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Beilstein J. Nanotechnol. 2026, 17, 292–302, doi:10.3762/bjnano.17.20
Figure 1: (a) Normalized resistive transitions and (b) μ0Hc2(T) for the NbRe/Au and NbRe/Py bilayers. The red...
Figure 2: I–V curves of (a) NbRe/Au and (b) NbRe/Py bilayers at t ≈ 0.5 in different magnetic fields from 3 m...
Figure 3: Magnetic field dependence for the critical current density at t ≈ 0.5 of NbRe/Au (a) and NbRe/Py (b...
Figure 4: Dissipated power at the instability point as a function of the magnetic field at t ≈ 0.5 for NbRe/A...
Figure 5: Vortex critical velocity as a function of the magnetic field for NbRe/Au and NbRe/Py at t ≈ 0.5. Th...
Beilstein J. Nanotechnol. 2024, 15, 1440–1452, doi:10.3762/bjnano.15.116
Figure 1: Top and side views of relaxed geometries, PDOS, and EBSs of (a) ψ-graphene, (b) ψ-graphone, and (c)...
Figure 2: Relaxed 2 × 2 × 1 supercell’s top and side views, PDOS, and EBS of ψ-graphene (a) at 0% and (b) −14...
Figure 3: Relaxed 2 × 2 × 1 supercell’s top and side views, PDOS, and EBS of ψ-graphone (a) at +1% and (b) at...
Figure 4: Relaxed 2 × 2 × 1 supercell’s top and side views, PDOS, and EBS of ψ-graphane (a) at −17% and (b) +...
Figure 5: Variation of (i) bandgap energy Eg and (ii) buckling height h of (a) ψ-graphene, (b) ψ-graphone, an...