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2 article(s) from Black-Schaffer, Annica M.

Solid-state Stern–Gerlach spin splitter for magnetic field sensing, spintronics, and quantum computing

Kristofer Björnson and
Annica M. Black-Schaffer

Beilstein J. Nanotechnol. 2018, 9, 1558–1563, doi:10.3762/bjnano.9.147

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Figure 1: A hole drilled in a 2D TI creates two edge channels (orange). Leads (grey) are attached on each sid...

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Figure 2: Three solid-state SG spin splitters in series, with the middle device at an angle π/2 relative to t...

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Full Research Paper

Published 25 May 2018

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Andreev spectrum and supercurrents in nanowire-based SNS junctions containing Majorana bound states

Jorge Cayao,
Annica M. Black-Schaffer,
Elsa Prada and
Ramón Aguado

Beilstein J. Nanotechnol. 2018, 9, 1339–1357, doi:10.3762/bjnano.9.127

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Figure 1: A semiconducting nanowire with Rashba SOC is placed on a s-wave superconductor (S’) with pairing po...

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Figure 2: Low-energy spectrum of a superconducting nanowire as function of the Zeeman field B. At zero superc...

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Figure 3: Schematic of SNS junctions based on Rashba nanowires. Top: A nanowire with Rashba SOC of length L = ...

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Figure 4: Low-energy Andreev spectrum as a function of the superconducting phase difference [Graphic 44] in a short SNS j...

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Figure 5: Same as in Figure 4 for a long junction with L_N = 2000 nm and L_S = 2000 nm. Note that, unlike short junctio...

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Figure 6: Same as in Figure 4 for a short junction with L_N = 20 nm and L_S = 10000 nm. Note that in this case, the eme...

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Figure 7: Same as in Figure 4 for a long junction with L_N = 2000 nm and L_S = 10000 nm. The four lowest levels coexist...

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Figure 8: Low-energy Andreev spectrum as a function of the Zeeman field in a short SNS junction at [Graphic 73] = 0 (a,b)...

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Figure 9: Same as in Figure 8 for an intermediate junction with L_N = 400 nm.

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Figure 10: Same as in Figure 8 for a long junction with L_N = 2000 nm.

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Figure 11: Supercurrent as a function of the superconducting phase difference in a short SNS junction, I( [Graphic 84] ), fo...

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Figure 12: Supercurrent as a function of the superconducting phase difference in a long SNS junction with L_N =...

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Figure 13: Supercurrent as a function of [Graphic 119] at B = 1.5B_c. Contributions to the supercurrent for (a,b) short and ...

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Figure 14: Finite temperature effect on the supercurrent, I( [Graphic 163] ), in (a,b) a short and (c,d) a long junction. (a,...

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Figure 15: Effect of normal transmission through the coupling parameter τ on the supercurrent, I( [Graphic 175] ), in (a,b) a...

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Figure 16: Effect of random on-site scalar disorder on the supercurrent I( [Graphic 186] ) in (a,b) a short and (c,d) a long ...

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Full Research Paper

Published 03 May 2018

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