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Structural and Optical Properties of Nonstoichiometric Titanium Hydride, Vanadium Hydride and Zirconium Hydride as Hot Carrier Solar Cell Absorbers

机译:非化学计量比氢化钛、氢化钒和氢化锆作为热载流子太阳能电池吸收剂的结构和光学性能

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Photovoltaic devices directly convert incident solar energy to electricity. Above bandgap incident photons excite carriers (electron and holes) deep into their respective bands. These excited carriers are called hot carriers and they undergo several physical loss processes to lose their excess energy to the lattice and thermalize to the band edge. In conventional photovoltaics, these carriers are collected from the band-edge before they recombine. The Hot Carrier Solar Cell (HCSC) is a promising third generation photovoltaics concept for energy loss reduction in solar cells by inhibiting the thermalization losses in the absorber. It has a limiting efficiency of 85%, well beyond the Shockley–Queisser limit of 33% which is the upper threshold for conventional photovoltaic cells e.g., Si solar cells. The primary mission of the hot carrier absorber engineering is to achieve a cooling rate of the carriers from 100s of picoseconds to nanoseconds, comparable to radiative recombination. One way to achieve a slower hot carrier cooling rate in the absorber is to acquire a phonon bottleneck effect. This would impede phonon assisted hot carrier relaxation. We have investigated the use of transition metal hydrides as HCSC absorber materials because of several potential advantages. The large atomic mass difference between the transition metal and hydrogen atoms leads to a large phononic band gap and a separation of the optical and acoustic phonon branches. This large phononic gap can inhibit the Klemens mechanism whereby longitudinal optical phonon decays into two acoustic phonons – the main route by which optical phonons decay - hence slowing down the hot carrier thermalization. In this work, we report on the fabrication and preliminary results of non-stoichiometric titanium hydride, vanadium hydride and zirconium hydride thin films for their quality and useability as HCSC absorbers. The thin films were prepared using electron beam evaporation and characterized using XRD, UV-VIS/IR, Ellipsometry and Raman spectroscopy. The results show that the amount of hydrogen in TiHx is such that x=1, for VHx x= 0.81 and for ZrHx x=1. From UV/VIS/IR, the reflection from all samples is dominated by a Pd layer used to prevent oxidation. The suitability of these materials as hot carrier absorbers is yet to be fully assessed, but the data presented here are important initial parameters in making that determination.
机译:光伏设备直接将入射的太阳能转化为电能。在带隙以上,入射光子激发了深入其各自带的载流子(电子和空穴)。这些激发的载流子被称为热载流子,它们经历了几个物理损耗过程,将多余的能量损失到晶格中,并热化到带边。在传统的光电技术中,这些载流子在重新组合之前从带边收集。热载流子太阳能电池(HCSC)是一种很有前途的第三代光伏概念,通过抑制吸收器中的热化损失来降低太阳能电池的能量损失。它的极限效率为85%,远远超过了33%的肖克利-奎塞尔极限,这是常规光伏电池(如硅太阳能电池)的上限。热载流子吸收工程的主要任务是实现载流子的冷却速度从100秒皮秒到纳秒,与辐射复合相当。在吸收体中实现较慢热载流子冷却速率的一种方法是获得声子瓶颈效应。这将阻碍声子辅助的热载流子弛豫。我们研究了过渡金属氢化物作为HCSC吸收剂材料的用途,因为它有几个潜在的优点。过渡金属原子和氢原子之间的原子质量差异大,导致声子带隙大,光学声子分支和声学声子分支分离。这种大的声子间隙可以抑制克莱门斯机制,即纵向光学声子衰变为两个声学声子——光学声子衰变的主要途径——从而减缓热载流子的热化。在这项工作中,我们报告了非化学计量比氢化钛、氢化钒和氢化锆薄膜的制备及其作为HCSC吸收剂的质量和可用性的初步结果。采用电子束蒸发法制备了薄膜,并用XRD、UV-VIS/IR、椭偏仪和拉曼光谱对其进行了表征。结果表明,TiH中的氢含量

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