Abstract
Crystals melt when thermal excitations or the concentration of defects in the lattice is sufficiently high. Upon melting, the crystalline long-range order vanishes, turning the solid to a fluid. In contrast to this classical scenario of solid melting, here a counter-intuitive behavior of the occurrence of crystalline long-range order in an initially disordered matrix is demonstrated. This unusual solidification is demonstrated in a system of passive colloidal particles accommodating chemically active defects—photocatalytic Janus particles. The observed crystallization occurs when the amount of active-defect-induced fluctuations (which is the measure of the effective temperature) reaches critical value. The driving mechanism behind this unusual behavior is purely internal and resembles a blast-induced solidification. Here, the role of “internal micro-blasts” is played by the photochemical activity of defects residing in the colloidal matrix. The defect-induced solidification occurs under non-equilibrium conditions: the resulting solid exists as long as a constant supply of energy in the form of ion flow is provided by the catalytic photochemical reaction at the surface of active Janus particle defects. The findings could be useful for the understanding of the phase transitions of matter under extreme conditions far from thermodynamic equilibrium.
Original language | English |
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Article number | 2003851 |
Journal | Advanced Functional Materials |
Volume | 30 |
Issue number | 39 |
DOIs | |
Publication status | Published - 1 Sep 2020 |
Bibliographical note
Funding Information:The authors thank B. Kruppke (TU Dresden) for support with the SEM measurements, B. Ibarlucea (TU Dresden) and A. Caspari (IPF) for Zeta potential measurements. This work was supported in part via the German Research Foundation (DFG) via DFG grants BA 4986/7‐1, MA 5144/9‐1, MA 5144/13‐1, MA 5144/14‐1. T.H. acknowledges the China Scholarship Council (CSC) for financial support. V.R.M. and F.N. acknowledge support by the Research Foundation‐Flanders (FWO‐Vl) and Japan Society for the Promotion of Science (JSPS) (JSPS‐FWO Grant No. VS.059.18N). F.N. is supported in part by the NTT Research, Army Research Office (ARO) (Grant No. W911NF‐18‐1‐0358), Japan Science and Technology Agency (JST) (via the CREST Grant No. JPMJCR1676), Japan Society for the Promotion of Science (JSPS) (via the KAKENHI Grant No. JP20H00134, and the grant JSPS‐RFBR Grant No. JPJSBP120194828), and the Grant No. FQXi‐IAF19‐06 from the Foundational Questions Institute Fund (FQXi), a donor advised fund of the Silicon Valley Community Foundation.
Funding Information:
The authors thank B. Kruppke (TU Dresden) for support with the SEM measurements, B. Ibarlucea (TU Dresden) and A. Caspari (IPF) for Zeta potential measurements. This work was supported in part via the German Research Foundation (DFG) via DFG grants BA 4986/7-1, MA 5144/9-1, MA 5144/13-1, MA 5144/14-1. T.H. acknowledges the China Scholarship Council (CSC) for financial support. V.R.M. and F.N. acknowledge support by the Research Foundation-Flanders (FWO-Vl) and Japan Society for the Promotion of Science (JSPS) (JSPS-FWO Grant No. VS.059.18N). F.N. is supported in part by the NTT Research, Army Research Office (ARO) (Grant No. W911NF-18-1-0358), Japan Science and Technology Agency (JST) (via the CREST Grant No. JPMJCR1676), Japan Society for the Promotion of Science (JSPS) (via the KAKENHI Grant No. JP20H00134, and the grant JSPS-RFBR Grant No. JPJSBP120194828), and the Grant No. FQXi-IAF19-06 from the Foundational Questions Institute Fund (FQXi), a donor advised fund of the Silicon Valley Community Foundation.
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