Eslami Hossein, Gharibi Ali, Müller-Plathe Florian
Eduard-Zintl-Institut für Anorganische und Physikalische Chemie, Technische Universität Darmstadt, Alarich-Weiss-Str. 8, 64287 Darmstadt, Germany.
Department of Chemistry, College of Sciences, Persian Gulf University, 75168 Boushehr, Iran.
J Chem Theory Comput. 2021 Mar 9;17(3):1742-1754. doi: 10.1021/acs.jctc.0c01080. Epub 2021 Feb 2.
A model, including the chemical details of core nanoparticles as well as explicit surface charges and hydrophobic patches, of triblock Janus particles is employed to simulate nucleation and solid-solid phase transitions in two-dimensional layers. An explicit solvent and a substrate are included in the model, and hydrodynamic and many-body interactions were taken into account within many-body dissipative particle dynamics simulation. In order not to impose a mechanism a priori, we performed free (unbiased) simulations, leaving the system the freedom to choose its own pathways. In agreement with the experiment and previous biased simulations, a two-step mechanism for the nucleation of a kagome lattice from solution was detected. However, a distinct feature of the present unbiased biased simulations is that multiple nuclei emerge from the solution; upon their growth, the aligned and misaligned facets at the grain boundaries are introduced into the system. The liquid-like particles trapped between the neighboring nuclei connect them together. A mismatch in the symmetry planes of neighboring nuclei hinders the growth of less stable (smaller) nuclei. Unification of such nuclei at the grain boundaries of misaligned facets obeys a two-step mechanism: melting of the smaller nuclei, followed by subsequent nucleation of liquid-like particles at the interface of bigger neighboring nuclei. Besides, multiple postcritical nuclei are formed in the simulation box; the growth of some of which stops due to introduction of a strain in the system. Such an incomplete nucleation/growth mechanism is in complete agreement with the recent experiments. The solid-solid (hexagonal-to-kagome) phase transition, at weak superheatings, obeys a two-step mechanism: a slower step (formation of a liquid droplet), followed by a faster step (nucleation of kagome from the liquid droplet).
采用一种包含核心纳米颗粒化学细节以及明确表面电荷和疏水斑块的三嵌段Janus颗粒模型,来模拟二维层中的成核和固-固相变。模型中包含明确的溶剂和基底,并在多体耗散粒子动力学模拟中考虑了流体动力学和多体相互作用。为了不预先设定一种机制,我们进行了自由(无偏)模拟,让系统自由选择其自身的路径。与实验和先前的有偏模拟一致,检测到了从溶液中形成 kagome 晶格的两步机制。然而,当前无偏模拟的一个显著特征是溶液中出现多个核;在它们生长时,晶界处的对齐和未对齐晶面被引入系统。被困在相邻核之间的类液体粒子将它们连接在一起。相邻核的对称平面不匹配阻碍了较不稳定(较小)核的生长。在未对齐晶面的晶界处这些核的合并遵循两步机制:较小核的熔化,随后在较大相邻核的界面处类液体粒子的后续成核。此外,在模拟盒中形成了多个临界后核;其中一些的生长由于系统中引入的应变而停止。这种不完全的成核/生长机制与最近的实验完全一致。在弱过热度下,固-固(六方相到kagome相)相变遵循两步机制:较慢的步骤(形成液滴),随后是较快的步骤(从液滴中形成kagome晶格)。