Resonant Raman and Exciton Coupling in High-Quality Single Crystals of Atomically Thin Molybdenum Diselenide Grown by Vapor-Phase Chalcogenization

被引:38
作者
Bilgin, Ismail [1 ]
Raeliarijaona, Aldo S. [2 ]
Lucking, Michael C. [2 ]
Hodge, Sebastian Cooper [1 ]
Mohite, Aditya D. [3 ]
de Luna Bugallo, Andres [1 ,4 ]
Terrones, Humberto [2 ]
Kar, Swastik [1 ]
机构
[1] Northeastern Univ, Dept Phys, Boston, MA 02115 USA
[2] Rensselaer Polytech Inst, Dept Phys Appl Phys & Astron, Troy, NY 12180 USA
[3] Los Alamos Natl Lab, Los Alamos, NM 87545 USA
[4] ICONACYT Cinvestav Unidad Queretaro, Queretaro 76230, Qro, Mexico
基金
美国国家科学基金会;
关键词
vapor-phase chalcogenization; Resonant Raman; MoSe2; Excitons; TMDs; single crystal; density functional theory; MONOLAYER MOS2; SPECTROSCOPY; DEPOSITION; DISULFIDE; BANDGAP; HETEROSTRUCTURES; SCATTERING; TRANSPORT; LAYERS; STATE;
D O I
10.1021/acsnano.7b07933
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
We report a detailed investigation on Raman spectroscopy in vapor-phase chalcogenization grown, high quality single-crystal atomically thin molybdenum diselenide samples. Measurements were performed in samples with four different incident laser excitation energies ranging from 1.95 eV <= E-ex <= 2.71 eV, revealing rich spectral information in samples ranging from N = 1-4 layers and a thick, bulk sample. In addition to previously observed (and identified) peaks, we specifically investigate the origin of a peak near omega approximate to 250 cm(-1). Our density functional theory and Bethe-Salpeter calculations suggest that this peak arises from a double-resonant Raman process involving the ZA. acoustic phonon perpendicular to the layer. This mode appears prominently in freshly prepared samples and disappears in aged samples, thereby offering a method for ascertaining the high optoelectronic quality of freshly prepared 2D-MoSe2 crystals. We further present an in-depth investigation of the energy-dependent variation of the position of this and other peaks and provide evidence of C-exciton-phonon coupling in monolayer MoSe2. Finally, we show how the signature peak positions and intensities vary as a function of layer thickness in these samples.
引用
收藏
页码:740 / 750
页数:11
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