Suppression of Andreev conductance in a topological insulator-superconductor nanostep junction

When two three-dimensional topological insulators (TIs) are brought close to each other with their surfaces aligned, the surfaces form a line junction. Similarly, three TI surfaces, not lying in a single plane, can form an atomic-scale nanostep junction. In this paper, Andreev reflection in a TI-TI-...

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Published inChinese physics B Vol. 25; no. 3; pp. 338 - 341
Main Author 郑翌洁 宋俊涛 李玉现
Format Journal Article
LanguageEnglish
Published 01.03.2016
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ISSN1674-1056
2058-3834
1741-4199
DOI10.1088/1674-1056/25/3/037301

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Abstract When two three-dimensional topological insulators (TIs) are brought close to each other with their surfaces aligned, the surfaces form a line junction. Similarly, three TI surfaces, not lying in a single plane, can form an atomic-scale nanostep junction. In this paper, Andreev reflection in a TI-TI-superconductor nanostep junction is investigated theoretically. Be- cause of the existence of edge states along each line junction, the conductance for a nanostep junction is suppressed. When the incident energy (e) of an electron is larger than the superconductor gap (A), the Andreev conductance in a step junction is less than unity while for a plane junction it is unity. The Andreev conductance is found to depend on the height of the step junction. The Andreev conductance exhibits oscillatory behavior as a function of the junction height with the amplitude of the oscillations remaining unchanged when e = 0, but decreasing for e = A, which is different from the case of the plane junction. The height of the step is therefore an important parameter for Andreev reflection in nanostep junctions, and plays a role similar to that of the delta potential barrier in normal metal-superconductor plane junctions.
AbstractList When two three-dimensional topological insulators (TIs) are brought close to each other with their surfaces aligned, the surfaces form a line junction. Similarly, three TI surfaces, not lying in a single plane, can form an atomic-scale nanostep junction. In this paper, Andreev reflection in a TI-TI-superconductor nanostep junction is investigated theoretically. Because of the existence of edge states along each line junction, the conductance for a nanostep junction is suppressed. When the incident energy ( epsilon ) of an electron is larger than the superconductor gap ( Delta ), the Andreev conductance in a step junction is less than unity while for a plane junction it is unity. The Andreev conductance is found to depend on the height of the step junction. The Andreev conductance exhibits oscillatory behavior as a function of the junction height with the amplitude of the oscillations remaining unchanged when epsilon = 0, but decreasing for epsilon = Delta , which is different from the case of the plane junction. The height of the step is therefore an important parameter for Andreev reflection in nanostep junctions, and plays a role similar to that of the delta potential barrier in normal metal-superconductor plane junctions.
When two three-dimensional topological insulators (TIs) are brought close to each other with their surfaces aligned, the surfaces form a line junction. Similarly, three TI surfaces, not lying in a single plane, can form an atomic-scale nanostep junction. In this paper, Andreev reflection in a TI-TI-superconductor nanostep junction is investigated theoretically. Be- cause of the existence of edge states along each line junction, the conductance for a nanostep junction is suppressed. When the incident energy (e) of an electron is larger than the superconductor gap (A), the Andreev conductance in a step junction is less than unity while for a plane junction it is unity. The Andreev conductance is found to depend on the height of the step junction. The Andreev conductance exhibits oscillatory behavior as a function of the junction height with the amplitude of the oscillations remaining unchanged when e = 0, but decreasing for e = A, which is different from the case of the plane junction. The height of the step is therefore an important parameter for Andreev reflection in nanostep junctions, and plays a role similar to that of the delta potential barrier in normal metal-superconductor plane junctions.
Author 郑翌洁 宋俊涛 李玉现
AuthorAffiliation College Of Physics & Information Engineering and Hebei Advanced Thin Films Laboratory, Hebei Norma/University, Shijiazhuang 050024, China
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Cites_doi 10.1103/PhysRevLett.97.067007
10.1126/science.1148047
10.1103/PhysRevB.90.045413
10.1103/PhysRevLett.74.1657
10.1103/PhysRevLett.108.106603
10.1103/RevModPhys.82.3045
10.1038/nphys1270
10.1103/PhysRevB.25.4515
10.1103/PhysRevLett.95.226801
10.1126/science.1133734
10.1103/PhysRevLett.107.166805
10.1103/PhysRevLett.104.016401
10.1126/science.282.5386.85
10.1103/PhysRevLett.98.106803
10.1103/PhysRevB.85.245402
10.1038/nature06843
10.1103/PhysRevLett.101.047005
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10.1103/RevModPhys.83.1057
10.1038/nphys1274
10.1103/PhysRevLett.95.146802
10.1103/PhysRevB.78.193406
10.1143/JPSJ.77.031007
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Notes topological insulator, nanostep junction, suppression of Andreev conductance
11-5639/O4
When two three-dimensional topological insulators (TIs) are brought close to each other with their surfaces aligned, the surfaces form a line junction. Similarly, three TI surfaces, not lying in a single plane, can form an atomic-scale nanostep junction. In this paper, Andreev reflection in a TI-TI-superconductor nanostep junction is investigated theoretically. Be- cause of the existence of edge states along each line junction, the conductance for a nanostep junction is suppressed. When the incident energy (e) of an electron is larger than the superconductor gap (A), the Andreev conductance in a step junction is less than unity while for a plane junction it is unity. The Andreev conductance is found to depend on the height of the step junction. The Andreev conductance exhibits oscillatory behavior as a function of the junction height with the amplitude of the oscillations remaining unchanged when e = 0, but decreasing for e = A, which is different from the case of the plane junction. The height of the step is therefore an important parameter for Andreev reflection in nanostep junctions, and plays a role similar to that of the delta potential barrier in normal metal-superconductor plane junctions.
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Snippet When two three-dimensional topological insulators (TIs) are brought close to each other with their surfaces aligned, the surfaces form a line junction....
When two three-dimensional topological insulators (TIs) are brought close to each other with their surfaces aligned, the surfaces form a line junction....
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SubjectTerms Conductance
Deltas
Nanostructure
Planes
Reflection
Three dimensional
Topology
Unity
三维拓扑
平面结
振荡行为
电导
绝缘体
超导体
超导能隙
钛表面
Title Suppression of Andreev conductance in a topological insulator-superconductor nanostep junction
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