ICFO - Institut de Ciencies Fotoniques, The Barcelona Institute of Science and Technology, 08860Castelldefels, Barcelona, Spain.
Departament de Física, Universitat Politècnica de Catalunya, Terrassa08222, Spain.
J Phys Chem Lett. 2023 Feb 23;14(7):1999-2005. doi: 10.1021/acs.jpclett.2c03585. Epub 2023 Feb 16.
Understanding the spatial dynamics of nanoscale exciton transport beyond the temporal decay is essential for further improvements of nanostructured optoelectronic devices, such as solar cells. The diffusion coefficient () of the nonfullerene electron acceptor Y6 has so far only been determined indirectly, from singlet-singlet annihilation (SSA) experiments. Here, we present the full picture of the exciton dynamics, adding the spatial domain to the temporal one, by spatiotemporally resolved photoluminescence microscopy. In this way, we directly track diffusion and we are able to decouple the real spatial broadening from its overestimation given by SSA. We measured the diffusion coefficient, = 0.017 ± 0.003 cm/s, which gives a Y6 film diffusion length of nm. Thus, we provide an essential tool that enables a direct and free-of-artifacts determination of diffusion coefficients, which we expect to be pivotal for further studies on exciton dynamics in energy materials.
了解纳米级激子输运的时空动力学对于进一步改进纳米结构光电设备(如太阳能电池)至关重要。到目前为止,非富勒烯电子受体 Y6 的扩散系数()仅通过单重态-单重态湮灭(SSA)实验间接确定。在这里,我们通过时空分辨光致发光显微镜将时间域扩展到空间域,呈现出激子动力学的全貌。通过这种方式,我们可以直接跟踪扩散,并能够将真实的空间展宽与其由 SSA 引起的高估区分开来。我们测量的扩散系数为 = 0.017 ± 0.003 cm/s,这给出了 Y6 薄膜的扩散长度为 nm。因此,我们提供了一种重要的工具,可以直接、无伪影地确定扩散系数,我们预计这对于进一步研究能量材料中的激子动力学至关重要。