Direct Observation of Symmetry-Dependent Electron-Phonon Coupling in Black Phosphorus

Nannan Mao, Xingzhi Wang, Yuxuan Lin, Bobby G. Sumpter, Qingqing Ji, Tomás Palacios, Shengxi Huang, Vincent Meunier, Mildred S. Dresselhaus, William A. Tisdale, Liangbo Liang, Xi Ling, Jing Kong

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25 Scopus citations

Abstract

Electron-phonon coupling in two-dimensional nanomaterials plays a fundamental role in determining their physical properties. Such interplay is particularly intriguing in semiconducting black phosphorus (BP) due to the highly anisotropic nature of its electronic structure and phonon dispersions. Here we report the direct observation of symmetry-dependent electron-phonon coupling in BP by performing the polarization-selective resonance Raman measurement in the visible and ultraviolet regimes, focusing on the out-of-plane Ag 1 and in-plane Ag 2 phonon modes. Their intrinsic resonance Raman excitation profiles (REPs) were extracted and quantitatively compared. The in-plane Ag 2 mode exhibits remarkably strong resonance enhancement across the excitation wavelengths when the excitation polarization is parallel to the armchair (Ag 2//AC) direction. In contrast, a dramatically weak resonance effect was observed for the same mode with the polarization parallel to zigzag (Ag 2//ZZ) direction and for the out-of-plane Ag 1 mode (Ag 1//AC and Ag 1//ZZ). Analysis on quantum perturbation theory and first-principles calculations on the anisotropic electron distributions in BP demonstrated that electron-phonon coupling considering the symmetry of the involved excited states and phonon vibration patterns is responsible for this phenomenon. Further analysis of the polarization-dependent REPs for Ag phonons allows us to resolve the existing controversies on the physical origin of Raman anomaly in BP and its dependence on excitation energy, sample thickness, phonon modes, and crystalline orientation. Our study gives deep insights into the underlying interplay between electrons and phonons in BP and paves the way for manipulating the electron-phonon coupling in anisotropic nanomaterials for future device applications.

Original languageEnglish
Pages (from-to)18994-19001
Number of pages8
JournalJournal of the American Chemical Society
Volume141
Issue number48
DOIs
StatePublished - Dec 4 2019

Funding

N.M. and J.K. acknowledge the National Science Foundation grant 2DARE (EFRI-1542815) and DMR-1507806 for financial support. X.W. and X.L. are thankful for the funding support from Boston University. Part of this research (theoretical calculations) used resources at the Center for Nanophase Materials Sciences, which is a DOE Office of Science User Facility. Q.J. acknowledges support by the STC Center for Integrated Quantum Materials, NSF Grant No. DMR-1231319. Y.L. and T.P. acknowledge the partial support of the STC Center for Integrated Quantum Materials, NSF Grant No. DMR 1231319, and the U.S. Army Research Office through the MIT Institute for Soldier Nanotechnologies, under Award No. W911NF-18-2-0048. W.A.T. acknowledges support from the Alfred P. Sloan Foundation and the Camille & Henry Dreyfus Foundation. The authors also thank D. Tuschel, Dr. F. Adar, and Dr. B. A. O’Donnell from Horiba Co. and Dr. L. Lin and M. Wetherington from The Pennsylvania State University for the help of UV Raman experiments. N.M. and J.K. acknowledge the National Science Foundation grant 2DARE (EFRI-1542815) and DMR-1507806 for financial support. X.W. and X.L. are thankful for the funding support from Boston University. Part of this research (theoretical calculations) used resources at the Center for Nanophase Materials Sciences, which is a DOE Office of Science User Facility. Q.J. acknowledges support by the STC Center for Integrated Quantum Materials, NSF Grant No. DMR-1231319. Y.L. and T.P. acknowledge the partial support of the STC Center for Integrated Quantum Materials, NSF Grant No. DMR 1231319, and the U.S. Army Research Office through the MIT Institute for Soldier Nanotechnologies, under Award No. W911NF-18-2-0048. W.A.T. acknowledges support from the Alfred P. Sloan Foundation and the Camille & Henry Dreyfus Foundation. The authors also thank D. Tuschel, Dr. F. Adar, and Dr. B. A. O Donnell from Horiba Co. and Dr. L. Lin and M. Wetherington from The Pennsylvania State University for the help of UV Raman experiments.

FundersFunder number
DOE Office of Science
MIT Institute for Soldier NanotechnologiesW911NF-18-2-0048
STC Center for Integrated Quantum Materials
U.S. Army Research Office
National Science Foundation2DARE, DMR 1231319, DMR-1507806, EFRI-1542815
Alfred P. Sloan Foundation
Camille and Henry Dreyfus Foundation
National Sleep Foundation
Boston University
Pennsylvania State University
U.S. Army Aeromedical Research Laboratory

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