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From the Laser-doped Semiconductor Fingers to the Advanced Semiconductor Fingers Silicon Solar Cell

机译:从激光掺杂的半导体指到先进的半导体指硅太阳能电池

摘要

To reach the goal of grid parity for photovoltaic-generated power, the efficiency ofconventional screen-printed p-type silicon solar cells should be increased withoutsignificant increase in the manufacturing cost. The semiconductor fingers (SCF)screen-printed silicon solar cell technology fabricated by laser-doping the SCF canpotentially achieve this aim. Previous laser-doped SCF p-type silicon solar cellefficiencies were too low, limited by the achievable SCF doping and therefore sheetresistance levels using available laser technology. Recently, the new Spectra PhysicsMillennia Prime laser introduced new laser technology apparently with the potentialto produce laser-doped features with sheet resistances low enough for the SCF cell.The objective of this thesis is to design and develop an n-type SCF with this laser soas to demonstrate high efficiency laser-doped SCF solar cells on p-type Czochralski(Cz) silicon wafers.Since the sheet resistance of the laser-doped SCF (lines) is important to the efficiencyof the SCF solar cell, appropriate methods to measure the sheet resistance of theselaser-doped lines were investigated. A method widely-used to measure the sheetresistance of a laser-doped line was demonstrated here to produce unreliable resultsand thus not used. Instead, a new measurement method was presented along with anew upper sheet resistance limit concept. A theory was also presented that relatesthese two different measurement methods, and was experimentally-supported withinan error of 10 %. The Spectra Physics laser was also demonstrated to produce laserdopedlines that can be as conductive as 2 Ω/□. Thus, this laser is suitable for highefficiency SCF solar cells.Beside the benefits that highly-conductive SCF can bring to a SCF cell, there aredrawbacks that appear mainly in the form of SCF effective shading losses. To accountfor them, a model was built to simulate the efficiencies of laser-doped SCF solar cellswith different SCF sheet resistance and junction depths. The cell efficiency potentialof SCF laser-doped by the Spectra Physics laser was then assessed. With the most optimistic assumptions for contact resistance, and with experimentally-derived SCFsheet resistances and junction depths, the highest efficiency was predicted to be 18.81% and was only 1.13 % relatively higher than that of an optimised screen-printedsilicon solar cell. High SCF effective shading loss was the limiting factor.Subsequently, laser-doped SCF solar cells screen-printed with appropriate lowreactivitysilver pastes were fabricated. From these cells, the contact resistance wasdetermined to be too high and not uniform enough for high efficiency laser-dopedSCF solar cells from being demonstrated in the duration of this thesis work.Plating the SCF with metal was then proposed as a solution that can overcome bothchallenges of high effective shading loss and low contact quality. This new metalplatedSCF solar cell is known as the advanced SCF solar cell. A laser-doping andmetallisation sequence in the order of screen-printing, laser-doping, and nickel/copperstack plating was analysed to be a practical sequence to fabricate the advanced SCFcell. During the development of the recipe, nickel was found to not uniformly plateacross the cell and these nickel voids resulted in higher series resistance levels. Amodified dopant dispense method for the laser-doping step was developed tosignificantly reduce these nickel voids. By applying this solution to a batch of sixadvanced SCF solar cells, an average batch and highest efficiency of 18.40 % and18.82 % respectively were achieved on p-type Cz 1 Ωcm textured silicon wafers.Modelling and simulation of the advanced SCF solar cell show that this new celldesign can have a direct ≈ 0.7 % absolute and ≈ 3.8 % relative efficiency gain over thelaser-doped SCF solar cell. This is mainly due to the ability of the advanced SCF solarcell to space the screen-printed silver fingers much wider apart and to use narrowerSCF. The predicted efficiency potential of the advanced SCF solar cell with a full areaback surface field exceeds 20 %.Of secondary importance and it was discovered while developing techniques tominimise the contact resistance between a screen-printed metal and a high sheetresistance diffused emitter, that using dilute hydrofluoric acid to improve the contactresistance can increase the cell’s recombination impact and reduce its pseudo-fillfactor. It was also demonstrated that by treating the cell in phosphoric acid, this impactcan be significantly reduced or eliminated. Chemical analyses suggest lead to be thelikely recombination source.
机译:为了达到光伏发电的同等发电量的目标,应提高常规的丝网印刷p型硅太阳能电池的效率,而不会显着增加制造成本。通过对SCF进行激光掺杂而制造的半导体指(SCF)丝网印刷硅太阳能电池技术有可能实现这一目标。先前的激光掺杂SCF p型硅太阳能电池效率太低,受可实现的SCF掺杂以及因此使用可用激光技术的薄层电阻水平所限制。最近,新的Spectra PhysicsMillennia Prime激光器引入了新的激光技术,显然有潜力生产出掺杂激光的特征,其薄层电阻对于SCF电池而言足够低。以演示在p型Czochralski(Cz)硅晶片上的高效激光掺杂SCF太阳能电池。由于激光掺杂SCF(线)的薄层电阻对于SCF太阳能电池的效率很重要,因此测量薄板的合适方法研究了这些掺激光线的电阻。这里展示了一种广泛用于测量激光掺杂线的薄层电阻的方法,该方法产生的结果不可靠,因此没有使用。取而代之的是,提出了一种新的测量方法以及一个新的薄层电阻上限概念。还提出了将这两种不同的测量方法相关联的理论,并得到了实验支持,误差在10%以内。还证明了Spectra Physics激光器产生的激光掺杂线可导电至2Ω/□。因此,该激光器适用于高效SCF太阳能电池。高导电性SCF可以为SCF电池带来好处,但缺点是主要以SCF有效遮光损失的形式出现。为了解决这些问题,建立了一个模型来模拟具有不同SCF薄层电阻和结深度的激光掺杂SCF太阳能电池的效率。然后评估由Spectra Physics激光器掺杂的SCF激光器的电池效率潜力。在最乐观的接触电阻假设下,并根据实验得出的SCFsheet电阻和结深度,预计最高效率为18.81%,仅比优化的丝网印刷硅太阳能电池高1.13%。高的SCF有效遮光损失是限制因素。随后,制造了用适当的低反应性银浆丝网印刷的激光掺杂SCF太阳能电池。从这些电池的接触电阻被确定为太高,并且在本论文的研究过程中无法证明其对高效激光掺杂的SCF太阳能电池而言不够均匀。然后提出了用金属镀SCF作为可以克服两个挑战的解决方案有效遮光损失高,接触质量低。这种新型的镀金属SCF太阳能电池被称为先进的SCF太阳能电池。分析了丝网印刷,激光掺杂和镍/铜堆叠镀层的激光掺杂和金属化顺序,这是制造高级SCFcell的实用顺序。在配方开发过程中,发现镍不能均匀地镀覆在整个电池上,并且这些镍空洞导致更高的串联电阻水平。开发了用于激光掺杂步骤的改进的掺杂剂分配方法,以显着减少这些镍空隙。通过将该解决方案应用于一批六个先进的SCF太阳能电池,在p型Cz 1Ωcm纹理硅晶片上平均分别获得了18.40%和18.82%的最高效率。与掺入激光的SCF太阳能电池相比,这种新的电池设计可直接带来约0.7%的绝对绝对值和3.8%的相对效率增益。这主要是由于先进的SCF太阳能电池能够将丝网印刷的银指间隔得更宽,并能使用更窄的SCF。具有整个背表面场的先进SCF太阳能电池的预测效率潜力超过20%。改善接触电阻的氢氟酸可以增加电池的重组影响并降低其假填充因子。还证明了通过用磷酸处理细胞,可以显着减少或消除这种影响。化学分析表明,铅可能是重组来源。

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