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| 001 | 852623 | ||
| 005 | 20210129235147.0 | ||
| 024 | 7 | _ | |a 10.1117/12.2322720 |2 doi |
| 024 | 7 | _ | |a WOS:000452820000009 |2 WOS |
| 037 | _ | _ | |a FZJ-2018-05521 |
| 100 | 1 | _ | |a Schäpers, Thomas |0 P:(DE-Juel1)128634 |b 0 |e Corresponding author |
| 111 | 2 | _ | |a Spintronics XI |c San Diego |d 2018-08-19 - 2018-08-23 |w United States |
| 245 | _ | _ | |a Phase-coherent transport in topological insulator nanocolumns and nanoribbons |
| 260 | _ | _ | |c 2018 |b SPIE |
| 295 | 1 | 0 | |a Spintronics XI : [Proceedings] - SPIE, 2018. - ISBN 97815106203539781510620360 - doi:10.1117/12.2322720 |
| 300 | _ | _ | |a 107320V-1 |
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| 520 | _ | _ | |a The transport properties of topological insulator nanostructures prepared by selective-area molecular beam epitaxy is investigated. For the nanocolumn structures based on Sb2Te3/Bi2Te3-heterostructures pronounced universal conductance fluctuations are observed in the magnetoconductance, indicating phase-coherent transport. Furthermore, angle-dependent measurements indicate that the phase coherent loops are mainly oriented parallel to the substrate plane. Measurements on nanoribbons based on (Bi0.57Sb0.43)2Te3 revealed a resistance dip due to weak antilocalization as well as universal conductance fluctuations. Here, we also found indications, that the phase-coherent loops are predominantly oriented parallel to the quintuple layers forming the topological insulator. |
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| 700 | 1 | _ | |a Weyrich, Christian |0 P:(DE-HGF)0 |b 1 |
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| 700 | 1 | _ | |a Jaffrès, Henri |0 P:(DE-HGF)0 |b 11 |e Editor |
| 700 | 1 | _ | |a Drouhin, Henri-Jean |0 P:(DE-HGF)0 |b 12 |e Editor |
| 700 | 1 | _ | |a Wegrowe, Jean-Eric |0 P:(DE-HGF)0 |b 13 |e Editor |
| 700 | 1 | _ | |a Razeghi, Manijeh |0 P:(DE-HGF)0 |b 14 |e Editor |
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