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4 article(s) from Bakurskiy, Sergey V

Tunable superconducting neurons for networks based on radial basis functions

Andrey E. Schegolev,
Nikolay V. Klenov,
Sergey V. Bakurskiy,
Igor I. Soloviev,
Mikhail Yu. Kupriyanov,
Maxim V. Tereshonok and
Anatoli S. Sidorenko

Beilstein J. Nanotechnol. 2022, 13, 444–454, doi:10.3762/bjnano.13.37

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Figure 1: (a) Schematic illustration of a RBF network. (b) Schematic representation of a Gauss-neuron ensurin...

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Figure 2: Transfer functions (normalized) and their main characteristics for the Gauss-neuron. (a, b) Familie...

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Figure 3: (a) Amplitude of the transfer function and (b) its standard deviation from the Gaussian-like functi...

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Figure 4: (a) Dynamic transfer function of a Gauss-neuron for a trapezoidal external signal for different val...

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Figure 5: Sketch of the tunable kinetic inductance based on multilayer structure in the (a) closed and (b) op...

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Figure 6: Spatial distribution of the pair amplitude F in the hybrid structures (a) S–FM₁–s–FM₂–s–FM₁–s–FM₂–N...

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Figure 7: Kinetic inductance of the hybrid structures S–FM₁–s–FM₂–s–FM₁–s–FM₂–s–N and S–FM₁–n–FM₂–n–FM₁–n–FM₂...

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Full Research Paper

Published 18 May 2022

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Unipolar magnetic field pulses as an advantageous tool for ultrafast operations in superconducting Josephson “atoms”

Daria V. Popolitova,
Nikolay V. Klenov,
Igor I. Soloviev,
Sergey V. Bakurskiy and
Olga V. Tikhonova

Beilstein J. Nanotechnol. 2019, 10, 1548–1558, doi:10.3762/bjnano.10.152

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Figure 1: (a) The potential energy and the eigenfunctions (with energies E₁ ,E₂, E_3, E₄) of the three-junctio...

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Figure 2: Analytical solution of Equation 7 obtained in the limit Δ→0 for two different magnetic field strengths: V = 5...

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Figure 3: Analytical solution of Equation 7 obtained for Δ = 0.3, V = 5, dashed lines, solid lines, circles and squares...

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Figure 4: The time-dependent populations of states calculated when the 4th upper lying state of the supercond...

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Figure 5: Population of the upper qubit state of the superconducting meta-atom obtained analytically for V = ...

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Figure 6: Eigenvalues, E_1,2,3,4, of the unperturbed Hamiltonian and matrix elements (μ_ij) for transitions bet...

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Figure 7: (a) A schematic diagram of a transmission line in ASL circuits, through which a soliton-like curren...

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Full Research Paper

Published 29 Jul 2019

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Beyond Moore’s technologies: operation principles of a superconductor alternative

Igor I. Soloviev,
Nikolay V. Klenov,
Sergey V. Bakurskiy,
Mikhail Yu. Kupriyanov,
Alexander L. Gudkov and
Anatoli S. Sidorenko

Beilstein J. Nanotechnol. 2017, 8, 2689–2710, doi:10.3762/bjnano.8.269

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Figure 1: Voltage pulse on a Josephson junction corresponding to a SFQ transition and its mechanical analogy ...

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Figure 2: Josephson transmission line. Josephson junctions are shown by crosses. I_b is the applied bias curre...

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Figure 3: An RSFQ logic cell coupled to a clocking JTL. I_b is the applied bias current. Blue arrows present c...

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Figure 4: RSFQ power supply scheme.

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Figure 5: ERSFQ power supply scheme. L_b is the inductance limiting the bias current variation.

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Figure 6: eSFQ power supply scheme. The dotted rectangle marks the decision-making pair.

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Figure 7: Realization of a dc bias voltage source in RSFQ circuitry.

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Figure 8: RQL ac power supply scheme. The blue arrow shows the SFQ current, violet arrows present magnetic co...

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Figure 9: RQL transmission line with four-phase bias. I_b1,b2 are ac bias currents providing the power supply ...

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Figure 10: Notional (left) and practical (right) schematic of a parametric quantron. The cell state is conditi...

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Figure 11: Potential energy of a parametric quantron U_PQ (Equation 2) (solid lines) and its terms: magnetic energy U_M (d...

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Figure 12: Logical state transfer in an array of magnetically coupled parametric quantrons under a driving cur...

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Figure 13: nSQUID-based adiabatic data bus and RSFQ data bus. Blue arrows show circulating currents, orange ar...

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Figure 14: Principal scheme of implementation of write and read operations in a circuit based on MJJ valve.

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Figure 15: Cross section of an SF-NFS MJJ with CPRs of its parts shifted in phase by π. Arrows show F-layer ma...

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Figure 16: Sketch of an orthogonal spin transfer (OST) device. Arrows show magnetization directions in the dev...

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Review

Published 14 Dec 2017

Full text

Magnetic reversal dynamics of a quantum system on a picosecond timescale

Nikolay V. Klenov,
Alexey V. Kuznetsov,
Igor I. Soloviev,
Sergey V. Bakurskiy and
Olga V. Tikhonova

Beilstein J. Nanotechnol. 2015, 6, 1946–1956, doi:10.3762/bjnano.6.199

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Figure 1: Magnetization reversal of a two-level system is shown as a transition between the states “0” and “1...

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Figure 2: The dynamics of the ground level population, W_a, of an atomic system (µ₁₂ = 10µ₀, ω₁₂ ≈ 2·10¹³ Hz, a...

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Figure 3: The dynamics of the ground level population, W_a, of the flux qubit system (µ₁₂ = 10⁶µ_0, ω₁₂ ≈ 10¹⁰ ...

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Figure 4: Dependence of the optimal magnetic field value versus the external magnetic pulse duration, T, for ...

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Figure 5: The ground level population dynamics of both the atomic-based qubit for an oscillating magnetic fie...

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Figure 6: The potential energy and the wavefunctions for the flux-driven, three-junction qubit (described in [2]...

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Figure 7: The dynamics of the ground level population, W_a, and the populations of the two lowest excited leve...

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Full Research Paper

Published 28 Sep 2015

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