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Cation–Eutectic Transition via Sublattice Melting in CuInP2S6/In4/3P2S6 van der Waals Layered Crystals
Author(s) -
Michael A. Susner,
Marius Chyasnavichyus,
Alexander A. Puretzky,
Qian He,
Benjamin S. Conner,
Yang Ren,
David A. Cullen,
Panchapakesan Ganesh,
Dongwon Shin,
Hakan Demir,
Jake Mcmurray,
Albina Y. Borisevich,
Petro Maksymovych,
Michael A. McGuire
Publication year - 2017
Publication title -
acs nano
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 5.554
H-Index - 382
eISSN - 1936-086X
pISSN - 1936-0851
DOI - 10.1021/acsnano.7b02695
Subject(s) - materials science , eutectic system , phase transition , van der waals force , condensed matter physics , heterojunction , dielectric , phase (matter) , chemical physics , crystal structure , ferroelectricity , lattice (music) , nanotechnology , crystallography , optoelectronics , chemistry , microstructure , physics , organic chemistry , molecule , acoustics , metallurgy
Single crystals of the van der Waals layered ferrielectric material CuInP 2 S 6 spontaneously phase separate when synthesized with Cu deficiency. Here we identify a route to form and tune intralayer heterostructures between the corresponding ferrielectric (CuInP 2 S 6 ) and paraelectric (In 4/3 P 2 S 6 ) phases through control of chemical phase separation. We conclusively demonstrate that Cu-deficient Cu 1-x In 1+x/3 P 2 S 6 forms a single phase at high temperature. We also identify the mechanism by which the phase separation proceeds upon cooling. Above 500 K both Cu + and In 3+ become mobile, while P 2 S 6 4- anions maintain their structure. We therefore propose that this transition can be understood as eutectic melting on the cation sublattice. Such a model suggests that the transition temperature for the melting process is relatively low because it requires only a partial reorganization of the crystal lattice. As a result, varying the cooling rate through the phase transition controls the lateral extent of chemical domains over several decades in size. At the fastest cooling rate, the dimensional confinement of the ferrielectric CuInP 2 S 6 phase to nanoscale dimensions suppresses ferrielectric ordering due to the intrinsic ferroelectric size effect. Intralayer heterostructures can be formed, destroyed, and re-formed by thermal cycling, thus enabling the possibility of finely tuned ferroic structures that can potentially be optimized for specific device architectures.

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