/ Home
/ SUBMISSION

/ The BJNANO
/ Diamond Open Access
/ Journal Statistics
/ Editorial Board
/ Community
/ Call for papers

/ Latest Articles
/ Most accessed
/ Thematic issues
/ Volumes
/ Authors

/ Alerts

/ TWITTER
/ LINKEDIN
/ Mastodon
/ RSS FEED

Empty search

Article Type

Publication Date Range

Search Tips

This search combines search strings from the content search (i.e. "Full Text", "Author", "Title", "Abstract", or "Keywords") with "Article Type" and "Publication Date Range" using the AND operator.

Search Examples

aromatic	the word “aromatic”
aromatic aldehyde	the word “aromatic” OR “aldehyde”
+aromatic +aldehyde	both words “aromatic” AND “aldehyde”
+aromatic -aldehyde	the word “aromatic” but NOT “aldehyde”
“aromatic aldehyde”	the exact phrase “aromatic aldehyde”
benz*	words which begin with “benz”, such as “benzene” or “benzyl”
benz*yl	words that begin with “benz” and end with “yl”, such as “benzyl” or “benzoyl”
benzyl~	words that are close to the word “benzyl”, such as “benzoyl” (i.e., fuzzy search)

BROWSE
Latest Articles
Most accessed
thematic issues
volumes
authors

BROWSE

Latest Articles Most Accessed Thematic Issues Volumes Authors

Author

2 article(s) from Prada, Elsa

Interaction-induced zero-energy pinning and quantum dot formation in Majorana nanowires

Samuel D. Escribano,
Alfredo Levy Yeyati and
Elsa Prada

Beilstein J. Nanotechnol. 2018, 9, 2171–2180, doi:10.3762/bjnano.9.203

PDF

Figure 1: (a) Schematic representation of the setup analyzed in the present work. A nanowire of rectangular c...

Jump to Figure 1

Figure 2: Majorana nanowire subject to interactions from the electrostatic environment (ignoring the influenc...

Jump to Figure 2

Figure 3: Majorana wave functions in the non-interacting case: Energy levels (a) and the absolute value of th...

Jump to Figure 3

Figure 4: Same as Figure 3 but for the interacting case (without leads). In the pinned regions the Majorana wave func...

Jump to Figure 4

Figure 5: Majorana nanowire subject to interactions from the electrostatic environment (including the influen...

Jump to Figure 5

Figure 6: Evolution with Zeeman field of the spectrum (a) and the absolute value of the Majorana charge Q_M (b...

Jump to Figure 6

Album

Supp Info

Full Research Paper

Published 15 Aug 2018

Full text

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

PDF

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

Jump to Figure 1

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

Jump to Figure 2

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

Jump to Figure 3

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

Jump to Figure 4

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...

Jump to Figure 5

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...

Jump to Figure 6

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...

Jump to Figure 7

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

Jump to Figure 8

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

Jump to Figure 9

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

Jump to Figure 10

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

Jump to Figure 11

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

Jump to Figure 12

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

Jump to Figure 13

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

Jump to Figure 14

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

Jump to Figure 15

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 ...

Jump to Figure 16

Album

Supp Info

Full Research Paper

Published 03 May 2018

Full text

Other Beilstein-Institut Open Science Activities

/ Help / Support & Contact / Alerts / Privacy Policy / Terms & Conditions / Impressum