Department of Chemistry , University of Washington , Seattle , Washington 98195-1700 , United States.
Nano Lett. 2019 Feb 13;19(2):1318-1325. doi: 10.1021/acs.nanolett.8b04905. Epub 2019 Jan 7.
A series of AgCu InS nanocrystals (NCs) spanning from 0 ≤ x ≤ ∼1 was synthesized by partial cation exchange to identify copper's contributions to the electronic structure and spectroscopic properties of these NCs. Discrete midgap states appear above the valence band upon doping AgInS NCs with Cu (small x). Density functional theory calculations confirm that these midgap states are associated with the 3d valence orbitals of the Cu impurities. With increasing x, these impurity d levels gradually evolve to become the valence-band edge of CuInS NCs, but the highest-occupied orbital's description does not change significantly across the entire range of x. In contrast with this gradual evolution, AgCu InS NC photoluminescence shifts rapidly with initial additions of Cu (small x) but then becomes independent of x beyond x > ∼0.20, all the way to CuInS ( x = 1.00). Data analysis suggests small but detectable hole delocalization in the luminescent excited state of CuInS NCs, estimated by Monte Carlo simulations to involve at most about four copper ions. These results provide unique insights into the luminescent excited states of these materials and they reinforce the description of CuInS NCs as "heavily copper-doped NCs" in which photogenerated holes are rapidly localized in copper 3d-based orbitals.
一系列 AgCuInS 纳米晶体(NCs),0 ≤ x ≤ ∼1,通过部分阳离子交换合成,以确定铜对这些 NCs 的电子结构和光谱性质的贡献。在掺杂 AgInS NCs 时,在价带上方出现离散的中场状态Cu(x 小)。密度泛函理论计算证实,这些中场状态与 Cu 杂质的 3d 价轨道有关。随着 x 的增加,这些杂质 d 能级逐渐演变为 CuInS NCs 的价带边缘,但整个 x 范围内最高占据轨道的描述没有显著变化。与这种逐渐演变形成对比的是,AgCuInS NC 光致发光随 Cu(x 小)的初始添加而迅速移动,但随后在 x > ∼0.20 之后与 x 无关,一直到 CuInS(x = 1.00)。数据分析表明,在 CuInS NCs 的发光激发态中存在小但可检测的空穴离域,通过蒙特卡罗模拟估计最多涉及约四个铜离子。这些结果为这些材料的发光激发态提供了独特的见解,并加强了 CuInS NCs 作为“严重铜掺杂 NCs”的描述,其中光生空穴迅速定域在铜 3d 轨道上。