2 article(s) from Yeyati, Alfredo Levy
- Full Research Paper
- Published 15 Aug 2018
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Figure 1: (a) Schematic representation of the setup analyzed in the present work. A nanowire of rectangular c...
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Figure 2: Majorana nanowire subject to interactions from the electrostatic environment (ignoring the influenc...
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Figure 3: Majorana wave functions in the non-interacting case: Energy levels (a) and the absolute value of th...
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Figure 4: Same as Figure 3 but for the interacting case (without leads). In the pinned regions the Majorana wave func...
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Figure 5: Majorana nanowire subject to interactions from the electrostatic environment (including the influen...
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Figure 6: Evolution with Zeeman field of the spectrum (a) and the absolute value of the Majorana charge QM (b...
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Supp. Info
- Full Research Paper
- Published 06 Jun 2018
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Figure 1: Schematic setups studied in this paper. a) S–QD–TS geometry: S denotes a conventional s-wave BCS su...
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Figure 2: Phase dependence of the subgap spectrum of an S–QD–TS junction in the noninteracting case, U = 0. T...
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Figure 3: Phase-dependent ABS spectrum from mean-field theory for S–QD–TS junctions as in Figure 2 but with U > 0 and...
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Figure 4: Main panel: Mean-field results for the CPR of S–QD–TS junctions with different Γ/Δ values, where we...
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Figure 5: Main panel: Mean-field results for the critical current Ic vs local magnetic field scale Bx in S–QD...
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Figure 6: Main panel: Critical current Ic vs Zeeman energy Vx for an S–TS junction using the spinful TS nanow...
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Figure 7: CPR for the S–TS junction with
![[Graphic 75]](/bjnano/content/inline/2190-4286-9-158-i137.svg?max-width=637&scale=1.18182)
= 1 in Figure 6, for different bulk Zeeman fields Vx (in meV) near the crit...
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Figure 8: Main panel: Critical current Ic vs Zeeman energy Vx for S–QD–TS junctions from mean-field theory us...
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Figure 9: Main panel: Mean-field results for Ic vs Bz in S–QD–TS junctions for several values of ΓS = ΓTS = Γ...
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