Cu2O/Au混合光学天线中的共振能量传递和Purcell效应

IF 3.9 Q2 MATERIALS SCIENCE, MULTIDISCIPLINARY
Nishan Khatri, Ravi Teja Addanki Tirumala, Susheng Tan, Marimuthu Andiappan, Ali Kaan Kalkan
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引用次数: 0

摘要

亚波长结构中的光捕获是一种迷人的效应,激发了太阳能收集的创新技术,如光催化和光伏发电。在这些应用中,困在激发Mie模式中的能量必须有效地转换为载流子并由载流子传输。为此,共振能量转移(RET)是一种有益的机制,可以规避电荷传输到电极的挑战。本文采用单粒子光散射和荧光光谱技术研究了在Au表面上直径为48 ~ 64 nm的Cu2O纳米球。将这种混合Cu2O/Au光学天线(OA)建模为振荡器,其中从激发的混合Mie模式到Au薄膜的RET被描述为阻尼通道(除了散射和吸收外),我们测量了532 nm激发的RET概率为70±9%。OA还以相反的方向介导RET,从Au中激发的电子-空穴对到谐振器模式,然后是光子发射(散射),使Au的荧光量子产率提高到1.3 × 105倍。这种巨大的Purcell增强归因于Cu2O/Au界面周围的光子态浓度高,与发射器(耦合Au体积)在空间上重叠,以及Cu2O颗粒中的低吸收和散射阻尼(即偶极子禁止间隙和较小的颗粒尺寸)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Resonance Energy Transfer and Purcell Effect in a Cu2O/Au Hybrid Optical Antenna

Resonance Energy Transfer and Purcell Effect in a Cu2O/Au Hybrid Optical Antenna

Light trapping in subwavelength structures is a fascinating effect inspiring innovative technologies for solar energy harvesting, such as photocatalysis and photovoltaics. In these applications, energy trapped in an excited Mie mode must be efficiently converted to and transported by charge carriers. To this end, resonance energy transfer (RET) is a beneficial mechanism circumventing the challenge of charge transport to electrodes. Here, 48–64 nm diameter Cu2O nanospheres on Au are investigated by single-particle light scattering and fluorescence spectroscopies. Modeling such a hybrid Cu2O/Au optical antenna (OA) as an oscillator, where RET from the excited hybrid Mie mode to Au film is described as a damping channel (in addition to scattering and absorption), we measure a RET probability of 70 ± 9% for 532 nm excitation. The OA also mediates RET in the reverse direction, from an excited electron-hole pair in Au to the resonator mode, followed by photon emission (scattering) that enhances fluorescence quantum yield of Au up to 1.3 × 105 times. This giant Purcell enhancement is attributed to strong concentration of the photon states around the Cu2O/Au interface which spatially overlap with the emitter (coupled Au volume) along with low absorption and scattering damping in Cu2O particles (i.e., dipole-forbidden gap and smaller particle size).

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