Development of a persistent-mode NMR magnet with superconducting joints between high-temperature superconductors

This paper describes the first persistent-mode medium magnetic field (400 MHz; 9.39 T) nuclear magnetic resonance (NMR) magnet which uses superconducting joints between high-temperature superconductors (HTSs). As the ultimate goal, we aim to develop a high-resolution 1.3 GHz (30.5 T) NMR magnet operated in the persistent-mode. The magnet requires superconducting joints between HTSs and those between an HTS and a low-temperature superconductor (LTS). Towards this goal, we have been developing persistent-mode HTS inner coils to be operated in a 400 MHz (9.39 T) NMR magnet and here we present the first prototype inner coil wound with a single piece (RE = rare earth)Ba2Cu3O7−x (REBCO) conductor. The coil and a REBCO persistent current switch are connected with intermediate grown superconducting joints with high critical currents in external magnetic fields. To evaluate the performance of the joints in an ultimately stable and homogeneous magnetic field, the coil is operated in the persistent-mode, generating 0.1 T, in a 9.3 T background magnetic field of a persistent-mode LTS outer coil. The magnetic field drift over two years of the 400 MHz LTS/REBCO NMR magnet is as small as ∼1 ppm, giving high-resolution NMR spectra. The magnetic field drift rate over the second year was 0.03 × 10−3 ppm h−1, which is more than three orders of magnitude smaller than that required for an NMR magnet, demonstrating that the superconducting joints function satisfactorily in a high-resolution NMR system. The corresponding joint resistance is inferred to be <10−14 Ω.

[1]  T. Takao,et al.  Quench and self-protecting behaviour of an intra-layer no-insulation (LNI) REBCO coil at 31.4 T , 2021, Superconductor Science and Technology.

[2]  Y. Ikuhara,et al.  Nanostructural evolution of intermediate grown superconducting joint layers between GdBa2Cu3Oy coated conductors , 2020, Superconductor Science and Technology.

[3]  T. Takao,et al.  Hoop Stress Modification, Stress Hysteresis and Degradation of a REBCO Coil Due to the Screening Current Under External Magnetic Field Cycling , 2020, IEEE Transactions on Applied Superconductivity.

[4]  Y. Yanagisawa,et al.  Future prospects for NMR magnets: A perspective. , 2019, Journal of magnetic resonance.

[5]  Y. Ishii,et al.  The MIRAI Program and the New Super-High Field NMR Initiative and Its Relevance to the Development of Superconducting Joints in Japan , 2019, IEEE Transactions on Applied Superconductivity.

[6]  Y. Yanagisawa,et al.  Superconducting joint between multi-filamentary Bi2Sr2Ca2Cu3O10+δ tapes based on incongruent melting for NMR and MRI applications , 2019, Superconductor Science and Technology.

[7]  D. Park,et al.  Design of a Tabletop Liquid-Helium-Free 23.5-T Magnet Prototype Toward 1-GHz Microcoil NMR , 2019, IEEE Transactions on Applied Superconductivity.

[8]  Shin-ichi Kobayashi,et al.  High Ic superconducting joint between Bi2223 tapes , 2019, Applied Physics Express.

[9]  S. Mukoyama,et al.  Superconducting joint of REBCO wires for MRI magnet , 2018, Journal of Physics: Conference Series.

[10]  S. Mukoyama,et al.  Performance of an HTS Persistent Current System for REBCO Pancake Coil , 2018, IEEE Transactions on Applied Superconductivity.

[11]  Y. Yanagisawa,et al.  Degradation of the performance of an epoxy-impregnated REBCO solenoid due to electromagnetic forces , 2018 .

[12]  佑 末富,et al.  Development plan of a persistent 1.3 GHz NMR magnet in a new MIRAI project on joint technology for HTS wires/cables in Japan , 2018 .

[13]  T. Takao,et al.  Fabrication, microstructure and persistent current measurement of an intermediate grown superconducting (iGS) joint between REBCO-coated conductors , 2017 .

[14]  T. Takao,et al.  Degradation of a REBCO conductor due to an axial tensile stress under edgewise bending: a major stress mode of deterioration in a high field REBCO coil’s performance , 2017 .

[15]  Y. Nishiyama,et al.  Development of Super‐High‐Field NMR Operated Beyond 1 GHz Using High‐Temperature Superconducting Coils , 2016 .

[16]  Dong Lak Kim,et al.  400-MHz/60-mm All-REBCO Nuclear Magnetic Resonance Magnet: Magnet Design , 2016, IEEE Transactions on Applied Superconductivity.

[17]  G. Nishijima,et al.  Successful Upgrading of 920-MHz NMR Superconducting Magnet to 1020 MHz Using Bi-2223 Innermost Coil , 2016, IEEE Transactions on Applied Superconductivity.

[18]  T. Takao,et al.  High resolution NMR measurements using a 400MHz NMR with an (RE)Ba2Cu3O7-x high-temperature superconducting inner coil: Towards a compact super-high-field NMR. , 2016, Journal of magnetic resonance.

[19]  T. Takao,et al.  Shimming for the 1020 MHz LTS/Bi-2223 NMR Magnet , 2016, IEEE Transactions on Applied Superconductivity.

[20]  T. Takao,et al.  Degradation of a REBCO Coil Due to Cleavage and Peeling Originating From an Electromagnetic Force , 2016, IEEE Transactions on Applied Superconductivity.

[21]  C. Grovenor,et al.  Persistent current joints between technological superconductors , 2015 .

[22]  G. Nishijima,et al.  Achievement of 1020MHz NMR. , 2015, Journal of magnetic resonance.

[23]  Y. Yanagisawa,et al.  Development of a superconducting joint between a GdBa2Cu3O7-δ-coated conductor and YBa2Cu3O7−δ bulk: towards a superconducting joint between RE (Rare Earth) Ba2Cu3O7−δ-coated conductors , 2015 .

[24]  J. Voccio,et al.  A High-Resolution 1.3-GHz/54-mm LTS/HTS NMR Magnet , 2015, IEEE Transactions on Applied Superconductivity.

[25]  Ruth Nussinov,et al.  Aβ(1–42) Fibril Structure Illuminates Self-recognition and Replication of Amyloid in Alzheimer’s , 2015, Nature Structural &Molecular Biology.

[26]  D. Larbalestier,et al.  Comparison of growth texture in round Bi2212 and flat Bi2223 wires and its relation to high critical current density development , 2014, Scientific Reports.

[27]  T. Takao,et al.  Operation of a 400MHz NMR magnet using a (RE:Rare Earth)Ba2Cu3O7-x high-temperature superconducting coil: Towards an ultra-compact super-high field NMR spectrometer operated beyond 1GHz. , 2014, Journal of magnetic resonance.

[28]  Haigun Lee,et al.  A superconducting joint for GdBa2Cu3O7|[minus]||[delta]|-coated conductors , 2014 .

[29]  Christian Scheuerlein,et al.  Isotropic round-wire multifilament cuprate superconductor for generation of magnetic fields above 30 T. , 2014, Nature materials.

[30]  M. Yoshikawa,et al.  Operation of a 500 MHz high temperature superconducting NMR: towards an NMR spectrometer operating beyond 1 GHz. , 2010, Journal of magnetic resonance.

[31]  T. Takao,et al.  Towards beyond 1 GHz NMR: Mechanism of the long-term drift of screening current-induced magnetic field in a Bi-2223 coil , 2009 .

[32]  Min Cheol Ahn,et al.  Operation and performance analyses of 350 and 700 MHz low-/high-temperature superconductor nuclear magnetic resonance magnets: A march toward operating frequencies above 1 GHz , 2009 .

[33]  S. Matsumoto,et al.  Field Stability of a 600 MHz NMR Magnet in the Driven-Mode Operation , 2008, IEEE Transactions on Applied Superconductivity.

[34]  Hideaki Maeda,et al.  Towards beyond-1 GHz solution NMR: internal 2H lock operation in an external current mode. , 2008, Journal of magnetic resonance.

[35]  S. Hahn,et al.  Field Mapping, NMR Lineshape, and Screening Currents Induced Field Analyses for Homogeneity Improvement in LTS/HTS NMR Magnets , 2008, IEEE Transactions on Applied Superconductivity.

[36]  L. Kay,et al.  A Gradient-Enhanced HCCH-TOCSY Experiment for Recording Side-Chain 1H and 13C Correlations in H2O Samples of Proteins , 1993 .