内的光学常数(n和k),通过对宝石衬底上的PMNT薄膜在200-1100nm波长范围内的可见-紫外透过率测试,并拟合得到了PMNT薄膜在200-1100nm波段的光学常数(n和k)和吸收系数α,进而推导出PMNT薄膜的禁带宽度为4.03eV.  相似文献   

6.
本文通过在硅衬底发光二极管(LED)薄膜p-GaN表面蒸发不同厚度的Ni覆盖层,将其在N2 ∶O2=4 ∶1的气氛中、400℃—750℃的温度范围内进行退火,在去掉薄膜表面Ni覆盖层之后制备Pt/p-GaN欧姆接触层.实验结果表明:退火温度和Ni覆盖层厚度均对硅衬底GaN基LED薄膜p型欧姆接触有重要影响,Ni覆盖退火能够显著降低p型层中Mg受主的激活温度.经牺牲Ni退火后,p型比接触电阻率随退火温度的升高呈先变小后变大的规律,随Ni覆盖层厚度的增加呈先变小后变 关键词: 氮化镓 发光二极管 牺牲Ni退火 p型接触  相似文献   

7.
采用高压射频等离子体增强化学气相沉积方法在非晶和微晶两种n型硅薄膜衬底上沉积了一系列不同厚度的本征微晶硅薄膜,研究了不同n型硅薄膜对本征微晶硅薄膜的表面形貌、晶化率和结晶取向等结构特性的影响.结果表明,本征微晶硅薄膜结构对n型掺杂层具有强烈的依赖作用,微晶n型掺杂层能够有效减少n/i界面非晶孵化层的厚度,改善本征微晶硅薄膜的纵向均匀性,进而提高微晶硅n-i-p太阳电池性能. 关键词: 孵化层 微晶硅薄膜 纵向均匀性 n-i-p太阳电池  相似文献   

8.
Ag掺杂p型ZnO薄膜及其光电性能研究   总被引:2,自引:0,他引:2       下载免费PDF全文
采用超声喷雾热分解法在石英衬底上以醋酸锌水溶液为前驱体,以硝酸银水溶液为Ag掺杂源生长了Ag掺杂ZnO(ZnO:Ag)薄膜.研究了衬底温度对所得ZnO:Ag薄膜的晶体结构、电学和光学性质的影响规律.所得ZnO:Ag薄膜结构良好,在室温光致发光谱中检测到很强的近带边紫外发光峰,透射光谱中观测到非常陡峭的紫外吸收截止边和较高的可见光区透过率,表明薄膜具有较高的晶体质量与较好的光学特性.霍尔效应测试表明,在500℃下获得了p型导电的ZnO:Ag薄膜,载流子浓度为5.30×1015cm关键词: ZnO:Ag薄膜 p型掺杂 超声喷雾热分解 霍尔效应  相似文献   

9.
立方氮化硼薄膜的光学带隙   总被引:1,自引:0,他引:1       下载免费PDF全文
邓金祥  汪旭洋  姚倩  周涛  张晓康 《物理学报》2008,57(10):6631-6635
用射频溅射法在p型Si(100)衬底上沉积立方氮化硼(c-BN)薄膜,薄膜的成分由傅里叶变换红外谱标识,用紫外-可见分光光度计测量了c-BN薄膜的反射光谱,利用K-K(Kramers-Kroning)关系从反射谱计算出c-BN薄膜的光吸收系数,进而确定c-BN薄膜的光学带隙.对于立方相含量为55.4%的c-BN薄膜,光学带隙为5.38eV. 关键词: 立方氮化硼薄膜 光学带隙 K-K关系  相似文献   

10.
以B2H6为掺杂剂,采用射频等离子体增强化学气相沉积技术在玻璃衬底上制备p型氢化微晶硅薄膜.研究了衬底温度和硼烷掺杂比对薄膜的微结构和暗电导率的影响.结果表明:在较高的衬底温度下很低的硼烷掺杂比即可导致薄膜非晶化;在实验范围内,随着衬底温度升高薄膜的晶化率单调下降,暗电导率先缓慢增加然后迅速下降,变化趋势与硼烷掺杂比的影响极为相似.最后着重讨论了p型氢化微晶硅薄膜的生长机理. 关键词: p型氢化微晶硅薄膜 衬底温度 晶化率 电导率  相似文献   

11.
倪牮  张建军  曹宇  王先宝  李超  陈新亮  耿新华  赵颖 《中国物理 B》2011,20(8):87309-087309
This paper identifies the contributions of p-a-SiC:H layers and i-a-Si:H layers to the open circuit voltage of p-i-n type a-Si:H solar cells deposited at a low temperature of 125 C.We find that poor quality p-a-SiC:H films under regular conditions lead to a restriction of open circuit voltage although the band gap of the i-layer varies widely.A significant improvement in open circuit voltage has been obtained by using high quality p-a-SiC:H films optimized at the "low-power regime" under low silane flow rates and high hydrogen dilution conditions.  相似文献   

12.
Thin films of 7,7′,8,8′ tertracyanoquinodimethane (TCNQ) were deposited using thermal evaporation technique. TCNQ was found to be polycrystalline in powder form and preferred to orient at one plane in thin films. The temperature dependence of the electrical resistivity of Au/TCNQ/Au device was studied. TCNQ thin films were deposited on p-GaAs single crystal substrate; the current-voltage and capacitance-voltage for TCNQ/p-GaAs junction sandwiched between two gold electrodes were investigated. The current of the device obeys the thermionic emission model in the voltage range of 0<V<0.5. The diode parameters such as rectification ratio, series resistance, quality factor and mean potential barrier height were evaluated. The space charge limited conduction dominated by single trapping level is applicable in the voltage range 0.5<V<1.5. The capacitance-voltage measurements showed that the formed junction is abrupt in its nature and the built-in potential is determined. Under illumination, the cell exhibited a photovoltaic characteristic from which the photovoltaic parameters such as open circuit voltage, short circuit current, fill factor and conversion efficiency were calculated.  相似文献   

13.
This paper reports that a double N layer (a-Si:H/μc-Si:H) is used to substitute the single microcrystalline silicon n layer (n-μc-Si:H) in n/p tunnel recombination junction between subcells in a-Si:H/μc-Si:H tandem solar cells. The electrical transport and optical properties of these tunnel recombination junctions are investigated by current-voltage measurement and transmission measurement. The new n/p tunnel recombination junction shows a better ohmic contact. In addition, the n/p interface is exposed to the air to examine the effect of oxidation on the tunnel recombination junction performance. The open circuit voltage and FF of a-Si:H/μc-Si:H tandem solar cell are all improved and the current leakage of the subcells can be effectively prevented efficiently when the new n/p junction is implemented as tunnel recombination junction.  相似文献   

14.
In order to considerable enhancement of the efficiency of silicon solar cells, in this paper, for the first time, we present a new proposal for silicon based tandem solar cells. For investigation of this idea, we have evaluated the characteristics of 3C–SiC/Si crystalline tandem solar cells connected series by a tunneling junction, under air mass 1.5 global irradiance spectrums. A 2D simulation including the effects of surface passivation, back surface field (BSF), and carrier tunneling have been performed to obtain the optical and electrical characteristics of single junction silicon, 3C–SiC, and finally the tandem cells. The obtained data illustrate that the best design parameters considering the experimental limitations can be obtained. High energy conversion efficiency for the proposed structure of 26.09% has been achieved for 3C–SiC/Si tandem structure driven by 20.49% and 17.86% conversion efficiencies of single junction Si and 3C–SiC solar cells, respectively. Our results justifies that the higher conversion efficiency of the Si-based tandem structure compared with 3C–SiC and Si cells stems from enhancement of open circuit voltage and fill factor parameter at the hands of decrease in short circuit current limited by the top 3C–SiC cell.  相似文献   

15.
采用KrF准分子激光器,在Si,Ge光学衬底上制备了碳化硼薄膜,研究了不同激光能量、靶材与衬底距离、衬底负偏压等条件对薄膜性能的影响。利用傅里叶变换红外光谱仪(FT-IR)和纳米压痕仪,并依据光学薄膜测试的通用标准,对样品的光学透过率、纳米硬度及膜层与衬底的结合性能进行了测试。结果表明:Si,Ge衬底单面镀碳化硼薄膜后最高透过率提高10%以上,纳米硬度提高到未镀膜的3倍以上,且膜层与衬底有较好的结合性能,表明制备的碳化硼薄膜可对光学材料起到较好的增透保护作用。  相似文献   

16.
雷青松  吴志猛  耿新华  赵颖  孙健  奚建平 《中国物理》2006,15(12):3033-3038
Hydrogenated silicon (Si:H) thin films for application in solar cells were deposited by using very high frequency plasma enhanced chemical vapour deposition (VHF PECVD) at a substrate temperature of about 170℃. The electrical, structural, and optical properties of the films were investigated. The deposited films were then applied as i-layers for p-i-n single junction solar cells. The current--voltage (I-V) characteristics of the cells were measured before and after the light soaking. The results suggest that the films deposited near the transition region have an optimum properties for application in solar cells. The cell with an i-layer prepared near the transition region shows the best stable performance.  相似文献   

17.
 采用表面热透镜技术,对3.8μm和2.8μm激光辐照下镀制在Si基底上的单层ZnS,YbF3和YBC薄膜及不同膜系的YbF3/ ZnS多层分光膜和多层高反膜,以及镀制在CaF2基底上的增透膜进行了吸收测量,并对3.8μm和2.8μm 激光的测量结果进行了比较分析。实验结果表明,2.8μm波长下的吸收比3.8μm的大得多,两者之间约相差一个量级,测得的多层高反膜YbF3/ZnS薄膜在的3.8μm处的最低吸收为4.57×10-4,测量系统的灵敏度约为10-5。  相似文献   

18.
We demonstrate the synthesis and investigate the electrical and optical characteristics of ‘nanocorals’ (NCs) composed of CuO/ZnO grown at low temperature through the hydrothermal approach. High-density CuO nanostructures (NSs) were selectively grown on ZnO nanorods (NRs). The synthesized NCs were used to fabricate p–n heterojunctions that were investigated by the current density–voltage (JV) and the capacitance–voltage (CV) techniques. It was found that the NC heterojunctions exhibit a well-defined diode behavior with a threshold voltage of about 1.52 V and relatively high rectification factor of ~760. The detailed forward JV characteristics revealed that the current transport is controlled by an ohmic behavior for V≤0.15 V, whereas at moderate voltages 1.46≤V<1.5 the current follows a J? α?exp(βV) relationship. At higher voltages (≥1.5 V) the current follows the relation J? α? V 2, indicating that the space-charge-limited current mechanism is the dominant current transport. The CV measurement indicated that the NC diode has an abrupt junction. The grown CuO/ZnO NCs exhibited a broad light absorption range that is covering the UV and the entire visible parts of the spectrum.  相似文献   

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