TY - JOUR
T1 - MoS2 edges and heterophase interfaces
T2 - energy, structure and phase engineering
AU - Zhou, Songsong
AU - Han, Jian
AU - Sun, Jianwei
AU - Srolovitz, David J
PY - 2017/6
Y1 - 2017/6
N2 - The transition metal dichalcogenides exhibit polymorphism; i.e. both 2H and 1T′ crystal structures, each with unique electronic properties. These two phases can coexist within the same monolayer microstructure, producing 2H/1T′ interfaces. Here we report a systematic investigation of the energetics of the experimentally most important MoS2 heterophase interfaces and edges. The stable interface and edge structures change with chemical potential (these edges/interfaces are usually non-stoichiometric). Stable edges tend to be those of highest atomic density and the stable interfaces correspond to those with local atomic structure very similar to the 2H crystal. The interfacial energies are lower than those of the edges, and the 1T′ edges have lower energy than the 2H edges. Because the 1T′ edges have much lower energy than the 2H edges, a sufficiently narrow 1T′ ribbon will be more stable than the corresponding 2H ribbon (this critical width is much larger in MoTe2 than in MoS2). Similarly, a large 2H flake have an equilibrium strip of 1T′ along its edge (again this effect is much larger in MoTe2 than in MoS2). Application of tensile strains can increase the width of the stable 1T′ strip or the critical thickness below which a ribbon favors the 1T′ structure. These effects provide a means to phase engineer transition metal dichalcogenide microstructures.
AB - The transition metal dichalcogenides exhibit polymorphism; i.e. both 2H and 1T′ crystal structures, each with unique electronic properties. These two phases can coexist within the same monolayer microstructure, producing 2H/1T′ interfaces. Here we report a systematic investigation of the energetics of the experimentally most important MoS2 heterophase interfaces and edges. The stable interface and edge structures change with chemical potential (these edges/interfaces are usually non-stoichiometric). Stable edges tend to be those of highest atomic density and the stable interfaces correspond to those with local atomic structure very similar to the 2H crystal. The interfacial energies are lower than those of the edges, and the 1T′ edges have lower energy than the 2H edges. Because the 1T′ edges have much lower energy than the 2H edges, a sufficiently narrow 1T′ ribbon will be more stable than the corresponding 2H ribbon (this critical width is much larger in MoTe2 than in MoS2). Similarly, a large 2H flake have an equilibrium strip of 1T′ along its edge (again this effect is much larger in MoTe2 than in MoS2). Application of tensile strains can increase the width of the stable 1T′ strip or the critical thickness below which a ribbon favors the 1T′ structure. These effects provide a means to phase engineer transition metal dichalcogenide microstructures.
KW - density functional theory calculations
KW - edges
KW - interfaces
KW - monolayer molybdenum disulfide
KW - phase transitions
UR - http://www.scopus.com/inward/record.url?scp=85021362363&partnerID=8YFLogxK
UR - https://www.scopus.com/record/pubmetrics.uri?eid=2-s2.0-85021362363&origin=recordpage
U2 - 10.1088/2053-1583/aa6d22
DO - 10.1088/2053-1583/aa6d22
M3 - RGC 21 - Publication in refereed journal
SN - 2053-1583
VL - 4
JO - 2D Materials
JF - 2D Materials
IS - 2
M1 - 025080
ER -