论文标题
用于近场嗜热伏洛尔特设备的砷氧化胺细胞的设计
Design of an indium arsenide cell for near-field thermophotovoltaic devices
论文作者
论文摘要
具有金色前触点的砷氧化胺光伏电池设计用于近场嗜热伏洛耐(NF-TPV)设备,该设备由毫米尺寸的表面组成,该设备由纳米化真空间隙隔开。该设备用掺杂的硅散热器保持在800 K的温度下。光伏电池的结构,包括发射极和基础厚度,底座的掺杂水平以及前触点网格参数,可优化,以最大化NF-TPV功率输出。这是通过通过波动电动力学和少数式荷载载流子连续性方程在电池中求解辐射和电荷传输的方法,此外还可以考虑由于前触点和前面触点和底物引入的其他串联电阻损失引起的阴影损失。结果表明,这些额外的损失机制以不可忽略的方式对NF-TPV的性能产生负面影响,并且最大功率输出是阴影损失与前触点引入的串联电阻损失之间的权衡。例如,当在100 nm的真空间隙以1 x 1 mm2设备进行优化的单元格时,与不存在前面接触网格的理想化情况相比,前触点引入的损失将最大功率输出降低约2.5倍。 If the optimized grid for the 1 x 1 mm2 device is scaled up for a 5 x 5 mm2 device, the maximum power output is only increased by a factor of ~ 1.08 with respect to the 1 x 1 mm2 case despite an increase of the surface area by a factor of 25. This work demonstrates that the photovoltaic cell in a NF-TPV device must be designed not only for a specific radiator temperature, but also for specific gap thickness and device surface area.
An indium arsenide photovoltaic cell with gold front contacts is designed for use in a near-field thermophotovoltaic (NF-TPV) device consisting of millimeter-size surfaces separated by a nanosize vacuum gap. The device operates with a doped silicon radiator maintained at a temperature of 800 K. The architecture of the photovoltaic cell, including the emitter and base thicknesses, the doping level of the base, and the front contact grid parameters, are optimized for maximizing NF-TPV power output. This is accomplished by solving radiation and charge transport in the cell via fluctuational electrodynamics and the minority charge carrier continuity equations, in addition to accounting for the shading losses due to the front contacts and additional series resistance losses introduced by the front contacts and the substrate. The results reveal that these additional loss mechanisms negatively affect NF-TPV performance in a non-negligible manner, and that the maximum power output is a trade-off between shading losses and series resistance losses introduced by the front contacts. For instance, when the cell is optimized for a 1 x 1 mm2 device operating at a vacuum gap of 100 nm, the losses introduced by the front contacts reduce the maximum power output by a factor of ~ 2.5 compared to the idealized case when no front contact grid is present. If the optimized grid for the 1 x 1 mm2 device is scaled up for a 5 x 5 mm2 device, the maximum power output is only increased by a factor of ~ 1.08 with respect to the 1 x 1 mm2 case despite an increase of the surface area by a factor of 25. This work demonstrates that the photovoltaic cell in a NF-TPV device must be designed not only for a specific radiator temperature, but also for specific gap thickness and device surface area.