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We review lattice vibrational modes in atomically thin two-dimensional (2D) layered materials, focusing on 2D materials beyond graphene, such as group Ⅵ transition metal dichalcogenides, topological insulator bismuth chalcogenides, and black phosphorus. Although the composition and structure of those materials are remarkably different, they share a common and important feature, i.e., their bulk crystals are stacked via van der Waals interactions between "layers" while each layer is comprised of one or more atomic planes. First, we review the background of some 2D materials (MX2, M = Mo, W; X = S, Se, Te. Bi2X3, X = Se, Te. Black phosphorus), including crystalline structures and stacking order. We then review the studies on vibrational modes of layered materials and nanostructures probed by the powerful yet nondestructive Raman spectroscopy technique. Based on studies conducted before 2010, recent investigations using more advanced techniques have pushed the studies of phonon modes in 2D layered materials to the atomically thin regime, down to monolayers. We will classify the recently reported general features into the following categories: phonon confinement effects and electron-phonon coupling, anomalous shifts in high-frequency intralayer vibrational modes and surface effects, reduced dimensionality and lower symmetry, the linear chain model and the substrate effect, stacking orders and interlayer shear modes, polarization dependence, and the resonance effect. Within the seven categories, both intralayer and interlayer vibrational modes will be discussed. The comparison between different materials will be provided as well.

Publication history
Copyright
Acknowledgements

Publication history

Received: 16 May 2016
Revised: 10 July 2016
Accepted: 18 July 2016
Published: 20 September 2016
Issue date: December 2016

Copyright

© Tsinghua University Press and Springer-Verlag Berlin Heidelberg 2016

Acknowledgements

Acknowledgements

Q. H. X. gratefully thanks Singapore National Research Foundation via a Fellowship grant (No. NRF-RF2009-06) and an Investigatorship grant (No. NRF-NRFI2015-03), Ministry of Education via a tier2 grant (No. MOE2012-T2-2-086) and a tier1 grant (No. 2013-T1-002-232). S. Y. Q. and X. Luo gratefully acknowledge the Singapore National Research Foundation (NRF) for funding under the NRF Fellowship (No. NRF-NRFF2013-07). Z. J. gratefully thanks National Natural Science Foundation of China (Nos. 11574305 and 51527901) and financial support from the National 1000 Talent Plan of China via a Young Project. The computations were performed on the cluster of NUS Graphene Research Centre. S. Y. Q. and X. Luo acknowledge the National Research Foundation, Prime Minister's Office, Singapore, under its Medium Sized Centre Programme.

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