In various embodiments, superconducting wires feature assemblies of clad composite filaments and/or stabilized composite filaments embedded within a wire matrix. The wires may include one or more stabilizing elements for improved mechanical properties.

Quench protected structured (QPS) superconducting cables, methods of fabricating the same, and methods of bending the same are disclosed. The methods of bending the QPS superconducting cables can be employed to produce windings. The QPS superconducting cables can rapidly drive a distributed quench to a normal conducting state in a superconducting cable if a region of the cable spontaneously quenches during high current operation.

There is a superconducting article that includes a superconducting film comprising a substrate, one or more buffer layers, and a high temperature superconducting (HTS) layer. The superconducting layer may be comprised of the chemical composition REBa.sub.2Cu.sub.3O.sub.7?x, where RE is one or more rare earth elements, for example: Y, La, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb and Lu. The superconductor layer is produced using Photo-Assisted Metal Organic Chemical Vapor Deposition (PAMOCVD) and contains non-superconducting nanoparticles. The nanoparticles are substantially provided in the a-b plane and naturally oriented. The non-superconducting nanoparticles provide flux pinning centers that improve the critical current properties of the superconducting film.

A high temperature superconducting, HTS, current lead comprising an HTS cable including a plurality of HTS tapes, a braided sleeve around the HTS cable, and a stabiliser material impregnating the HTS cable and the braided sleeve, the stabiliser material having a melting point above 290K and below a thermal degradation temperature of the HTS tapes.

Disclosed herein are superconducting wires. The superconducting wires can comprise a metallic matrix and at least one continuous subelement embedded in the matrix. Each subelement can comprise a non-superconducting core, a superconducting layer coaxially disposed around the non-superconducting core, and a barrier layer coaxially disposed around the superconducting layer. The superconducting layer can comprise a plurality of Nb.sub.3Sn grains stabilized by metal oxide particulates disposed therein. The Nb.sub.3Sn grains can have an average grain size of from 5 nm to 90 nm (for example, from 15 nm to 30 nm). The superconducting wire can have a high-field critical current density (J.sub.c) of at least 5,000 A/mm.sup.2 at a temperature of 4.2 K in a magnetic field of 12 T. Also described are superconducting wire precursors that can be heat treated to prepare superconducting wires, as well as methods of making superconducting wires.

A technique relates a superconducting microwave cavity. An array of posts has different heights in the cavity, and the array supports a localized microwave mode. The array of posts includes lower resonant frequency posts and higher resonant frequency posts. The higher resonant frequency posts are arranged around the lower resonant frequency posts. A first plate is opposite a second plate in the cavity. One end of the lower resonant frequency posts is positioned on the second plate so as to be electrically connected to the second plate. Another end of the lower resonant frequency posts in the array is open so as not to form an electrical connection to the first plate. Qubits are connected to the lower resonant frequency posts in the array of posts, such that each of the qubits is physically connected to one or two of the lower resonant frequency posts in the array of posts.

In various embodiments, superconducting wires incorporate diffusion barriers composed of Ta alloys that resist internal diffusion and provide superior mechanical strength to the wires.

Insulative superconductor coatings are provided which include amorphous ceramic thin films deposited at low temperature. The breakdown strength and thermal resistance performance of the insulative layer are advantageous even at very thin thicknesses and the mechanical strength characteristics are aided by compressive stress profiles resulting from the processes disclosed. The thin insulative layers thus enable unique superconductor architectures while maintaining high current density performance characteristics.

Insulative superconductor coatings are provided which include amorphous ceramic thin films deposited at low temperature. The breakdown strength and thermal resistance performance of the insulative layer are advantageous even at very thin thicknesses and the mechanical strength characteristics are aided by compressive stress profiles resulting from the processes disclosed. The thin insulative layers thus enable unique superconductor architectures while maintaining high current density performance characteristics.

Examples described in this disclosure relate to superconducting devices, including reciprocal quantum logic (RQL) compatible devices. A superconducting device including at least one superconducting element having a first coefficient of thermal expansion is provided. The at least one superconducting element is formed on a dielectric layer having a second coefficient of thermal expansion and the first coefficient of thermal expansion is different from the second coefficient of thermal expansion causing a strain mismatch between the at least one superconducting element and the dielectric layer when the superconducting device is operating in a cryogenic environment. The superconducting device may also include at least one dummy element configured to lower stress at an interface between the at least one superconducting element and the dielectric layer when the at least one superconducting device is operating in the cryogenic environment.