ARC Centre of Excellence in Exciton Science, School of Chemistry, and Bio21 Institute, University of Melbourne , Parkville, Victoria 3010, Australia.
Acc Chem Res. 2017 Dec 19;50(12):2925-2935. doi: 10.1021/acs.accounts.7b00313. Epub 2017 Nov 16.
The phenomenon of symmetry breaking-in which the order of symmetry of a system is reduced despite manifest higher-order symmetry in the underlying fundamental laws-is pervasive throughout science and nature, playing a critical role in fields ranging from particle physics and quantum theory to cosmology and general relativity. For the growth of crystals, symmetry breaking is the crucial step required to generate a macroscopic shape that has fewer symmetry elements than the unit cell and/or seed crystal from which it grew. Advances in colloid synthesis have enabled a wide variety of nanocrystal morphologies to be achieved, albeit empirically. Of the various nanoparticle morphologies synthesized, gold nanorods have perhaps been the most intensely studied, thanks largely to their unique morphology-dependent optical properties and exciting application potential. However, despite intense research efforts, an understanding of the mechanism by which a single crystal breaks symmetry and grows anisotropically has remained elusive, with many reports presenting seemingly conflicting data and theories. A fundamental understanding of the symmetry breaking process is needed to provide a rational framework upon which future synthetic approaches can be built. Inspired by recent experimental results and drawing upon the wider literature, we present a mechanism for gold nanorod growth from the moments prior to symmetry breaking to the final product. In particular, we describe the steps by which a cuboctahedral seed particle breaks symmetry and undergoes anisotropic growth to form a nanorod. With an emphasis on the evolving crystal structure, we highlight the key geometrical and chemical drivers behind the symmetry breaking process and factors that govern the formation and growth of nanorods, including control over the crystal width, length, and surface faceting. We propose that symmetry breaking is induced by an initial formation of a new surface structure that is stabilized by the deposition of silver, thus preserving this facet in the embryonic nanorod. These new surfaces initially form stochastically as truncations that remove high-energy edge atoms at the intersection of existing {111} facets and represent the beginnings of a {011}-type surface. Crucially, the finely tuned [HAuCl]:[AgNO] ratio and reduction potential of the system mean that silver deposition can occur on the more atomically open surface but not on the pre-existing lower-index facets. The stabilized surfaces develop into side facets of the nascent nanorod, while the largely unpassivated {111} facets are the predominant site of Au atom deposition. Growth in the width direction is tightly controlled by a self-sustaining cycle of galvanic replacement and silver deposition. It is the [HAuCl]:[AgNO] ratio that directly determines the particle size at which the more open atomic surfaces can be stabilized by silver and the rate of growth in the width direction following symmetry breaking, thus explaining the known aspect ratio control with Ag ion concentration. We describe the evolving surface faceting of the nanorod and the emergence of higher-index facets. Collectively, these observations allow us to identify facet-size and edge-atom effects as a simple fundamental driver of symmetry breaking and the subsequent development of new surfaces in the presence of adsorbates.
对称破缺现象——尽管基础定律中存在更高阶的对称性,但系统的对称性顺序却降低了——在科学和自然界中普遍存在,在从粒子物理和量子理论到宇宙学和广义相对论等领域都起着关键作用。对于晶体的生长而言,对称破缺是生成宏观形状所必需的关键步骤,因为该形状的对称元素比其生长的单元晶胞和/或晶种要少。胶体合成的进步使得能够实现各种纳米晶体形态,尽管这是经验性的。在所合成的各种纳米颗粒形态中,金纳米棒受到的研究最为深入,这在很大程度上要归功于其独特的形态依赖性光学特性和令人兴奋的应用潜力。然而,尽管进行了大量的研究工作,但对于单个晶体如何打破对称性并进行各向异性生长的机制仍难以理解,许多报告提出了看似相互矛盾的数据和理论。需要深入了解对称破缺过程,才能为未来的合成方法提供合理的框架。受最近的实验结果的启发,并借鉴更广泛的文献,我们提出了从对称破缺之前到最终产物的金纳米棒生长机制。特别是,我们描述了从具有立方八面体种子颗粒的对称性破坏到各向异性生长形成纳米棒的步骤。我们特别强调了不断变化的晶体结构,突出了对称破缺过程背后的关键几何和化学驱动力以及控制纳米棒形成和生长的因素,包括对晶体宽度、长度和表面分形的控制。我们提出,对称破缺是由新表面结构的初始形成引起的,该表面结构通过银的沉积而稳定,从而在胚胎纳米棒中保留了该表面。这些新表面最初作为随机形成的截形而形成,截形去除了现有{111}面相交处的高能边缘原子,代表了{011}型表面的开始。至关重要的是,精细调节的[HAuCl]:[AgNO]比和系统的还原电位意味着银的沉积可以发生在原子更开放的表面上,但不能发生在预先存在的低指数面。稳定的表面发展成新生纳米棒的侧表面,而大部分未钝化的{111}面是 Au 原子沉积的主要位置。在宽度方向上的生长受到自维持的电置换和银沉积循环的紧密控制。正是[HAuCl]:[AgNO]比直接决定了可以通过银稳定的更开放原子表面的尺寸,以及对称破缺后宽度方向的生长速率,从而解释了已知的与 Ag 离子浓度有关的纵横比控制。我们描述了纳米棒的表面分形的演变和更高指数面的出现。总之,这些观察结果使我们能够将表面尺寸和边缘原子效应确定为对称破缺的简单基本驱动因素,以及在吸附剂存在下新表面的后续发展。