2021
DOI: 10.1103/physrevb.104.094526
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Critical current in thin flat superconductors with Bean-Livingston and geometrical barriers

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Cited by 8 publications
(3 citation statements)
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“…According to the previous studies, the H dependence of I c showed a sharp peak. 19,20,[36][37][38] This behavior has been observed in the thin film of V and Nb, 21) however, in our thin film, there were broad peaks around H = −15 Oe for I + and H = 15 Oe for I − . Further, there was a difference between the H at which the I c and η showed maximum.…”
supporting
confidence: 65%
“…According to the previous studies, the H dependence of I c showed a sharp peak. 19,20,[36][37][38] This behavior has been observed in the thin film of V and Nb, 21) however, in our thin film, there were broad peaks around H = −15 Oe for I + and H = 15 Oe for I − . Further, there was a difference between the H at which the I c and η showed maximum.…”
supporting
confidence: 65%
“…[4] The effects of the current streamline bending on the vortex dynamics can be probed, for instance, via the artificial introduction of a single edge defect. [5][6][7] An edge defect locally suppresses the energy barrier for the vortex entry [8] and acts as a gate for fluxons which then cross the superconducting constriction under the action of the transport current. [9] The repulsive interaction between vortices stipulates their arrangement in the form of a vortex jet, [10] which has an apex at the defect and diverges toward the opposite edge of the constriction, see Figure 1b.…”
Section: Introductionmentioning
confidence: 99%
“…The geometrical barrier originates from the shape of the superconductor and it appears for samples different from an ellipsoid. In the case of superconductor thin strips with thickness d ≪ λ , in which vortices interact mostly via the stray fields in the surrounding space, the vortex-vortex and vortex-image interaction length scale is determined by the noticeably larger effective penetration depth * Corresponding author: oleksandr.dobrovolskiy@univie.ac.at λ eff = λ 2 /d [30,31] while effects of the geometrical barrier are not essential [32].…”
Section: Introductionmentioning
confidence: 99%