# US 7,745,376 B2 · Superconducting composite

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- Number: US 7,745,376 B2
- Document ID: US7745376B2
- Status: Granted
- Kind: B2
- Application number: 11/195,992
- Filed: 2005-08-02
- Published: 2007-08-23
- Granted: 2010-06-29
- Earliest claimed: 2004-08-10
- Assignees: Nove Technologies, Inc.
- Inventors: Matthew J. Holcomb
- Web page: https://patentgrep.com/patent/US7745376B2

## CPC

- H10N 60/202: {comprising metal borides, e.g. MgB2}
- Y10T 29/49014: Superconductor
- Y10T 428/2991: Coated
- H10N: ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- Y10T: TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION

## Abstract

The invention provides a superconductor comprising particles made of a superconductive material, and a conductive material. The conductive material is selected to be driven to a superconductive state when in proximity to the superconductive material, and preferably at least includes bismuth. An unbroken length of the conductive material is located sufficiently close to a plurality of the particles to be driven to a superconductive state by the superconductive material.

## Claims

### Claim 1

A superconductor, comprising:
a plurality of particles made of a superconductive material; and
a conductive material at least including bismuth semimetal, an unbroken section of the conductive material being located sufficiently close to the plurality of the particles to be driven to a superconductive state by the plurality of particles.

### Claim 2 (depends on 1)

The superconductor of claim 1, wherein the superconductive material is magnesium diboride.

### Claim 3 (depends on 1)

The superconductor of claim 1, wherein the unbroken section of the conductive material is in contact with the plurality of particles.

### Claim 4 (depends on 1)

The superconductor of claim 1, wherein a substantial volume of the unbroken section of the conductive material being located at a distance greater than the thermal limit of the proximity decay length and less than the inelastic mean free path of the superconductive material from the plurality of particles at a temperature less than the superconducting critical temperature of the plurality of particles.

### Claim 5 (depends on 1)

The superconductor of claim 1, wherein the bismuth semimetal has a larger inelastic mean free pat than lead/bismuth alloy at 20K.

### Claim 6 (depends on 5)

The superconductor of claim 5, wherein the bismuth semimetal has an inelastic mean free path at 20K of at least 2000 nm.

### Claim 7

A method of making a superconductor, comprising:
forming a plurality of particles of a superconductive material; and
locating a conductive material adjacent the plurality of particles, the conductive material at least including bismuth semimetal, and an unbroken length of the conductive material being in sufficiently close proximity to the plurality of the particles to be driven to a superconductive state by the plurality of particles.

### Claim 8 (depends on 7)

The method of claim 7, wherein the superconductive material is magnesium diboride.

### Claim 9 (depends on 8)

The method of claim 8, further comprising:
assembling an elongate member from the unbroken length of the conductive material and the plurality of particles; and
drawing the elongate member into a wire.

### Claim 10 (depends on 7)

The method of claim 7, wherein a substantial volume of the unbroken section of the conductive material being located at a distance greater than the thermal limit of the proximity decay length and less than the inelastic mean free path of the superconductive material from the plurality of particles of superconductive material at a temperature less than the superconducting critical temperature of the plurality of particles.

### Claim 11 (depends on 7)

The method of claim 7, wherein the bismuth semimetal has a larger inelastic mean free pat than lead/bismuth alloy at 20K.

### Claim 12 (depends on 11)

The method of claim 11, wherein the bismuth semimetal has an inelastic mean free path at 20K of at least 2000 nm.