Method of controlling a super conductor

• US 5,872,368 A
• Filed: 11/30/1995
• Issued: 02/16/1999
• Est. Priority Date: 11/30/1995
• Status: Expired due to Fees

• Current Assignee: the united states of america as represented by the secretary of the navy
• Original Assignee: the united states of america as represented by the secretary of the navy
• Inventors: Johnson, Mark, Auyeung, Raymond, Osofsky, Michael, Chrisey, Doug B., Soulen, Robert J. Jr., Horwitz, James S.
• Primary Examiner(s): Whitehead, Jr., Carl W.
• Assistant Examiner(s): WILSON, ALLAN R
• Application Number:
  US08/565,487
• Time in Patent Office: 1,174 Days
• Field of Search: 257/31, 257/32, 257/33, 257/35, 257/36, 257/37, 257/38, 505/190, 505/193, 505/220, 505/235, 505/310, 505/329, 505/702, 505/706, 505/726, 505/842, 505/874
• US Class Current: 257/34
• CPC Class Codes: H10N 60/207 Field effect devices
• CPC Class Codes: Y10S 505/726 Measuring or testing of superconducting property
• CPC Class Codes: Y10S 505/842 Measuring and testing

Abstract

The order parameter of a superconductor is reduced by injecting spin-polarized carriers into the superconductor. The reduction in the order parameter is used to modulate the critical current of the superconductor. In a typical embodiment, a current is caused to flow through a superconductor. Spin polarized electrons are then injected into the path of the current in the superconductor by biasing a magnetic metal with respect to a terminal of the superconductor. The bias current may be varied to modulate the injection and thus the flow of current through the superconductor.

Claims

1. A method for modulating a superconducting current in at least one region of a superconductor having paired spin-up and spin-down charge carriers, comprising the step of suppressing the order parameter within said at least one region of said superconductor by injecting spin-polarized charge carriers into said at least one region of said superconductor.

2. A method of suppressing the superconductivity of a superconducting material, comprising the steps of:

driving, from a first terminal of said superconducting material to a second terminal of said superconducting material, a superconducting current along a layer of superconducting material, said layer of superconducting material being in electrical contact with a layer of spin injection material capable of producing a spin-polarized current of spin-polarized carriers;

electrically biasing said spin injection material with respect to said superconducting material so that a spin-polarized current of said spin-polarized carriers from said spin-injection material is injected into said superconducting layer between said first and second terminals, whereby said injected spin-polarized carriers reduce the order parameter of said superconducting layer between said first and second terminals.

3. The method of claim 2 wherein said spin-polarized carriers are electrons.

4. The method of claim 2 wherein said spin-polarized carriers are holes.

5. The method of claim 2, wherein said spin injection material is a ferromagnetic metal.

6. The method of claim 5, wherein said spin injection material is selected from the group consisting of iron, iron-based alloys, nickel, nickel-based alloys, cobalt and cobalt-based alloys, SmCo, and collosal magnetoresistive materials.

7. The method of claim 6, wherein said spin injection material is selected from the group consisting of iron, iron-based alloys, nickel, nickel-based alloys, cobalt and cobalt-based alloys, SmCo, and LaCaMnO.

8. The method of claim 2, wherein said spin injection material is a layer of a nonmagnetic metal in physical contact with a spin insulator layer, said spin insulator layer being sufficiently thin to allow carriers from said nonmagnetic metal to tunnel into said superconducting material.

9. The method of claim 8, wherein said spin insulator is magnetite.

10. The of claim 8, wherein said nonmagnetic metal is selected from the group consisting of gold, silver, aluminum, and mixtures thereof.

11. The method of claim 5, wherein a nonmagnetic metal buffer layer exists between said spin injection material and said superconducting material, so that said spin-polarized carriers injected from said spin injection material pass through said nonmagnetic buffer layer before reaching said superconducting material.

12. The method of claim 2, wherein said superconducting material is selected from the group consisting of Tl(BaSr)CaCuO superconductors, Hg(BaSr)CaCuO superconductors, BiSrCaCuO superconductors, and NdCeCuO superconductors.

13. Circuitry for suppressing the superconductivity of a superconducting material, comprising:

a layer of a superconducting material having a first terminal and a second terminal opposite said first terminal

a first biasing circuit electrically biasing said first terminal with respect to said second terminal so as to drive a superconducting current along said layer of said superconducting material;

a layer of a spin injection material, capable of producing a spin-polarized current of spin-polarized carriers, in electrical contact with said superconducting material; and

a second biasing circuit electrically biasing said layer of spin injection material with respect to said superconducting material so that a spin-polarized current of said spin-polarized carriers from said spin-injection material is injected into a portion of said superconducting layer between said first and second terminals.

14. The circuitry of claim 13, wherein said spin injection material is a ferromagnetic metal.

15. The circuitry of claim 14, wherein said spin injection material is selected from the group consisting of iron, iron-based alloys, nickel, nickel-based alloys, cobalt and cobalt-based alloys, SmCo, and colossal magnetoresistive materials.

16. The circuitry of claim 15, wherein said spin injection material is selected from the group consisting of iron, iron-based alloys, nickel, nickel-based alloys, cobalt and cobalt-based alloys, SmCo, and LaCaMnO.

17. The circuitry of claim 14, further comprising a buffer layer between said spin injection material and said superconducting material so that said spin-polarized carriers injected from said spin injection material will pass through said buffer layer before reaching said superconducting material, said buffer layer being a non-magnetic metal, a semiconductor, or a semimetal.

18. The circuitry of claim 17, wherein said buffer layer is non-magnetic.

19. The circuitry of claim 18, wherein said nonmagnetic metal is selected from the group consisting of gold, silver, aluminum, and mixtures thereof.

20. The circuitry of claim 18, wherein said buffer layer is a semiconductor or a semimetal.

21. The circuitry of claim 14, further comprising an electrically insulting layer between said spin injection material and said superconducting material, said insulator layer being sufficiently thin to allow spin-polarized carriers from said ferromagnetic metal to tunnel into said superconducting material.

22. The circuitry of claim 13, wherein said spin injection material is a layer of a nonmagnetic metal in physical contact with a spin insulator layer, said spin insulator layer being sufficiently thin to allow carriers from said nonmagnetic metal to tunnel into said superconducting material.

23. The circuitry of claim 22, wherein said spin insulator is magnetite.

24. The circuitry of claim 13, wherein said superconducting material is selected from the group consisting of YBaCuO superconductors, Tl(Ba,Sr)CaCuO superconductors, Hg(BaSr)CaCuO superconductors, BiSrCaCuO superconductors, and NdCeCuO superconductors.