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New type of hybrid magnetic lens for practical applications of HTS bulk superconductors

Published 4 February 2021 © 2021 The Author(s). Published by IOP Publishing Ltd
, , Citation Shinya Nariki 2021 Supercond. Sci. Technol. 34 030501 DOI 10.1088/1361-6668/abcb47

0953-2048/34/3/030501

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This is a viewpoint on the letter by S Namba et al 2019 (Supercond. Sci. Technol. 32 12LT03).

High-Tc bulk superconductors such as RE-Ba-Cu-O (RE: a rare earth element) and MgB2 can trap high magnetic fields at low temperatures. The magnetized bulk superconductors can be used as a compact, high strength trapped field magnet (TFM) for many practical applications.

However, the trapped field is limited experimentally by the poor mechanical strength of the brittle ceramic material. A large Lorentz force is developed in the bulk during the magnetization process, which sometimes results in crack formation and propagation, leading to eventual mechanical failure. Remarkable progress has been made in increasing trapped fields with mechanical reinforcement using epoxy resin or shrink-fit stainless steel. Up to now, trapped magnetic fields over 17 T are achieved in RE-Ba-Cu-O disk pairs through field-cooling magnetization (FCM) [1, 2]. The group of Iwate University and University of Cambridge has been working on the magnetization techniques of bulk superconductors. Recently, Fujishiro et al [3] suggested the possibility to achieve a trapped field over 20 T in the RE-Ba-Cu-O disk pair by FCM method using numerical simulation. However, FCM requires a high applied field generated by a superconducting magnet, which has limitations for practical applications. Pulsed-field magnetization (PFM) is the most practical method to magnetize bulk superconductors since it is a faster magnetizing process than FCM and is an inexpensive and mobile experimental setup using a copper pulsed magnet. A trapped field of 5.2 T by PFM is reported in an HTS bulk [4]. A flux jump assisted multi-pulse magnetization has recently been reported led to a trapped field of 5.3 T in Gd-Ba-Cu-O bulk [5]. However, the maximum trapped field by PFM is still significantly lower than that achieved by FCM.

The magnetic lens was reported by Matsumoto et al for the first time in 2003 [6]. In this device, magnetic flux concentration was carried out by using hollow cylinders made of low- and high-temperatures superconductors. It is important to develop compact high magnetic field systems. A magnetic lens made of a Gd-Ba-Cu-O bulk was placed in a superconducting magnet. An external field of 2 T was amplified to 5.65 T at the center of the lens, demonstrating magnetic flux concentration by a Gd-Ba-Cu-O magnetic lens [7]. A concentrated field of Bc = 12.42 T has been obtained at 20 K for a background field of 8 T using a Gd-Ba-Cu-O bulk magnetic lens, and Bc = 30.35 T at 4.2 K achieved for a background field of 28.3 T [8].

Since the magnetic lens effect vanishes after the applied field decreased to zero, the external magnet must be operated continuously, which consumes energy and is not environmentally friendly. In 2018, the new concept of a hybrid trapped field magnet lens (HTFML) was reported [9]. This consists of a TFM cylinder exploiting the 'vortex pinning effect', combined with a bulk magnetic lens exploiting the 'diamagnetic shielding effect'. The HTFML can reliably generate a concentrated magnetic field in the central bore of the magnetic lens that is higher than both the trapped field in the single cylindrical bulk TFM and the external magnetizing field, even after the externally applied field decreases to zero. In this letter, the first experimental realization using HTFML device was presented. In the HTFML consisting of a Gd-Ba-Cu-O bulk lens and a MgB2 bulk TMF cylinder, a maximum concentrated magnetic field of Bc = 3.55 T was achieved at the central bore after removing the applied field of 2.0 T at 20 K. Although, the experimental value of Bc = 3.55 T is lower than the value predicted from numerical simulation, the concentrated field will be enhanced with the design optimization of HTFML.

A ring-shaped RE-Ba-Cu-O bulk superconductor is a strong candidate for NMR and MRI systems [10]. An Eu-Ba-Cu-O bulk is suitable for a compact NMR magnet because of its low relative magnetic permeability. The HTFML using a RE-Ba-Cu-O bulk TFM cylinder and a RE-Ba-Cu-O lens pair can be expected to achieve higher HTFM effect compared to that using a MgB2 bulk TFM cylinder [9, 11, 12]. Most recently, the performance of HTFML consisting of an Eu-Ba-Cu-O bulk TFM cylinder and a Gd-Ba-Cu-O lens was reported [13]. At 77 K, a concentrated magnetic field of Bc = 0.8 T was experimentally confirmed after removing an applied magnetic field of 0.5 T. The concentrated magnetic field will be enhanced with lowering the operating temperature. In this letter, the authors mentioned that the goal of a concentrated magnetic field is over 10 T (e.g. Bc = 13.5 T) when an applied field is 10 T. It is extremely effective for an improvement in the resolution of a compact NMR. The realization of the magnetic field over 10 T in an open space using the HTML system will accelerate practical applications of bulk superconductors.

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