Department of Chemical Engineering & Applied Chemistry, University of Toronto, Toronto, ONM5S3E5, Canada.
Department of Physical & Environmental Sciences, Department of Chemistry, University of Toronto, Scarborough, ONM1C1A4, Canada.
J Am Chem Soc. 2022 Oct 26;144(42):19417-19429. doi: 10.1021/jacs.2c07423. Epub 2022 Oct 13.
Crystals are known to grow nonclassically or via four classical modes (the layer-by-layer, dislocation-driven, dendritic, and normal modes, which generally involve minimal interfacet surface diffusion). The field of nanoscience considers this framework to interpret how nanocrystals grow; yet, the growth of many anisotropic nanocrystals remains enigmatic, suggesting that the framework may be incomplete. Here, we study the solution-phase growth of pentatwinned Au nanorods without Br, Ag, or surfactants. Lower supersaturation conditions favored anisotropic growth, which appeared at variance with the known modes. Temporal electron microscopy revealed kinetically limited adatom funneling, as adatoms diffused asymmetrically along the vicinal facets (situated inbetween the {100} side-facets and {111} end-facets) of our nanorods. These vicinal facets were perpetuated throughout the synthesis and, especially at lower supersaturation, facilitated {100}-to-vicinal-to-{111} adatom diffusion. We derived a growth model from classical theory in view of our findings, which showed that our experimental growth kinetics were consistent with nanorods growing via two modes simultaneously: radial growth occurred via the layer-by-layer mode on {100} side-facets, whereas the asymmetric interfacet diffusion of adatoms to {111} end-facets mediated longitudinal growth. Thus, shape anisotropy was not driven by modulating the relative rates of monomer deposition on different facets, as conventionally thought, but rather by modulating the relative rates of monomer integration via interfacet diffusion. This work shows how controlling supersaturation, a thermodynamic parameter, can uncover distinct kinetic phenomena on nanocrystals, such as asymmetric interfacet surface diffusion and a fundamental growth mode for which monomer deposition and integration occur on different facets.
晶体的生长通常是非经典的,或者通过四种经典模式(逐层、位错驱动、枝晶和正常模式,这些模式通常涉及最小的界面表面扩散)。纳米科学领域认为这个框架可以解释纳米晶体的生长方式;然而,许多各向异性纳米晶体的生长仍然是个谜,这表明该框架可能不完整。在这里,我们研究了在没有 Br、Ag 或表面活性剂的情况下,在溶液相中生长的五重孪晶 Au 纳米棒。较低的过饱和度条件有利于各向异性生长,这与已知的模式不同。时间分辨电子显微镜揭示了动力学上受限的原子扩散漏斗,因为原子沿晶面的非对称扩散(位于{100}侧晶面和{111}端晶面之间)。这些晶面在整个合成过程中得以维持,尤其是在过饱和度较低的情况下,促进了{100}到晶面到{111}的原子扩散。鉴于我们的发现,我们从经典理论中推导出了一个生长模型,该模型表明我们的实验生长动力学与纳米棒通过两种模式同时生长的情况一致:在{100}侧晶面上通过逐层模式发生径向生长,而原子在界面的不对称扩散到{111}端晶面则介导了纵向生长。因此,形状各向异性不是通过调节单体在不同晶面上的沉积相对速率来驱动的,如传统观点所认为的那样,而是通过调节单体通过界面扩散的整合相对速率来驱动的。这项工作展示了如何通过控制过饱和度(热力学参数)来揭示纳米晶体上不同的动力学现象,例如不对称的界面表面扩散和单体沉积和整合发生在不同晶面的基本生长模式。