Growth and anisotropic transport properties of off-axis MgB2 thin films

Wang, Hongzhang; Li, Yulong; Wang, Yue; Gan, Zizhao

doi:10.1016/j.physc.2019.1353587

Cited by 5 publications

(1 citation statement)

References 29 publications

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“…Near zero applied field, it is shown that the J c is in the range 1.2 − 2.6 × 10 6 A cm −2 at temperatures 5-25 K, with the value 1.7 × 10 6 A cm −2 at 5 K-10 K lower than 2.6 × 10 6 A cm −2 at 15 K because of the suppression from flux jumps at 5-10 K as exemplified in the inset of figure 10(a) [52]. We note that these J c values are lower than the superior values of above 10 7 A cm −2 for high-quality epitaxial MgB 2 thin films [36,67], but comparable to both typical values for epitaxial MgB 2 films [68] and that reported on high-quality polycrystalline MgB 2 planar films [33,36,69]. According to previous simulations [18,19,26], these values of J c would be promising for potential applications in ICF.…”

Section: Superconducting Transitionmentioning

confidence: 67%

Properties of superconducting MgB₂ spherical shells deposited on 2 mm and 1 mm diameter Si₃N₄ spheres

Xu¹,

Sun²,

Zhao³

et al. 2023

Supercond. Sci. Technol.

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Superconducting spherical shells may not only provide an appealing platform for exploring superconductivity in three-dimensional (3D) geometries with curved surfaces, but also be practically applied in important fields, such as in gyroscopes and gravimeters. In inertial confinement fusion (ICF), the perturbation on the target capsule caused by traditional contact support methods is recognized as one of the major contributors to performance degradation in ICF implosions. It was proposed recently that coating the capsule with a thin superconducting MgB2 spherical shell to realize non-contact support by means of magnetic levitation at the required temperatures ∼ 20 K might offer a promising solution to this longstanding problem. To simulate the coating of ICF capsules, we deposited MgB2 spherical shells onto polycrystalline Si3N4 spheres (diameter d = 2 mm and 1 mm) via a hybrid physical–chemical vapour deposition technique. For both diameters, the spherical shells, of about 1 µm in thickness and covering the whole spheres completely, were polycrystalline with thin plate-shaped MgB2 crystallites oriented randomly and closely connected. The spherical shells exhibited superconducting transition at a zero resistance temperature T c z e r o of 38.5–39.4 K in four-probe resistance measurements and ideal diamagnetism at low temperatures in magnetization measurements, suggesting the good crystallinity and homogeneity of the shells. The upper critical field H c 2 , the irreversibility field H i r r and the lower critical field H c 1 were characterized and showed similar magnitudes and temperature dependencies for the d = 2 mm and 1 mm shells, yielding H i r r of 7–8 T and H c 1 of 7–12 mT at 20 K. The superconducting critical current density J c values, evaluated from the magnetization hysteresis loops, were 1.8 × 10 6 A cm−2 and 8.5 × 10 4 A cm−2 at 20 K under zero and 2 T applied field, respectively, for the d = 1 mm shell. The occurrence of small flux jumps was observed at low temperatures up to 12 K and in low fields below 0.3 T. The results demonstrate the feasibility of fabricating MgB2 spherical shells with properties applicable to potential areas employing magnetic levitation such as in ICF and that MgB2 spherical shells may be exploited as an experimental system to study superconductivity in 3D curvilinear geometry.

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