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3 article(s) from Kupriyanov, Mikhail Yu.

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

Full text

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

Thickness dependence of the triplet spin-valve effect in superconductor–ferromagnet–ferromagnet heterostructures

Daniel Lenk,
Vladimir I. Zdravkov,
Jan-Michael Kehrle,
Günter Obermeier,
Aladin Ullrich,
Roman Morari,
Hans-Albrecht Krug von Nidda,
Claus Müller,
Mikhail Yu. Kupriyanov,
Anatolie S. Sidorenko,
Siegfried Horn,
Rafael G. Deminov,
Lenar R. Tagirov and
Reinhard Tidecks

Beilstein J. Nanotechnol. 2016, 7, 957–969, doi:10.3762/bjnano.7.88

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Figure 1: Sketch of the prepared Nb/Cu₄₁Ni₅₉/nc-Nb/Co/CoO_x sample system SF₁NF₂-AF1. The dotted lines indicat...

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Figure 2: Cross-sectional TEM images of samples SF₁NF₂-AF1 #5, #20, and #25 from left to right. The dashed ye...

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Figure 3: Thickness analysis of the sample series SF₁NF₂-AF1. While the solid squares show the data obtained ...

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Figure 4: (a) Magnetic hysteresis loop of SF₁NF₂-AF1#1 recorded by a SQUID magnetometer. Here, m is the magne...

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Figure 5: Superconducting transition as a function of the temperature, T, and the applied magnetic field, H, ...

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Figure 6: (a) Superconducting transition temperature T_c of SF₁NF₂-AF1#22 as a function of the applied magneti...

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Figure 7: (a) Dimensionality parameter α and (b) the (fictive) upper critical field at zero temperature, H_c(0...

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Figure 8: Superconducting transition temperature, T_c0, in zero external magnetic field as a function of the F₁...

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Figure 9: Maximum reduction of the transition temperature, ΔT_c,max by the triplet SSV effect at crossed confi...

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Full Research Paper

Published 04 Jul 2016

Full text

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