Double resonance Raman modes in monolayer and few-layer MoTe[subscript 2]

We study the second-order Raman process of mono- and few-layer MoTe[subscript 2], by combining ab initio density functional perturbation calculations with experimental Raman spectroscopy using 532, 633, and 785 nm excitation lasers. The calculated electronic band structure and the density of states...

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Bibliographic Details
Main Authors: Guo, Huaihong, Yang, Teng, Yamamoto, Mahito, Zhou, Lin, Ishikawa, Ryo, Ueno, Keiji, Tsukagoshi, Kazuhito, Zhang, Zhidong, Saito, Riichiro, Dresselhaus, Mildred
Other Authors: Massachusetts Institute of Technology. Department of Electrical Engineering and Computer Science
Format: Article
Language:English
Published: American Physical Society 2015
Online Access:http://hdl.handle.net/1721.1/96972
https://orcid.org/0000-0001-8492-2261
https://orcid.org/0000-0001-8749-7408
Description
Summary:We study the second-order Raman process of mono- and few-layer MoTe[subscript 2], by combining ab initio density functional perturbation calculations with experimental Raman spectroscopy using 532, 633, and 785 nm excitation lasers. The calculated electronic band structure and the density of states show that the resonance Raman process occurs at the M point in the Brillouin zone, where a strong optical absorption occurs due to a logarithmic Van Hove singularity of the electronic density of states. The double resonance Raman process with intervalley electron-phonon coupling connects two of the three inequivalent M points in the Brillouin zone, giving rise to second-order Raman peaks due to the M-point phonons. The calculated vibrational frequencies of the second-order Raman spectra agree with the observed laser-energy-dependent Raman shifts in the experiment.