Nanoscale Topological Morphology Transition and Controllable Thermal Conductivity of Wrinkled Hexagonal Boron Nitride: Implications for Thermal Manipulation and Management
Source abstract
Abstract
Understanding the nanoscale morphology and transition process of two-dimensional (2D) materials would promote the design of emerging 2D devices with controllable properties. Wrinkles induced by mechanical strains have attracted extensive interest as a promising approach to the predictable modulation of structures. Here, a reciprocal-space characterization is implemented to capture the nanoscale topological morphology of free-standing monolayer hexagonal boron nitride (h-BN). Various morphology types and transition processes under different strains are observed. For biaxial compressive strain, the topological morphology of wrinkled h-BN is found to be the same as that of pristine h-BN. For uniaxial compressive strain, different from commonly supposed one-step transition, a three-step morphology transition process within a very narrow strain range is uncovered. The topological morphology under shear strain and angular pinching strain is investigated as well. In addition, the manipulation of thermal conductivity of h-BN by wrinkles is demonstrated to exemplify wrinkle-based thermal manipulation and thermal management in electronic devices.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Graphene research and applications · Thermal properties of materials · 2D Materials and Applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics, National University of Defense Technology, Changsha 410073, P. R. China
Funding
National Natural Science Foundation of China · National Key R&D Program of China · Science Challenge Project · Science and Technology Innovation Program of Hunan Province
References (71)
Show source-provided references
1. 10.1038/s41563-019-0366-810.1038/s41563-019-0366-8 ↗
2. 10.1038/s41377-020-00412-610.1038/s41377-020-00412-6 ↗
3. 10.1038/s41578-021-00304-010.1038/s41578-021-00304-0 ↗
4. 10.1021/acs.nanolett.0c0298310.1021/acs.nanolett.0c02983 ↗
5. 10.1021/acs.nanolett.1c0029410.1021/acs.nanolett.1c00294 ↗
6. 10.1038/nature0856910.1038/nature08569 ↗
7. 10.1038/s41586-019-1226-z10.1038/s41586-019-1226-z ↗
8. 10.1038/s41586-019-1870-310.1038/s41586-019-1870-3 ↗
9. 10.1038/s41586-021-03753-310.1038/s41586-021-03753-3 ↗
10. 10.1038/nnano.2009.19110.1038/nnano.2009.191 ↗
11. 10.1038/ncomms1444010.1038/ncomms14440 ↗
12. 10.1038/nmat354210.1038/nmat3542 ↗
13. 10.1021/acs.nanolett.8b0027310.1021/acs.nanolett.8b00273 ↗
14. 10.1103/PhysRevLett.113.08610210.1103/PhysRevLett.113.086102 ↗
15. 10.1038/ncomms468910.1038/ncomms4689 ↗
16. 10.1038/ncomms478210.1038/ncomms4782 ↗
17. 10.1038/nature2616010.1038/nature26160 ↗
18. 10.1126/sciadv.aav012910.1126/sciadv.aav0129 ↗
19. 10.1103/PhysRevLett.125.08590210.1103/PhysRevLett.125.085902 ↗
20. 10.1103/PhysRevApplied.3.01401010.1103/PhysRevApplied.3.014010 ↗
21. 10.1039/C6NR01992G10.1039/C6NR01992G ↗
22. 10.1103/RevModPhys.90.04100210.1103/RevModPhys.90.041002 ↗
23. 10.1088/0957-4484/23/36/36570110.1088/0957-4484/23/36/365701 ↗
24. 10.1038/ncomms978910.1038/ncomms9789 ↗
25. 10.1103/PhysRevLett.90.07430210.1103/PhysRevLett.90.074302 ↗
26. 10.1016/j.carbon.2019.09.03510.1016/j.carbon.2019.09.035 ↗
27. 10.1021/nn103153x10.1021/nn103153x ↗
28. 10.1103/PhysRevB.86.03542710.1103/PhysRevB.86.035427 ↗
29. 10.1038/nphys238910.1038/nphys2389 ↗
30. 10.1038/nmat201110.1038/nmat2011 ↗
31. 10.1088/0953-8984/25/4/04500910.1088/0953-8984/25/4/045009 ↗
32. 10.1088/0953-8984/27/31/31530210.1088/0953-8984/27/31/315302 ↗
33. 10.1021/acs.jpcc.0c0583110.1021/acs.jpcc.0c05831 ↗
34. 10.1016/j.nanoen.2021.10574910.1016/j.nanoen.2021.105749 ↗
35. 10.1038/s41563-021-00918-310.1038/s41563-021-00918-3 ↗
36. 10.1021/acs.nanolett.5b0149110.1021/acs.nanolett.5b01491 ↗
37. 10.1021/acs.jpcc.8b0200110.1021/acs.jpcc.8b02001 ↗
38. 10.1016/j.mtphys.2019.10013910.1016/j.mtphys.2019.100139 ↗
39. 10.1088/2053-1583/ab20ea10.1088/2053-1583/ab20ea ↗
40. 10.1021/acsnano.0c0271810.1021/acsnano.0c02718 ↗
41. 10.1080/15567265.2017.128642110.1080/15567265.2017.1286421 ↗
42. 10.1039/C4NR04455J10.1039/C4NR04455J ↗
43. 10.1038/nmat320710.1038/nmat3207 ↗
44. 10.1039/C5NR03579A10.1039/C5NR03579A ↗
45. 10.1021/acsanm.0c0264710.1021/acsanm.0c02647 ↗
46. 10.1038/nnano.2010.17210.1038/nnano.2010.172 ↗
47. 10.1073/pnas.200749511710.1073/pnas.2007495117 ↗
48. 10.1103/PhysRevB.37.699110.1103/PhysRevB.37.6991 ↗
49. 10.1103/PhysRevB.84.08540910.1103/PhysRevB.84.085409 ↗
50. 10.1039/D0MH00787K10.1039/D0MH00787K ↗
51. 10.1016/j.cpc.2020.10758310.1016/j.cpc.2020.107583 ↗
52. 10.1016/j.mtphys.2020.10018110.1016/j.mtphys.2020.100181 ↗
53. 10.1103/PhysRevResearch.3.03311610.1103/PhysRevResearch.3.033116 ↗
54. 10.1006/jcph.1995.103910.1006/jcph.1995.1039 ↗
55. 10.1088/0965-0393/18/1/01501210.1088/0965-0393/18/1/015012 ↗
56. 10.1103/PhysRevB.103.20542110.1103/PhysRevB.103.205421 ↗
57. 10.1103/PhysRevB.95.14430910.1103/PhysRevB.95.144309 ↗
58. 10.1103/PhysRevB.92.09430110.1103/PhysRevB.92.094301 ↗
59. 10.1103/PhysRevB.99.06430810.1103/PhysRevB.99.064308 ↗
60. 10.1021/acs.jpcc.9b0910510.1021/acs.jpcc.9b09105 ↗
61. 10.1088/0256-307X/38/1/01440110.1088/0256-307X/38/1/014401 ↗
62. 10.1063/1.510748510.1063/1.5107485 ↗
63. 10.1016/j.ijheatmasstransfer.2019.11871910.1016/j.ijheatmasstransfer.2019.118719 ↗
64. 10.1051/jphys:01987004807010850010.1051/jphys:019870048070108500 ↗
65. 10.1103/PhysRevLett.69.120910.1103/PhysRevLett.69.1209 ↗
66. 10.1103/PhysRevB.84.15542110.1103/PhysRevB.84.155421 ↗
67. 10.1103/PhysRevB.81.24531810.1103/PhysRevB.81.245318 ↗
68. 10.1103/PhysRevB.97.04520210.1103/PhysRevB.97.045202 ↗
69. 10.1021/acs.nanolett.7b0292610.1021/acs.nanolett.7b02926 ↗
70. 10.1063/1.369087110.1063/1.3690871 ↗
71. 10.1103/PhysRevB.97.13430910.1103/PhysRevB.97.134309 ↗