Topological states in two-dimensional hexagon lattice bilayers
We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t &g...
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| Autor*in: |
Zhang, Ming-Ming [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2016transfer abstract |
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| Schlagwörter: |
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| Umfang: |
5 |
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| Übergeordnetes Werk: |
Enthalten in: Transient response and failure of medium density fibreboard panels subjected to air-blast loading - Langdon, G.S. ELSEVIER, 2021, Amsterdam |
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| Übergeordnetes Werk: |
volume:380 ; year:2016 ; number:41 ; day:7 ; month:10 ; pages:3389-3393 ; extent:5 |
| Links: |
|---|
| DOI / URN: |
10.1016/j.physleta.2016.05.039 |
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ELV035336145 |
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| 520 | |a We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. | ||
| 520 | |a We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. | ||
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| 650 | 7 | |a Quantum valley Hall state |2 Elsevier | |
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| 700 | 1 | |a Xu, Lei |4 oth | |
| 700 | 1 | |a Zhang, Jun |4 oth | |
| 773 | 0 | 8 | |i Enthalten in |n North-Holland Publ |a Langdon, G.S. ELSEVIER |t Transient response and failure of medium density fibreboard panels subjected to air-blast loading |d 2021 |g Amsterdam |w (DE-627)ELV006407811 |
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10.1016/j.physleta.2016.05.039 doi GBVA2016012000006.pica (DE-627)ELV035336145 (ELSEVIER)S0375-9601(16)30245-6 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Zhang, Ming-Ming verfasserin aut Topological states in two-dimensional hexagon lattice bilayers 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. Hexagon lattice bilayer Elsevier Quantum valley Hall state Elsevier Topological phase transition Elsevier Xu, Lei oth Zhang, Jun oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:41 day:7 month:10 pages:3389-3393 extent:5 https://doi.org/10.1016/j.physleta.2016.05.039 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 41 7 1007 3389-3393 5 045F 530 |
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10.1016/j.physleta.2016.05.039 doi GBVA2016012000006.pica (DE-627)ELV035336145 (ELSEVIER)S0375-9601(16)30245-6 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Zhang, Ming-Ming verfasserin aut Topological states in two-dimensional hexagon lattice bilayers 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. Hexagon lattice bilayer Elsevier Quantum valley Hall state Elsevier Topological phase transition Elsevier Xu, Lei oth Zhang, Jun oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:41 day:7 month:10 pages:3389-3393 extent:5 https://doi.org/10.1016/j.physleta.2016.05.039 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 41 7 1007 3389-3393 5 045F 530 |
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10.1016/j.physleta.2016.05.039 doi GBVA2016012000006.pica (DE-627)ELV035336145 (ELSEVIER)S0375-9601(16)30245-6 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Zhang, Ming-Ming verfasserin aut Topological states in two-dimensional hexagon lattice bilayers 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. Hexagon lattice bilayer Elsevier Quantum valley Hall state Elsevier Topological phase transition Elsevier Xu, Lei oth Zhang, Jun oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:41 day:7 month:10 pages:3389-3393 extent:5 https://doi.org/10.1016/j.physleta.2016.05.039 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 41 7 1007 3389-3393 5 045F 530 |
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10.1016/j.physleta.2016.05.039 doi GBVA2016012000006.pica (DE-627)ELV035336145 (ELSEVIER)S0375-9601(16)30245-6 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Zhang, Ming-Ming verfasserin aut Topological states in two-dimensional hexagon lattice bilayers 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. Hexagon lattice bilayer Elsevier Quantum valley Hall state Elsevier Topological phase transition Elsevier Xu, Lei oth Zhang, Jun oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:41 day:7 month:10 pages:3389-3393 extent:5 https://doi.org/10.1016/j.physleta.2016.05.039 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 41 7 1007 3389-3393 5 045F 530 |
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10.1016/j.physleta.2016.05.039 doi GBVA2016012000006.pica (DE-627)ELV035336145 (ELSEVIER)S0375-9601(16)30245-6 DE-627 ger DE-627 rakwb eng 530 530 DE-600 670 VZ 51.75 bkl Zhang, Ming-Ming verfasserin aut Topological states in two-dimensional hexagon lattice bilayers 2016transfer abstract 5 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. Hexagon lattice bilayer Elsevier Quantum valley Hall state Elsevier Topological phase transition Elsevier Xu, Lei oth Zhang, Jun oth Enthalten in North-Holland Publ Langdon, G.S. ELSEVIER Transient response and failure of medium density fibreboard panels subjected to air-blast loading 2021 Amsterdam (DE-627)ELV006407811 volume:380 year:2016 number:41 day:7 month:10 pages:3389-3393 extent:5 https://doi.org/10.1016/j.physleta.2016.05.039 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U 51.75 Verbundwerkstoffe Schichtstoffe VZ AR 380 2016 41 7 1007 3389-3393 5 045F 530 |
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Topological states in two-dimensional hexagon lattice bilayers |
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Zhang, Ming-Ming |
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Transient response and failure of medium density fibreboard panels subjected to air-blast loading |
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Transient response and failure of medium density fibreboard panels subjected to air-blast loading |
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eng |
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Zhang, Ming-Ming |
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Elektronische Aufsätze |
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Zhang, Ming-Ming |
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10.1016/j.physleta.2016.05.039 |
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530 670 |
| title_sort |
topological states in two-dimensional hexagon lattice bilayers |
| title_auth |
Topological states in two-dimensional hexagon lattice bilayers |
| abstract |
We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. |
| abstractGer |
We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. |
| abstract_unstemmed |
We investigate the topological states of the two-dimensional hexagon lattice bilayer. The system exhibits a quantum valley Hall (QVH) state when the interlayer interaction t ⊥ is smaller than the nearest neighbor hopping energy t, and then translates to a trivial band insulator state when t ⊥ / t > 1 . Interestingly, the system is found to be a single-edge QVH state with t ⊥ / t = 1 . The topological phase transition also can be presented via changing bias voltage and sublattice potential in the system. The QVH states have different edge modes carrying valley current but no net charge current. The bias voltage and external electric field can be tuned easily in experiments, so the present results will provide potential application in valleytronics based on the two-dimensional hexagon lattice. |
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41 |
| title_short |
Topological states in two-dimensional hexagon lattice bilayers |
| url |
https://doi.org/10.1016/j.physleta.2016.05.039 |
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Xu, Lei Zhang, Jun |
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Xu, Lei Zhang, Jun |
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2024-07-06T17:17:55.331Z |
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