journal article·2017-12-26Open access

Low-Frequency Shear and Layer-Breathing Modes in Raman Scattering of Two-Dimensional Materials

Liangbo Liang, Jun Zhang, Bobby G. Sumpter, Qing-Hai Tan, Ping-Heng Tan, Vincent Meunier

ACS Nano· Volume 11· Issue 12

Abstract

Ever since the isolation of single-layer graphene in 2004, two-dimensional layered structures have been among the most extensively studied classes of materials. To date, the pool of two-dimensional materials (2DMs) continues to grow at an accelerated pace and already covers an extensive range of fascinating and technologically relevant properties. An array of experimental techniques have been developed and used to characterize and understand these properties. In particular, Raman spectroscopy has proven to be a key experimental technique, thanks to its capability to identify minute structural and electronic effects in nondestructive measurements. While high-frequency (HF) intralayer Raman modes have been extensively employed for 2DMs, recent experimental and theoretical progress has demonstrated that low-frequency (LF) interlayer Raman modes are more effective at determining layer numbers and stacking configurations and provide a unique opportunity to study interlayer coupling. These advantages are due to 2DMs' unique interlayer vibration patterns where each layer behaves as an almost rigidly moving object with restoring forces corresponding to weak interlayer interactions. Compared to HF Raman modes, the relatively small attention originally devoted to LF Raman modes is largely due to their weaker signal and their proximity to the strong Rayleigh line background, which previously made their detection challenging. Recent progress in Raman spectroscopy with technical and hardware upgrades now makes it possible to probe LF modes with a standard single-stage Raman system and has proven crucial to characterize and understand properties of 2DMs. Here, we present a comprehensive and forward-looking review on the current status of exploiting LF Raman modes of 2DMs from both experimental and theoretical perspectives, revealing the fundamental physics and technological significance of LF Raman modes in advancing the field of 2DMs. We review a broad array of materials, with varying thickness and stacking configurations, discuss the effect of in-plane anisotropy, and present a generalized linear chain model and interlayer bond polarizability model to rationalize the experimental findings. We also discuss the instrumental improvements of Raman spectroscopy to enhance and separate LF Raman signals from the Rayleigh line. Finally, we highlight the opportunities and challenges ahead in this fast-developing field.
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: Graphene research and applications · 2D Materials and Applications · Ga2O3 and related materials

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United States

State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China

CAS Center of Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences, Beijing 100190, China

Computational Sciences and Engineering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United States

Department of Physics, Applied Physics, and Astronomy, Rensselaer Polytechnic Institute, Troy, New York 12180, United States

Funding

Oak Ridge National Laboratory · Ministry of Science and Technology of the People's Republic of China · Division of Emerging Frontiers in Research and Innovation · Office of Naval Research · National Natural Science Foundation of China · Chinese Academy of Sciences · Central Committee of the Communist Party of China · Beijing Municipal Science and Technology Commission

References (100+)

Show source-provided references
1. 10.1126/science.110289610.1126/science.1102896 ↗
2. 10.1088/0031-8949/2012/T146/01400610.1088/0031-8949/2012/T146/014006 ↗
3. 10.1080/0001873690010130710.1080/00018736900101307 ↗
4. 10.1038/nnano.2010.27910.1038/nnano.2010.279 ↗
5. 10.1021/nn400280c10.1021/nn400280c ↗
6. 10.1038/ncomms425210.1038/ncomms4252 ↗
7. 10.1021/nn400758r10.1021/nn400758r ↗
8. 10.1038/nchem.158910.1038/nchem.1589 ↗
9. 10.1021/acsnano.5b0555610.1021/acsnano.5b05556 ↗
10. 10.1039/C4CS00282B10.1039/C4CS00282B ↗
11. 10.1039/C5NR07205K10.1039/C5NR07205K ↗
12. 10.1007/s12274-016-1224-510.1007/s12274-016-1224-5 ↗
13. 10.1021/jacs.7b0486510.1021/jacs.7b04865 ↗
14. 10.1038/nnano.2014.3510.1038/nnano.2014.35 ↗
15. 10.1021/nn501226z10.1021/nn501226z ↗
16. 10.1038/ncomms545810.1038/ncomms5458 ↗
17. 10.1021/nl503229310.1021/nl5032293 ↗
18. 10.1021/nl502892t10.1021/nl502892t ↗
19. 10.1021/acs.nanolett.5b0111710.1021/acs.nanolett.5b01117 ↗
20. 10.1073/pnas.141658111210.1073/pnas.1416581112 ↗
21. 10.1021/acsnano.5b0114310.1021/acsnano.5b01143 ↗
22. 10.1063/1.341993210.1063/1.3419932 ↗
23. 10.1103/PhysRevLett.108.24550110.1103/PhysRevLett.108.245501 ↗
24. 10.1103/PhysRevLett.108.15550110.1103/PhysRevLett.108.155501 ↗
25. 10.1038/nnano.2014.32510.1038/nnano.2014.325 ↗
26. 10.1021/nn400940610.1021/nn4009406 ↗
27. 10.1088/1367-2630/16/9/09500210.1088/1367-2630/16/9/095002 ↗
28. 10.1038/ncomms438910.1038/ncomms4389 ↗
29. 10.1038/nmat438410.1038/nmat4384 ↗
30. 10.1126/science.aad108010.1126/science.aad1080 ↗
31. 10.1038/nnano.2013.4610.1038/nnano.2013.46 ↗
32. 10.1038/nnano.2014.15010.1038/nnano.2014.150 ↗
33. 10.1038/nnano.2014.16710.1038/nnano.2014.167 ↗
34. 10.1021/nn505736z10.1021/nn505736z ↗
35. 10.1021/nn502738810.1021/nn5027388 ↗
36. 10.1021/nl903868w10.1021/nl903868w ↗
37. 10.1103/PhysRevLett.105.13680510.1103/PhysRevLett.105.136805 ↗
38. 10.1103/PhysRevB.89.23531910.1103/PhysRevB.89.235319 ↗
39. 10.1038/nature1238510.1038/nature12385 ↗
40. 10.1038/nature1218610.1038/nature12186 ↗
41. 10.1038/nphys146310.1038/nphys1463 ↗
42. 10.1038/nnano.2014.17610.1038/nnano.2014.176 ↗
43. 10.1038/ncomms630910.1038/ncomms6309 ↗
44. 10.1038/nphys210410.1038/nphys2104 ↗
45. 10.1038/nphys210210.1038/nphys2102 ↗
46. 10.1038/nphys210310.1038/nphys2103 ↗
47. 10.1038/nphys343010.1038/nphys3430 ↗
48. 10.1038/nnano.2014.14810.1038/nnano.2014.148 ↗
49. 10.1021/nl501077m10.1021/nl501077m ↗
50. 10.1021/nl501459710.1021/nl5014597 ↗
51. 10.1038/ncomms596610.1038/ncomms5966 ↗
52. 10.1021/acsnano.5b0188410.1021/acsnano.5b01884 ↗
53. 10.1002/adfm.20160446810.1002/adfm.201604468 ↗
54. 10.1021/nn100393710.1021/nn1003937 ↗
55. 10.1007/s12274-014-0446-710.1007/s12274-014-0446-7 ↗
56. 10.1016/j.physe.2016.01.04010.1016/j.physe.2016.01.040 ↗
57. 10.1038/nmat324510.1038/nmat3245 ↗
58. 10.1021/nl302450s10.1021/nl302450s ↗
59. 10.1103/PhysRevB.87.12140410.1103/PhysRevB.87.121404 ↗
60. 10.1021/nl501678j10.1021/nl501678j ↗
61. 10.1103/PhysRevB.87.11541310.1103/PhysRevB.87.115413 ↗
62. 10.1103/PhysRevB.86.24130110.1103/PhysRevB.86.241301 ↗
63. 10.1103/PhysRevB.87.19531610.1103/PhysRevB.87.195316 ↗
64. 10.1021/nl304169w10.1021/nl304169w ↗
65. 10.1021/acs.nanolett.5b0077510.1021/acs.nanolett.5b00775 ↗
66. 10.1103/PhysRevLett.116.08740110.1103/PhysRevLett.116.087401 ↗
67. 10.1007/s12274-015-0865-010.1007/s12274-015-0865-0 ↗
68. 10.1002/pssr.20151041210.1002/pssr.201510412 ↗
69. 10.1103/PhysRevB.90.24542810.1103/PhysRevB.90.245428 ↗
70. 10.1038/nnano.2015.14310.1038/nnano.2015.143 ↗
71. 10.1088/2053-1583/3/3/03100810.1088/2053-1583/3/3/031008 ↗
72. 10.1088/2053-1583/aa77d410.1088/2053-1583/aa77d4 ↗
73. 10.1063/1.490657910.1063/1.4906579 ↗
74. 10.1016/j.carbon.2015.11.06210.1016/j.carbon.2015.11.062 ↗
75. 10.1002/adma.20150108610.1002/adma.201501086 ↗
76. 10.1021/acs.nanolett.5b0359710.1021/acs.nanolett.5b03597 ↗
77. 10.1038/srep1947610.1038/srep19476 ↗
78. 10.1021/acsnano.5b0583110.1021/acsnano.5b05831 ↗
79. 10.1039/C6NR01569G10.1039/C6NR01569G ↗
80. 10.1021/acs.nanolett.5b0492510.1021/acs.nanolett.5b04925 ↗
81. 10.1039/C7NR05839J10.1039/C7NR05839J ↗
82. 10.1038/ncomms570910.1038/ncomms5709 ↗
83. 10.1021/acsnano.5b0250210.1021/acsnano.5b02502 ↗
84. 10.1021/acsnano.5b0780710.1021/acsnano.5b07807 ↗
85. 10.1021/acs.nanolett.5b0501510.1021/acs.nanolett.5b05015 ↗
86. 10.1103/PhysRevB.91.16540310.1103/PhysRevB.91.165403 ↗
87. 10.1002/adma.20150463110.1002/adma.201504631 ↗
88. 10.1103/PhysRevLett.25.36210.1103/PhysRevLett.25.362 ↗
89. 10.1103/PhysRevB.88.19531310.1103/PhysRevB.88.195313 ↗
90. 10.1103/PhysRev.142.57010.1103/PhysRev.142.570 ↗
91. 10.1021/nl200773n10.1021/nl200773n ↗
92. 10.1039/c3nr06906k10.1039/c3nr06906k ↗
93. 10.1016/0038-1098(73)90111-710.1016/0038-1098(73)90111-7 ↗
94. 10.1038/srep1456510.1038/srep14565 ↗
95. 10.1088/0957-4484/27/14/14570410.1088/0957-4484/27/14/145704 ↗
96. 10.1103/PhysRevB.93.11540910.1103/PhysRevB.93.115409 ↗
97. 10.1021/acs.nanolett.5b0268310.1021/acs.nanolett.5b02683 ↗
98. 10.1021/acsnano.5b0784410.1021/acsnano.5b07844 ↗
99. 10.1063/1.492191110.1063/1.4921911 ↗
100. 10.1117/12.92357510.1117/12.923575 ↗