Cargando…
K-Λ crossover transition in the conduction band of monolayer MoS(2) under hydrostatic pressure
Monolayer MoS(2) is a promising material for optoelectronics applications owing to its direct bandgap, enhanced Coulomb interaction, strong spin-orbit coupling, unique valley pseudospin degree of freedom, etc. It can also be implemented for novel spintronics and valleytronics devices at atomic scale...
Autores principales: | , , , , , , , , , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Association for the Advancement of Science
2017
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5669610/ https://www.ncbi.nlm.nih.gov/pubmed/29119136 http://dx.doi.org/10.1126/sciadv.1700162 |
_version_ | 1783275872059392000 |
---|---|
author | Fu, Lei Wan, Yi Tang, Ning Ding, Yi-min Gao, Jing Yu, Jiachen Guan, Hongming Zhang, Kun Wang, Weiying Zhang, Caifeng Shi, Jun-jie Wu, Xiang Shi, Su-Fei Ge, Weikun Dai, Lun Shen, Bo |
author_facet | Fu, Lei Wan, Yi Tang, Ning Ding, Yi-min Gao, Jing Yu, Jiachen Guan, Hongming Zhang, Kun Wang, Weiying Zhang, Caifeng Shi, Jun-jie Wu, Xiang Shi, Su-Fei Ge, Weikun Dai, Lun Shen, Bo |
author_sort | Fu, Lei |
collection | PubMed |
description | Monolayer MoS(2) is a promising material for optoelectronics applications owing to its direct bandgap, enhanced Coulomb interaction, strong spin-orbit coupling, unique valley pseudospin degree of freedom, etc. It can also be implemented for novel spintronics and valleytronics devices at atomic scale. The band structure of monolayer MoS(2) is well known to have a direct gap at K (K′) point, whereas the second lowest conduction band minimum is located at Λ point, which may interact with the valence band maximum at K point, to make an indirect optical bandgap transition. We experimentally demonstrate the direct-to-indirect bandgap transition by measuring the photoluminescence spectra of monolayer MoS(2) under hydrostatic pressure at room temperature. With increasing pressure, the direct transition shifts at a rate of 49.4 meV/GPa, whereas the indirect transition shifts at a rate of −15.3 meV/GPa. We experimentally extract the critical transition point at the pressure of 1.9 GPa, in agreement with first-principles calculations. Combining our experimental observation with first-principles calculations, we confirm that this transition is caused by the K-Λ crossover in the conduction band. |
format | Online Article Text |
id | pubmed-5669610 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | American Association for the Advancement of Science |
record_format | MEDLINE/PubMed |
spelling | pubmed-56696102017-11-08 K-Λ crossover transition in the conduction band of monolayer MoS(2) under hydrostatic pressure Fu, Lei Wan, Yi Tang, Ning Ding, Yi-min Gao, Jing Yu, Jiachen Guan, Hongming Zhang, Kun Wang, Weiying Zhang, Caifeng Shi, Jun-jie Wu, Xiang Shi, Su-Fei Ge, Weikun Dai, Lun Shen, Bo Sci Adv Research Articles Monolayer MoS(2) is a promising material for optoelectronics applications owing to its direct bandgap, enhanced Coulomb interaction, strong spin-orbit coupling, unique valley pseudospin degree of freedom, etc. It can also be implemented for novel spintronics and valleytronics devices at atomic scale. The band structure of monolayer MoS(2) is well known to have a direct gap at K (K′) point, whereas the second lowest conduction band minimum is located at Λ point, which may interact with the valence band maximum at K point, to make an indirect optical bandgap transition. We experimentally demonstrate the direct-to-indirect bandgap transition by measuring the photoluminescence spectra of monolayer MoS(2) under hydrostatic pressure at room temperature. With increasing pressure, the direct transition shifts at a rate of 49.4 meV/GPa, whereas the indirect transition shifts at a rate of −15.3 meV/GPa. We experimentally extract the critical transition point at the pressure of 1.9 GPa, in agreement with first-principles calculations. Combining our experimental observation with first-principles calculations, we confirm that this transition is caused by the K-Λ crossover in the conduction band. American Association for the Advancement of Science 2017-11-03 /pmc/articles/PMC5669610/ /pubmed/29119136 http://dx.doi.org/10.1126/sciadv.1700162 Text en Copyright © 2017 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC). http://creativecommons.org/licenses/by-nc/4.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution-NonCommercial license (http://creativecommons.org/licenses/by-nc/4.0/) , which permits use, distribution, and reproduction in any medium, so long as the resultant use is not for commercial advantage and provided the original work is properly cited. |
spellingShingle | Research Articles Fu, Lei Wan, Yi Tang, Ning Ding, Yi-min Gao, Jing Yu, Jiachen Guan, Hongming Zhang, Kun Wang, Weiying Zhang, Caifeng Shi, Jun-jie Wu, Xiang Shi, Su-Fei Ge, Weikun Dai, Lun Shen, Bo K-Λ crossover transition in the conduction band of monolayer MoS(2) under hydrostatic pressure |
title | K-Λ crossover transition in the conduction band of monolayer MoS(2) under hydrostatic pressure |
title_full | K-Λ crossover transition in the conduction band of monolayer MoS(2) under hydrostatic pressure |
title_fullStr | K-Λ crossover transition in the conduction band of monolayer MoS(2) under hydrostatic pressure |
title_full_unstemmed | K-Λ crossover transition in the conduction band of monolayer MoS(2) under hydrostatic pressure |
title_short | K-Λ crossover transition in the conduction band of monolayer MoS(2) under hydrostatic pressure |
title_sort | k-λ crossover transition in the conduction band of monolayer mos(2) under hydrostatic pressure |
topic | Research Articles |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5669610/ https://www.ncbi.nlm.nih.gov/pubmed/29119136 http://dx.doi.org/10.1126/sciadv.1700162 |
work_keys_str_mv | AT fulei klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT wanyi klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT tangning klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT dingyimin klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT gaojing klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT yujiachen klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT guanhongming klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT zhangkun klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT wangweiying klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT zhangcaifeng klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT shijunjie klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT wuxiang klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT shisufei klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT geweikun klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT dailun klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure AT shenbo klcrossovertransitionintheconductionbandofmonolayermos2underhydrostaticpressure |