Geuchies Jaco J, Dijkhuizen Robbert, Koel Marijn, Grimaldi Gianluca, du Fossé Indy, Evers Wiel H, Hens Zeger, Houtepen Arjan J
Optoelectronic Materials Section, Faculty of Applied Sciences, Delft University of Technology, Van der Maasweg 9, 2926 HZDelft, The Netherlands.
Department of Chemistry and Center for Nano and Biophotonics, Ghent University, 9000Ghent, Belgium.
ACS Nano. 2022 Nov 22;16(11):18777-18788. doi: 10.1021/acsnano.2c07519. Epub 2022 Oct 18.
Colloidal nanoplatelets (NPLs) are promising materials for lasing applications. The properties are usually discussed in the framework of 2D materials, where strong excitonic effects dominate the optical properties near the band edge. At the same time, NPLs have finite lateral dimensions such that NPLs are not true extended 2D structures. Here we study the photophysics and gain properties of CdSe/CdS/ZnS core-shell-shell NPLs upon electrochemical n doping and optical excitation. Steady-state absorption and PL spectroscopy show that excitonic effects are weaker in core-shell-shell nanoplatelets due to the decreased exciton binding energy. Transient absorption studies reveal a gain threshold of only one excitation per nanoplatelet. Using electrochemical doping, we observe the complete bleaching of the band edge exciton transitions. Combining electrochemical doping with transient absorption spectroscopy, we demonstrate that the gain threshold is fully removed over a broad spectral range and gain coefficients of several thousand cm are obtained. These doped NPLs are the best performing colloidal nanomaterial gain medium reported to date, with the lowest gain threshold and broadest gain spectrum and gain coefficients that are 4 times higher than in n-doped colloidal quantum dots. The low exciton binding energy due to the CdS and ZnS shells, in combination with the relatively small lateral size of the NPLs, results in excited states that are effectively delocalized over the entire platelet. Core-shell NPLs are thus on the border between strong confinement in QDs and dominant Coulombic effects in 2D materials. We demonstrate that this limit is in effect ideal for optical gain and that it results in an optimal lateral size of the platelets where the gain threshold per nm is minimal.
胶体纳米片(NPLs)是用于激光应用的有前景的材料。其性质通常在二维材料的框架内进行讨论,在二维材料中,强激子效应主导着带边附近的光学性质。同时,NPLs具有有限的横向尺寸,因此NPLs并非真正的扩展二维结构。在此,我们研究了电化学n型掺杂和光激发下CdSe/CdS/ZnS核壳壳结构NPLs的光物理性质和增益特性。稳态吸收光谱和光致发光光谱表明,由于激子结合能降低,核壳壳结构纳米片中的激子效应较弱。瞬态吸收研究揭示了每个纳米片仅一次激发的增益阈值。通过电化学掺杂,我们观察到带边激子跃迁的完全漂白。将电化学掺杂与瞬态吸收光谱相结合,我们证明在很宽的光谱范围内增益阈值被完全消除,并且获得了数千厘米的增益系数。这些掺杂的NPLs是迄今为止报道的性能最佳的胶体纳米材料增益介质,具有最低的增益阈值、最宽的增益光谱以及比n型掺杂的胶体量子点高4倍的增益系数。由于CdS和ZnS壳层导致的低激子结合能,再加上NPLs相对较小的横向尺寸,使得激发态有效地离域在整个薄片上。因此,核壳结构NPLs处于量子点中的强限制和二维材料中占主导的库仑效应之间的边界。我们证明这个界限实际上对于光学增益是理想的,并且它导致了薄片的最佳横向尺寸,此时每纳米的增益阈值最小。