Proximity coupling of superconducting nanograins with fractal distributions

Takashi Uchino, Nanami Teramachi, Ryosuke Matsuzaki, Emi Tsushima, Shusuke Fujii, Yusuke Seto, Kazuyuki Takahashi, Takao Mori, Yutaka Adachi, Yukihito Nagashima, Yoshifumi Sakaguchi, Kazuki Ohishi, Akihiro Koda, Takahiro Sakurai, and Hitoshi Ohta
Phys. Rev. B 101, 035146 – Published 27 January 2020
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Abstract

We explore the electrical and magnetic properties of a fractal assembly of Josephson junctions with transparent interfaces. For this purpose, we employ an Mg/MgO/MgB2 nanocomposite with ∼16 vol. % of MgB2 nanograins, which are distributed in a fractal manner in the normal matrix. Irrespective of the low volume fraction of MgB2 nanograins, the nanocomposite behaves as a bulk-like superconductor, i.e., zero resistivity, perfect diamagnetism, and strong vortex pinning. Thus, a global Josephson phase coherence is achieved in the nanocomposite. The lower (Hc1J) and higher (Hc2J) critical fields of the Josephson network are exceptionally high (Hc1J=96Oe and Hc2J=83.5kOe) as compared to those reported previously for granular superconductors. This will give an example of robust macroscopic superconducting coherence derived from long-range proximity coupling among fractally distributed superconducting nanograins through quantum interference of Andreev quasiparticles. Transverse-field muon spin rotation measurements reveal that the mean internal field in the superconducting mixed state increases with decreasing temperature below which the Josephson phase coherence sets in, opposite to the diamagnetic response observed in magnetization measurements. This unusual behavior implies a highly disordered and fluctuating nature of the Josephson vortices in the present superconducting nanocomposite.

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  • Received 1 November 2019
  • Revised 8 January 2020

DOI:https://doi.org/10.1103/PhysRevB.101.035146

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Takashi Uchino1,*, Nanami Teramachi1, Ryosuke Matsuzaki1, Emi Tsushima1, Shusuke Fujii1, Yusuke Seto2, Kazuyuki Takahashi1, Takao Mori3, Yutaka Adachi4, Yukihito Nagashima5, Yoshifumi Sakaguchi6, Kazuki Ohishi6, Akihiro Koda7, Takahiro Sakurai8, and Hitoshi Ohta9

  • 1Department of Chemistry, Graduate School of Science, Kobe University, Nada, Kobe 657–8501, Japan
  • 2Department of Planetology, Graduate School of Science, Kobe University, Nada, Kobe 657–8501, Japan
  • 3International Center for Materials Nanoarchitectonics, National Institute for Materials Science, Namiki 1-1, Tsukuba 305–0044, Japan
  • 4Optoelectonic Materials Group, Optical and Electronic Materials Unit, National Institute for Materials Science, Namiki 1-1, Tsukuba 305–0044, Japan
  • 5Nippon Sheet Glass Co., LTD., Konoike, Itami 664–8520, Japan
  • 6Neutron Science and Technology Center, Comprehensive Research Organization for Science and Society (CROSS), Tokai 319–1106, Japan
  • 7Institute of Materials Structure Science, High Energy Accelerator Research Organization, Tsukuba, Ibaraki 305–0801, Japan
  • 8Center for Support to Research and Education Activities, Kobe University, Nada, Kobe 657–8501, Japan
  • 9Molecular Photoscience Research Center, Kobe University, Nada, Kobe 657–8501, Japan

  • *uchino@kobe-u.ac.jp

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Issue

Vol. 101, Iss. 3 — 15 January 2020

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