From Bulk to Monolayer MoS 2 : Evolution of Raman Scattering
Abstract Molybdenum disulfide (MoS 2 ) is systematically studied using Raman spectroscopy with ultraviolet and visible laser lines. It is shown that only the Raman frequencies of $ E_{2{\rm g}}^1 $ and $ A_{{\rm 1g}}^{} $ peaks vary monotonously with the layer number of ultrathin MoS 2 flakes, while...
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Published in | Advanced functional materials Vol. 22; no. 7; pp. 1385 - 1390 |
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Main Authors | , , , , , , |
Format | Journal Article |
Language | English |
Published |
10.04.2012
|
Online Access | Get full text |
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Summary: | Abstract
Molybdenum disulfide (MoS
2
) is systematically studied using Raman spectroscopy with ultraviolet and visible laser lines. It is shown that only the Raman frequencies of
$ E_{2{\rm g}}^1 $
and
$ A_{{\rm 1g}}^{} $
peaks vary monotonously with the layer number of ultrathin MoS
2
flakes, while intensities or widths of the peaks vary arbitrarily. The coupling between electronic transitions and phonons are found to become weaker when the layer number of MoS
2
decreases, attributed to the increased electronic transition energies or elongated intralayer atomic bonds in ultrathin MoS
2
. The asymmetric Raman peak at 454 cm
−1
, which has been regarded as the overtone of longitudinal optical M phonons in bulk MoS
2
, is actually a combinational band involving a longitudinal acoustic mode (LA(M)) and an optical mode (
$ A_{{\rm 2u}}^{} $
). Our findings suggest a clear evolution of the coupling between electronic transition and phonon when MoS
2
is scaled down from three‐ to two‐dimensional geometry. |
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ISSN: | 1616-301X 1616-3028 |
DOI: | 10.1002/adfm.201102111 |