†Department of Electrical and Electronics Engineering, Department of Physics, UNAM-Institute of Materials Science and Nanotechnology, Bilkent University, Ankara 06800 Turkey.
‡Department of Physics, Abant Izzet Baysal University, Bolu 14280, Turkey.
ACS Nano. 2015 May 26;9(5):5041-50. doi: 10.1021/acsnano.5b01927. Epub 2015 May 12.
Here, we systematically investigated the spontaneous and stimulated emission performances of solution-processed atomically flat quasi-2D nanoplatelets (NPLs) as a function of their lateral size using colloidal CdSe core NPLs. We found that the photoluminescence quantum efficiency of these NPLs decreases with increasing lateral size while their photoluminescence decay rate accelerates. This strongly suggests that nonradiative channels prevail in the NPL ensembles having extended lateral size, which is well-explained by the increasing number of the defected NPL subpopulation. In the case of stimulated emission the role of lateral size in NPLs influentially emerges both in the single- and two-photon absorption (1PA and 2PA) pumping. In the amplified spontaneous emission measurements, we uncovered that the stimulated emission thresholds of 1PA and 2PA exhibit completely opposite behavior with increasing lateral size. The NPLs with larger lateral sizes exhibited higher stimulated emission thresholds under 1PA pumping due to the dominating defected subpopulation in larger NPLs. On the other hand, surprisingly, larger NPLs remarkably revealed lower 2PA-pumped amplified spontaneous emission thresholds. This is attributed to the observation of a "giant" 2PA cross-section overwhelmingly growing with increasing lateral size and reaching record levels higher than 10(6) GM, at least an order of magnitude stronger than colloidal quantum dots and rods. These findings suggest that the lateral size control in the NPLs, which is commonly neglected, is essential to high-performance colloidal NPL optoelectronic devices in addition to the vertical monolayer control.
在这里,我们系统地研究了胶体 CdSe 核 NPL 作为各向异性 2D 纳米片(NPL)的横向尺寸的函数的自发和受激发射性能。我们发现,这些 NPL 的光致发光量子效率随横向尺寸的增加而降低,而光致发光衰减率则加速。这强烈表明,在具有扩展横向尺寸的 NPL 中,非辐射通道占主导地位,这很好地解释了缺陷 NPL 子群数量的增加。在受激发射的情况下,横向尺寸在 NPL 中的作用在单光子和双光子吸收(1PA 和 2PA)泵浦中都明显显现出来。在放大自发发射测量中,我们发现 1PA 和 2PA 的受激发射阈值随横向尺寸的增加呈现出完全相反的行为。在 1PA 泵浦下,较大横向尺寸的 NPL 由于较大 NPL 中主导的缺陷子群而表现出较高的受激发射阈值。另一方面,令人惊讶的是,较大的 NPL 明显显示出较低的 2PA 泵浦放大自发发射阈值。这归因于观察到“巨大”的 2PA 截面随横向尺寸的增加而呈指数增长,并达到创纪录的水平,高于 10^6 GM,至少比胶体量子点和棒强一个数量级。这些发现表明,除了垂直单层控制之外,对高性能胶体 NPL 光电设备而言,对 NPL 进行横向尺寸控制是至关重要的,而这种控制通常被忽略。