Research Institute for Electronic Science, Hokkaido University, Sapporo, Japan.
Acc Chem Res. 2011 Apr 19;44(4):251-60. doi: 10.1021/ar100117w. Epub 2011 Mar 7.
Efficient solar energy conversion has been vigorously pursued since the 1970s, but its large-scale implementation hinges on the availability of high-efficiency modules. For maximum efficiency, it is important to absorb most of the incoming radiation, which necessitates both efficient photoexcitation and minimal electron-hole recombination. To date, researchers have primarily focused on the latter difficulty: finding a strategy to effectively separate photoinduced electrons and holes. Very few reports have been devoted to broadband sunlight absorption and photoexcitation. However, the currently available photovoltaic cells, such as amorphous silicon, and even single-crystal silicon and sensitized solar cells, cannot respond to the wide range of the solar spectrum. The photoelectric conversion characteristics of solar cells generally decrease in the infrared wavelength range. Thus, the fraction of the solar spectrum absorbed is relatively poor. In addition, the large mismatch between the diffraction limit of light and the absorption cross-section makes the probability of interactions between photons and cell materials quite low, which greatly limits photoexcitation efficiency. Therefore, there is a pressing need for research aimed at finding conditions that lead to highly efficient photoexcitation over a wide spectrum of sunlight, particularly in the visible to near-infrared wavelengths. As characterized in the emerging field of plasmonics, metallic nanostructures are endowed with optical antenna effects. These plasmonic antenna effects provide a promising platform for artificially sidestepping the diffraction limit of light and strongly enhancing absorption cross-sections. Moreover, they can efficiently excite photochemical reactions between photons and molecules close to an optical antenna through the local field enhancement. This technology has the potential to induce highly efficient photoexcitation between photons and molecules over a wide spectrum of sunlight, from visible to near-infrared wavelengths. In this Account, we describe our recent work in using metallic nanostructures to assist photochemical reactions for augmenting photoexcitation efficiency. These studies investigate the optical antenna effects of coupled plasmonic gold nanoblocks, which were fabricated with electron-beam lithography and a lift-off technique to afford high resolution and nanometric accuracy. The two-photon photoluminescence of gold and the resulting nonlinear photopolymerization on gold nanoblocks substantiate the existence of enhanced optical field domains. Local two-photon photochemical reactions due to weak incoherent light sources were identified. The optical antenna effects support the unprecedented realization of (i) direct photocarrier injection from the gold nanorods into TiO(2) and (ii) efficient and stable photocurrent generation in the absence of electron donors from visible (450 nm) to near-infrared (1300 nm) wavelengths.
自 20 世纪 70 年代以来,人们一直在大力研究高效的太阳能转换,但要实现其大规模应用,关键在于获得高效的模块。为了达到最高的效率,重要的是吸收大部分入射辐射,这就需要高效的光激发和最小的电子-空穴复合。迄今为止,研究人员主要集中在后者的困难上:找到一种有效分离光诱导电子和空穴的策略。很少有报道致力于宽带阳光吸收和光激发。然而,目前可用的光伏电池,如非晶硅,甚至单晶硅和敏化太阳能电池,都不能响应宽范围的太阳光谱。太阳能电池的光电转换特性通常在红外波长范围内下降。因此,吸收的太阳光谱部分相对较差。此外,光的衍射极限与吸收截面之间的大不匹配使得光子与材料之间相互作用的概率非常低,这极大地限制了光激发效率。因此,迫切需要研究如何在宽光谱的太阳光下实现高效光激发的条件,特别是在可见光到近红外波长范围内。正如等离子体学这一新兴领域所描述的,金属纳米结构具有光学天线效应。这些等离子体天线效应为人工规避光的衍射极限和强烈增强吸收截面提供了一个很有前途的平台。此外,它们可以通过局部场增强有效地激发光子和靠近光学天线的分子之间的光化学反应。这项技术有可能在从可见到近红外波长的宽光谱范围内诱导光子和分子之间的高效光激发。在本报告中,我们描述了我们最近使用金属纳米结构辅助光化学反应来提高光激发效率的工作。这些研究探讨了耦合等离子体金纳米块的光学天线效应,这些纳米块是通过电子束光刻和剥离技术制造的,以实现高分辨率和纳米级精度。金的双光子光致发光和由此产生的金纳米块上的非线性光聚合证实了增强光场域的存在。确定了由于弱非相干光源引起的局部双光子光化学反应。光学天线效应支持前所未有的实现(i)金纳米棒直接将光载流子注入 TiO(2),以及(ii)在没有电子给体的情况下,从可见光(450nm)到近红外(1300nm)波长高效且稳定的光电流产生。