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1.
通过仿真软件AFORS-HET对a-Si:H(p)/i-a-Si:H/c-Si(n)异质结太阳能电池的光伏特性进行分析及优化,主要对比了a-Si:H(p)层的均匀掺杂和表面掺杂浓度D1=1×1020 cm-3>界面掺杂浓度D2=4×1019 cm-3的梯度掺杂情况时的光伏特性,实现了在梯度掺杂时22.32%的光电转换效率。与均匀梯度掺杂相比,发射层的梯度掺杂除了引入一个附加电场,还优化了能带结构、光谱响应、表面复合速率。结果表明,梯度掺杂可以有效地改善电池的光电转换性能。 相似文献
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采用美国滨州大学研发的AMPS-1D软件,模拟了TCO与非晶硅界面势垒对TCO/a-Si:H(p+)/a-Si:H(i)/c-Si(n) /a-Si:H(i) /a-Si:H(n+) /TCO双面HIT异质结太阳电池光伏特性的影响。结果表明太阳电池的TCO/p+前接触界面势垒(对于电子)越高,越易形成欧姆接触,且电池的短波响应增强,使电池性能变好。模拟还发现,n+ /TCO背接触界面势垒(对于电子)越低,电池性能越好。若背场重掺杂,在背接触势垒小于等于0.5ev时,电池的转换效率不会受到背接触势垒的影响;若背场低掺杂,在背接触势垒很小的情况下,也能达到与重掺杂相同的转换效率。 相似文献
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采用美国滨州大学研发的AMPS-1D软件,模拟了TCO与非晶硅界面势垒对TCO/a-Si:H(p+)/a-Si:H(i)/c-Si(n)/a-Si:H(i) /a-Si:H(n+)/TCO双面HIT异质结太阳电池光伏特性的影响.结果表明太阳电池的TCO/p+前接触界面势垒(对于电子)越高,越易形成欧姆接触,且电池的短波响应增强,使电池性能变好.模拟还发现,n+/TCO背接触界面势垒(对于电子)越低,电池性能越好.若背场重掺杂,在背接触势垒小于等于0.5 eV时,电池的转换效率不会受到背接触势垒的影响;若背场低掺杂,在背接触势垒很小的情况下,也能达到与重掺杂相同的转换效率. 相似文献
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本文从a-Si:H体材料的缺陷态模型出发,考虑在a-Si:H/a-SiNx:H超晶格中由于空间电荷转移掺杂效应,以及界面不对称引起的a-Si:H阱层的能带下降和弯曲,严格求解空间电势分布和电荷分布,发现a-Si:H阱层中能带的下降值远大于由界面电荷不对称所引起的两端电势能差,且随转移到阱层中的电荷总量的变化非常敏感。空间电荷分布比较平缓,当不对称参数K=0.9时,空间电荷浓度的最大差值不到两倍。在此基础上,计算了超晶格中光电导的温度曲线,发现引起超晶格中暗电导和光电导相对于单层膜增大的主要原因是转移电荷量的多少,而界面电荷不对称的影响则小得多。计算中对带尾态采用Simmons-Taylor理论,考虑a-Si:H中悬挂键的相关性,并用巨正则分布讨论其在复合过程中的行为。
关键词: 相似文献
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通过异质结界面分析与 AMPS 模拟计算研究了 a-Si:H/c-Si 异质结太阳电池在低温工作、a-Si:H 层低掺杂、高价带补偿以及高界面态时光态 J-V 曲线出现 S-Shape 现象的物理过程,总结了 S-Shape 现象的物理原因.分析结果表明,当空穴输运受到界面势垒的限制时,空穴在 c-Si 界面附近聚集,能带重新分配,c-Si 耗尽区的电场减小,更多的电子从 c-Si 准中性区反转至 c-Si 界面及耗尽区与空穴复合,复合速率显著增大,光电流的损失显著增大,光态 J-V<
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模拟
异质结太阳电池
a-Si:H/c-Si 异质结 相似文献
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A. G. U. Perera S. G. Matsik M. B. M. Rinzan A. Weerasekara M. Alevli H. C. Liu M. Buchanan B. Zvonkov V. Gavrilenko 《Infrared Physics & Technology》2003,44(5-6):347-353
Results are presented on the effects of doping variation on the cutoff wavelength (λc) of homojunction interfacial workfunction internal photoemission far infrared detectors. The behavior at low doping (<1019 cm−3) is well predicted by the free carrier absorption model used previously. However at high doping the observed λc is much shorter than the values predicted by the workfunction obtained from Arrhenius plots. An explanation for the reduced λc in the high doping region is presented using a model for depletion of the heavy hole band due to direct transitions from the heavy hole to light hole band. 相似文献
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Based on the branching fractions of J/ψ(ψ(2S))→ VP from different collaborations, pseudoscalar mixing is extensively discussed with a well established phenomenological model. The mixing angle is determined to be -14° by fitting to the new world average if only quark content is considered. After taking into account the gluonic content in η and η' simultaneously, the investigation shows that η favors only consisting of light quarks, while the gluonic content of η' is Z2η', = 0.30±0.24. 相似文献
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邱宇 《原子与分子物理学报》2013,30(6)
基于扩展Su-Shrieffer-Heeger (SSH)模型,通过自洽计算的数值方法,研究了共轭高聚物链表现为孤子态和大极化子态两种不同晶格形态时链内的杂质分布情况,计算结果显示,分立的畴壁可导致高聚物链中形成多个稳定的势阱,有利于杂质在链中聚集分布。此外,还研究了在较高浓度的掺杂条件下,共轭高聚物链内的杂质分布规律。结果显示,杂质倾向于在中心区形成高浓度分布,而在链端区,杂质更倾向于离散分布。该研究表明,高浓度掺杂下杂质分布具有稳定的特征,晶格形态对杂质分布具有显著的影响,这些结论可为实验上操控杂质在共轭高聚物中的分布提供一定的帮助。 相似文献
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基于扩展Su-Shrieffer-Heeger(SSH)模型,通过自洽计算的数值方法,研究了共轭高聚物链表现为孤子态和大极化子态两种不同晶格形态时链内的杂质分布情况,计算结果显示,分立的畴壁可导致高聚物链中形成多个稳定的势阱,有利于杂质在链中聚集分布.此外,还研究了在较高浓度的掺杂条件下,共轭高聚物链内的杂质分布规律.结果显示,杂质倾向于在中心区形成高浓度分布,而在链端区,杂质更倾向于离散分布.该研究表明,高浓度掺杂下杂质分布具有稳定的特征,晶格形态对杂质分布具有显著的影响,这些结论可为实验上操控杂质在共轭高聚物中的分布提供一定的帮助. 相似文献
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Ye. S. Golubeva A. S. Iljinov E. Ya. Paryev I. A. Pshenichnov 《Zeitschrift für Physik A Hadrons and Nuclei》1993,345(2):223-226
A simple expression for the inclusive cross section of η production on light nuclei by protons has been obtained in the first collision approximation in the framework of the intranuclear cascade approach. An intranuclear cascade model which takes into account η production by primary proton and secondary pion, elastic scattering of η on intranuclear nucleons and absorption of η in nuclear matter has been developed. The calculated cross sections are found to be in satisfactory agreement with the experimental data. 相似文献
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Ivan A. Pshenichnyuk 《Physics letters. A》2018,382(7):523-527
The dynamics of quantum vortex pairs carrying heavy doping matter trapped inside their cores is studied. The nonlinear classical matter field formalism is used to build a universal mathematical model of a heavy vortex applicable to different types of quantum mixtures. It is shown how the usual vortex dynamics typical for undoped pairs qualitatively changes when heavy dopants are used: heavy vortices with opposite topological charges (chiralities) attract each other, while vortices with the same charge are repelled. The force responsible for such behavior appears as a result of superposition of vortices velocity fields in the presence of doping substance and can be considered as a special realization of the Magnus effect. The force is evaluated quantitatively and its inverse proportionality to the distance is demonstrated. The mechanism described in this paper gives an example of how a light nonlinear classical field may realize repulsive and attractive interactions between embedded heavy impurities. 相似文献
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The gluon and Goldstone boson induced tensor interaction effect on
the dibaryon mass and the D-wave decay width has been studied in
the quark delocalization, color screening model. The effective S-D
wave transition interactions induced by gluon and Goldstone boson exchanges decrease quickly as the increasing of the channel strangeness. The K and η meson tensor contribution is
negligible in this model. No six-quark state in the light flavor world can become a bound one by the help of these tensor interactions except the deuteron. The partial D-wave decay width
of IJp=\frac{1}{2}2+ NΩ state to spin 0, 1 ΛΞ
final state is 20.7 keV and 63.1 keV respectively. It is a very narrow
dibaryon resonance and might be detected in the
relativistic heavy ion reaction by the existing RHIC
detectors through the reconstruction of the ΛΞ vertex
mass and the future COMPAS detector at CERN and FAIR project
in Germany. 相似文献
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We studied doping CWO with several different dopant ions in order to create new heavy and fast scintillators by quenching the efficient but slow scintillation in CWO. Transmittance, excitation–emission spectra, decay time and the light yield were measured for the dopants of Cs, La, Si, Bi, Na, Nb and Pb. None of them caused efficient quenching. Trivalent ions seem to degrade crystal transparency, while monovalent ions do not seem to cause quenching. While heavy doping of Pb causes quenching to some extent, crystal growth is not easy for heavy doping. Heavy doping of the same wolframite structure crystal should be further examined. 相似文献
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We predict that the Auger hole-hole collision process involving a transition from the light hole band to the heavy hole band is an important recombination mechanism in non-degenerate p-type (Hg,Cd)Te. This is based on a comparison of the calculated lifetime for this mechanism with that due to the electron-electron collision mechanism discussed by Beattie and Landsberg which involves only the heavy hole valence band. We have estimated the ratio of the intrinsic lifetimes of these two mechanisms by approximating the integrals appearing in the lifetime expressions. We have determined the range of composition, temperature and doping density over which the Auger lifetime in p-type (Hg,Cd)Te is controlled by the light hole mechanism. 相似文献