Shih Cheng-Yu, Shugaev Maxim V, Wu Chengping, Zhigilei Leonid V
Department of Materials Science and Engineering, University of Virginia, 395 McCormick Road, Charlottesville, Virginia 22904-4745, USA.
Phys Chem Chem Phys. 2020 Apr 6;22(13):7077-7099. doi: 10.1039/d0cp00608d.
The generation of colloidal solutions of chemically clean nanoparticles through pulsed laser ablation in liquids (PLAL) has evolved into a thriving research field that impacts industrial applications. The complexity and multiscale nature of PLAL make it difficult to untangle the various processes involved in the generation of nanoparticles and establish the dependence of nanoparticle yield and size distribution on the irradiation parameters. Large-scale atomistic simulations have yielded important insights into the fundamental mechanisms of ultrashort (femtoseconds to tens of picoseconds) PLAL and provided a plausible explanation of the origin of the experimentally observed bimodal nanoparticle size distributions. In this paper, we extend the atomistic simulations to short (hundreds of picoseconds to nanoseconds) laser pulses and focus our attention on the effect of the pulse duration on the mechanisms responsible for the generation of nanoparticles at the initial dynamic stage of laser ablation. Three distinct nanoparticle generation mechanisms operating at different stages of the ablation process and in different parts of the emerging cavitation bubble are identified in the simulations. These mechanisms are (1) the formation of a thin transient metal layer at the interface between the ablation plume and water environment followed by its decomposition into large molten nanoparticles, (2) the nucleation, growth, and rapid cooling/solidification of small nanoparticles at the very front of the emerging cavitation bubble, above the transient interfacial metal layer, and (3) the spinodal decomposition of a part of the ablation plume located below the transient interfacial layer, leading to the formation of a large population of nanoparticles growing in a high-temperature environment through inter-particle collisions and coalescence. The coexistence of the three distinct mechanisms of the nanoparticle formation at the initial stage of the ablation process can be related to the broad nanoparticle size distributions commonly observed in nanosecond PLAL experiments. The strong dependence of the nanoparticle cooling and solidification rates on the location within the low-density metal-water mixing region has important implications for the long-term evolution of the nanoparticle size distribution, as well as for the ability to quench the nanoparticle growth or dope them by adding surface-active agents or doping elements to the liquid environment.
通过液体中的脉冲激光烧蚀(PLAL)生成化学纯净纳米颗粒的胶体溶液,已发展成为一个蓬勃发展的研究领域,并对工业应用产生影响。PLAL的复杂性和多尺度性质使得难以理清纳米颗粒生成过程中涉及的各种过程,也难以确定纳米颗粒产率和尺寸分布对辐照参数的依赖性。大规模原子模拟对超短(飞秒到几十皮秒)PLAL的基本机制产生了重要见解,并对实验观察到的双峰纳米颗粒尺寸分布的起源提供了合理的解释。在本文中,我们将原子模拟扩展到短(数百皮秒到纳秒)激光脉冲,并将注意力集中在脉冲持续时间对激光烧蚀初始动态阶段纳米颗粒生成机制的影响上。模拟中确定了在烧蚀过程的不同阶段以及在新兴空化泡的不同部分起作用的三种不同的纳米颗粒生成机制。这些机制是:(1)在烧蚀羽流与水环境的界面处形成薄的瞬态金属层,随后其分解成大的熔融纳米颗粒;(2)在新兴空化泡的最前端,瞬态界面金属层上方,小纳米颗粒的成核、生长和快速冷却/凝固;(3)位于瞬态界面层下方的部分烧蚀羽流的旋节分解,导致大量纳米颗粒在高温环境中通过颗粒间碰撞和聚结而生长。烧蚀过程初始阶段三种不同的纳米颗粒形成机制共存,可能与纳秒PLAL实验中通常观察到的宽纳米颗粒尺寸分布有关。纳米颗粒冷却和凝固速率对低密度金属 - 水混合区域内位置的强烈依赖性,对纳米颗粒尺寸分布的长期演变以及通过向液体环境中添加表面活性剂或掺杂元素来淬灭纳米颗粒生长或对其进行掺杂的能力具有重要意义。