Abstract
The magnetisation reversal phenomena in the superconducting quantum interference device (SQUID) with the single \({{\varphi }_{0}}\) junction is investigated. Dynamics of the considered system is described in the framework of Landau–Lifshitz–Gilbert equation for magnetization of the ferromagnetic layer and resistively shunted junction model for phase difference of \({{\varphi }_{0}}\) Josephson junction. We have demonstrated the magnetization reversal by the pulse of the external magnetic field. The effect of parameters on the realization of magnetization reversal is clarified. It is shown that the magnetisation reversal has a periodic behaviour on the amplitude of pulse and SQUID inductance. We expect the obtained results can be used in different applications of modern superconducting electronics and spintronics.
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04 December 2023
An Erratum to this paper has been published: https://doi.org/10.1134/S1547477123060456
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Funding
This work is supported by the Russian Science Foundation (RSF) in the framework of research project no. 22-42-04408. Numerical simulations were funded by the RSF project no. 18-71-10095.
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The original online version of this article was revised: Surname of the first author should read Rahmonov and surname of the second author should read Rahmonova.
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Rahmonov, I.R., Rahmonova, A.R. & Shukrinov, Y.M. Magnetization Reversal by Pulse of Magnetic Field in SQUID with Single φ0-Junction. Phys. Part. Nuclei Lett. 20, 1161–1164 (2023). https://doi.org/10.1134/S1547477123050643
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DOI: https://doi.org/10.1134/S1547477123050643