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Beilstein J. Nanotechnol. 2019, 10, 1548–1558, doi:10.3762/bjnano.10.152
Figure 1: (a) The potential energy and the eigenfunctions (with energies E1 ,E2, E3, E4) of the three-junctio...
Figure 2: Analytical solution of Equation 7 obtained in the limit Δ→0 for two different magnetic field strengths: V = 5...
Figure 3: Analytical solution of Equation 7 obtained for Δ = 0.3, V = 5, dashed lines, solid lines, circles and squares...
Figure 4: The time-dependent populations of states calculated when the 4th upper lying state of the supercond...
Figure 5: Population of the upper qubit state of the superconducting meta-atom obtained analytically for V = ...
Figure 6: Eigenvalues, E1,2,3,4, of the unperturbed Hamiltonian and matrix elements (μij) for transitions bet...
Figure 7: (a) A schematic diagram of a transmission line in ASL circuits, through which a soliton-like curren...
Beilstein J. Nanotechnol. 2015, 6, 1946–1956, doi:10.3762/bjnano.6.199
Figure 1: Magnetization reversal of a two-level system is shown as a transition between the states “0” and “1...
Figure 2: The dynamics of the ground level population, Wa, of an atomic system (µ12 = 10µ0, ω12 ≈ 2·1013 Hz, a...
Figure 3: The dynamics of the ground level population, Wa, of the flux qubit system (µ12 = 106µ0, ω12 ≈ 1010 ...
Figure 4: Dependence of the optimal magnetic field value versus the external magnetic pulse duration, T, for ...
Figure 5: The ground level population dynamics of both the atomic-based qubit for an oscillating magnetic fie...
Figure 6: The potential energy and the wavefunctions for the flux-driven, three-junction qubit (described in [2]...
Figure 7: The dynamics of the ground level population, Wa, and the populations of the two lowest excited leve...