432 resultados para Voie P


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采用等离子体增强化学气相沉积技术和电子束蒸发技术制备了一种新型的线性缓变异质结变容二极管--Au/Cr合金(电极)/multi-layer(p)nc-Si:H/(n)c-Si/(电极)Au/Ge合金结构.I-V,C-V,G-f以及DLTS的测试结果表明:其电容变化系数远大于单晶硅线性缓变异质结的电容变化系数,正向导电机制符合隧穿辅助辐射-复合模型,这是nc-Si:H层中nc-Si晶粒的量子效应所致;反向电流主要由异质结中空间电荷区的产生电流决定,且反向漏电流小,反向击穿电压高,表现出较好的整流特性.

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采用正交实验设计方法设计p型GaN的生长,通过较少的实验,优化了影响p型GaN性质的三个生长参数:Mg流量、生长温度和Ⅴ/Ⅲ比.过量的Mg源流量、过高的生长温度、过大的Ⅴ/Ⅲ比都会降低自由空穴浓度.还研究了退火温度对p型GaN的载流子浓度和光学性质的影响.实验结果表明,700~750℃范围为最佳退火温度.

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该文报道了通过适当氢稀释(RH=15)和合适的衬底温度(Ts=170℃)下,用PECVD制备得到的宽带隙氢化纳米非晶硅(na-Si:H)薄膜,并将其用作pin太阳电池的本征层.经过电池结构和工艺条件的优化设计,在p/i,i/n界面插入渐变带隙缓冲层,制备出了glass/ITO/p-a-SiC:H/i-na-Si:H/n-nc-Si:H/Al结构的pin太阳电池.电池初始开路电压(Voc)高达0.94V,同时还能保证0.72的填充因子(FF).光电转换效率(Eff)达到8.35%(AM1.5,100mW/cm2).

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The results of second-order Raman-scattering experiments on n- and p-type 4H-SiC are presented,covering the acoustic and the optical overtone spectral regions.Some of the observed structures in the spectra are assigned to particular phonon branches and the points in the Brillouin zone from which the scattering originates.There exists a doublet at 626/636cm-1 with energy difference about 10cm-1 in both n- and p-type 4H-SiC,which is similar to the doublet structure with the same energy difference founded in hexagonal GaN,ZnO, and AlN.The cutoff frequency at 1926cm-1 of the second-order Raman is not the overtone of the A1(LO) peak of the n-type doping 4H-SiC,but that of the undoping one.The second-order Raman spectrum of 4H-SiC can hardly be affected by doping species or doping density.

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利用LPCVD方法在Si(100)衬底上获得了3C-SiC外延膜,扫描电子显微镜(SEM)研究表明3C-SiC/p—Si界面平整、光滑,无明显的坑洞形成。研究了以In和Al为接触电极的3C-SiC/p—Si异质结的I—V,C-V特性及I—V特性的温度依赖关系,比较了In电极的3C-SiC/p—Si异质结构和以SiGe作为缓冲层的3C-SiC/SiGe/p—Si异质结构的I—V特性,实验发现引入SiGe缓冲层后,器件的反向击穿电压由40V提高到70V以上。室温下A1电极3C-SiC/p—Si二极管的最大反向击穿电压接近100V,品质因子为1.95。

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本研究针对多晶硅p-n结光伏器件开展工作。基于倾斜光电转换器件的思想,倾斜本研究采用的光电转换器件使入射光线与器件表面法线成75度的夹角,从而使红外光在器件内形成多次全反射。这种内部全反射增加了光在器件内的光程,使得光在器件内的吸收得以增加。从采光的角度上发现,倾斜多晶硅光电转换器件可使器件的光电转换效率提高15%。此外,还发现了由倾斜器件造成开路电压稍微减小的现象并给予了解释。

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Highly oriented voids-free 3C-SiC heteroepitaxial layers are grown on φ50mm Si (100) substrates by low pressure chemical vapor deposition (LPCVD). The initial stage of carbonization and the surface morphology of carbonization layers of Si(100) are studied using reflection high energy electron diffraction (RHEED) and scanning electron microscopy (SEM). It is shown that the optimized carbonization temperature for the growth of voids-free 3S-SiC on Si (100) substrates is 1100 ℃. The electrical properties of SiC layers are characterized using Van der Pauw method. The I-V, C-V, and the temperature dependence of I-V characteristics in n-3C-SiC-p-Si heterojunctions with AuGeNi and Al electrical pads are investigated. It is shown that the maximum reverse breakdown voltage of the n-3C-SiC-p-Si heterojunction diodes reaches to 220V at room temperature. These results indicate that the SiC/Si heterojunction diode can be used to fabricate the wide bandgap emitter SiC/Si heterojunction bipolar transistors (HBT's).

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现在普遍采用ITO薄膜(In_2O_3:Sn)作为太阳电池的窗口材料,但由于In资源的稀缺,使太阳能电池的成本增加。Zn-O是一种低成本材料,具有良好的电学、光学特性,因此可代替ITO薄膜作为窗口材料。由于ZnO/n-Si异质结太阳电池的转化效率为6.9%~8.5%,而ITO光电转换效率为12%~15%,采用液态源掺杂方法,取得较好效果,证实了掺P、B对纳米ZnO薄膜提高导电性是有效的。本文利用扫描俄歇探针等手段研究分析了掺P、B随热处理温度的变化对纳米Zn-O薄膜电学特性的影响。在研制过程中,对掺入P、B的纳米Zn薄膜,曾采用X射线衍射议进行分析,其结果未见P、B。

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GaP:N绿色LED发光效率的提高有赖于对其结构参数的优化。根据载流子分布的连续性,由泊松方程自洽求解,得出了半导体n~--n结势垒分布的计算方法。在此基础上,计入n~-区内的电位降,计算了商用发光二极管p~+-n~-n结构的势垒分布,为整体结构的参数优化准备了必要的条件。

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采用常规等离子体增强化学气相沉积工艺,以高H_2稀释的SiH_4作为反应气体源和PH_3作为磷原子的参杂剂,在p型(100)单晶硅C(p)c-Si)衬底上,成功地生长了施主掺杂型纳米硅膜C(n)nc-Si:H),进而制备了(n)nc-Si;H/(p)c-Si异质结,并在230-420K温度范围内实验研究了该异质结的I-V特性。结果表明,(n)nc-Si:H/(p)c-Si异质结为一典型的突变异质结构,具有良好的温度稳定性和整流特性。正向偏压下,该异质结的电流输运机理为复合-隧穿模型。当正向偏压V_F<0.8V时,电流输运过程由复合机理所支配;而当V_F>1.0V时由隧穿机理决定。反向偏压下,该异质结具有良好的反向击穿持性。

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室温下在p-Si(100)上采用直流反应磁控溅射法外延生长了ZnO薄膜。XRD测量表明了ZnO是高度c轴单一取向生长的,XRC测量则表明了ZnO的高质量。在室温下的PL测量中见到了带边发射,其强度与晶体质量有关。

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于2010-11-23批量导入

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研究了MOVPE方法外延P型GaN和Al0.13 Ga0.87N的生长工艺,包括掺杂剂量和热退火条件,对材料电学性质的影响。得到了性能优良的P型材料,并研制了InGaN/AlGaN双异质结蓝光发光二极管。

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于2010-11-23批量导入

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利用光电流谱,结合X射线双晶衍射研究了快速退火对Si_(1-x)Ge/Si多量子阱p-i-n光电二极管的影响。由于应变SiGe的部分弛豫和Si-Ge互扩散,退火后的二极管的截止波长有显著的减小。但是,在750-850℃范围内,波长蓝移量随着退火温度的增加而变化缓慢,而样品的光电流强度却随温度是先减弱而后又增强,这可能主要是由于在不同温度退火过程中失配位错的产生和点缺陷的减小造成的。