Crystallization kinetics of atomic crystals revealed by a single-shot and single-particle X-ray diffraction experiment




Niozu Akinobu, Kumagai Yoshiaki, Hiraki Toshiyuki Nishiyama, Fukuzawa Hironobu, Motomura Koji, Bucher Maximilian, Asa Kazuki, Sato Yuhiro, Ito Yuta, You Daehyun, Ono Taishi, Li Yiwen, Kukk Edwin, Miron Catalin, Neagu Liviu, Callegari Carlo, Di Fraia Michele, Rossi Giorgio, Galli Davide Emilio, Pincelli Tommaso, Colombo Alessandro, Owada Shigeki, Tono Kensuke, Kameshima Takashi, Joti Yasumasa, Katayama Tetsuo, Togashi Tadashi, Yabashi Makina, Matsuda Kazuhiro, Bostedt Christoph, Ueda Kiyoshi, Nagaya Kiyonobu

PublisherNATL ACAD SCIENCES

2021

Proceedings of the National Academy of Sciences of the United States of America

PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA

P NATL ACAD SCI USA

e2111747118

118

51

8

0027-8424

1091-6490

DOIhttps://doi.org/10.1073/pnas.2111747118



Crystallization is a fundamental natural phenomenon and the ubiquitous physical process in materials science for the design of new materials. So far, experimental observations of the structural dynamics in crystallization have been mostly restricted to slow dynamics. We present here an exclusive way to explore the dynamics of crystallization in highly controlled conditions (i.e., in the absence of impurities acting as seeds of the crystallites) as it occurs in vacuum. We have measured the early formation stage of solid Xe nanoparticles nucleated in an expanding supercooled Xe jet by means of an X-ray diffraction experiment with 10-fs X-ray free-electron laser (XFEL) pulses. We found that the structure of Xe nanoparticles is not pure face-centered cubic (fcc), the expected stable phase, but a mixture of fcc and randomly stacked hexagonal close-packed (rhcp) structures. Furthermore, we identified the instantaneous coexistence of the comparably sized fcc and rhcp domains in single Xe nanoparticles. The observations are explained by the scenario of structural aging, in which the nanoparticles initially crystallize in the highly stacking-disordered rhcp phase and the structure later forms the stable fcc phase. The results are reminiscent of analogous observations in hard-sphere systems, indicating the universal role of the stacking-disordered phase in nucleation.



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