Active superconducting devices formed of thin films

• US 5,019,721 A
• Filed: 08/18/1989
• Issued: 05/28/1991
• Est. Priority Date: 08/18/1989
• Status: Expired due to Fees

• Current Assignee: Wisconsin Alumni Research Foundation (University of Wisconsin System)
• Original Assignee: Wisconsin Alumni Research Foundation (University of Wisconsin System)
• Inventors: Martens, Jon S., Hohenwarter, Gert K. G., Beyer, James B., Nordman, James E.
• Primary Examiner(s): Zazworsky, John
• Application Number:
  US07/395,965
• Time in Patent Office: 648 Days
• Field of Search: 307/245, 307/277, 307/306, 307/476, 357/5, 505/1, 505/832, 505/861, 505/865, 505/874
• US Class Current: 327/527
• CPC Class Codes: H03K 17/92 by the use, as active elements, of superconductive devices
• CPC Class Codes: H03K 3/38 by the use, as active elements, of superconductive devices
• CPC Class Codes: H10N 60/124 comprising high-Tc ceramic materials
• CPC Class Codes: H10N 60/205 having three or more electrodes, e.g. transistor-like structures H10N60/128 takes precedence
• CPC Class Codes: Y10S 505/865 with josephson junction
• CPC Class Codes: Y10S 505/874 with josephson junction, e.g. squid

Abstract

Active superconducting devices are formed of thin films of superconductor which include a main conduction channel which has an active weak link region. The weak link region is composed of an array of links of thin film superconductor spaced from one another by voids and selected in size and thickness such that magnetic flux can propagate across the weak link region when it is superconducting. Magnetic flux applied to the weak link region will propagate across the array of links causing localized loss of superconductivity in the links and changing the effective resistance across the links. The magnetic flux can be applied from a control line formed of a superconducting film deposited coplanar with the main conduction channel and weak link region on a substrate. The devices can be formed of any type to superconductor but are particularly well suited to the high temperature superconductors since the devices can be entirely formed from coplanar films with no overlying regions. The devices can be utilized for a variety of electrical components, including switching circuits, amplifiers, oscillators and modulators, and are well suited to microwave frequency applications.

Claims

1. A controllable active superconducting device comprising:

(a) a main conduction channel formed of a film of superconductor on a substrate;

(b) an active weak link region interposed sin the main conduction channel, the active weak link region composed of a plurality of links formed of a thin film of superconductor separated by non-superconductive voids, the thickness and lateral dimensions of the links selected such that magnetic flux can propagate across the weak link region when it is superconducting;

(c) means for providing a magnetic flux to the active weak link region which can propagate across the weak link region to control the resistance of the weak region.

2. The device of claim 1 wherein the means for providing a magnetic flux comprises a control line formed of a film of superconductor on the substrate coplanar with the main conduction channel and having a portion adjacent to the active weak link region such that current in the control line will impose a magnetic flux on the weak link region.

3. The device of claim 1 wherein the main conduction channel and the weak link region are formed of a superconductor having a superconducting transition temperature above the temperature of liquid helium or liquid hydrogen.

4. The device of claim 3 wherein the superconductor is selected from the group consisting of superconducting compounds of YBaCuO, BiSrCaCuO, and TlCaBaCuO.

5. The device of claim 1 wherein the superconductor forming the main conduction channel and the active weak link region is a metallic superconductor.

6. The device of claim 5 wherein the superconductor is niobium.

7. The device of claim 1 wherein the weak link region is formed of a thin film of superconductor with a series of spaced holes formed in the film in a row, the portions of the superconductor between the holes defining the weak links.

8. The device of claim 4 wherein the thickness of the superconducting film forming the weak links is about 100 nanometers or less.

9. The device of claim 8 wherein the thickness of the superconducting film forming the weak links is in the range of 20 to 100 nanometers.

10. The device of claim 5 wherein the thickness of the superconducting film forming the weak links is about 10 nanometers or less.

11. The device of claim 5 wherein the thickness of the superconducting film forming the weak links is in the range of about 5 to 10 nanometers.

12. The device of claim 1 wherein each weak link has a size in the range of about 5 to 10 microns wide and 5 to 10 microns long.

13. The device of claim 2 wherein the control line is formed with a portion thereof spaced no more than about 15 microns from one end of the weak link region.

14. The device of claim 1 wherein the weak link region comprises an array of weak links spaced from one another in a row in a straight line with voids between them and wherein the means for providing magnetic flux comprises a conducting control line formed coplanar with the main conduction channel and the weak link superconducting film, the control line having a portion which extends to a position adjacent to one end of the row of links such that magnetic flux initiated from current in the control line will propagate along the row of links.

15. The device of claim 14 wherein the control line is formed of a film of a superconducting material.

16. A superconducting amplifying device comprising;

(a) a main conduction channel formed of a film of superconductor on a substrate;

(b) an active weak link region interposed in the main conduction channel, the active weak link region composed of at least one link formed of a thin film of superconductor bounded by non-superconductive voids, the thickness and lateral dimensions of the links selected such that magnetic flux can propagate across the weak link region when it is superconducting;

(c) a control line having a portion adjacent to the active weak link region such that current in the control line will impose a magnetic flux on the weak link region;

(d) means for applying selected biasing current to the main conduction channel when in the superconducting state such that a change in the current applied to the control line will result in a change in the voltage across the weak link region of the main conduction channel.

17. The device of claim 16 wherein the main conduction channel and the weak link region are formed of a superconductor having a superconducting transition temperature above the temperature of liquid helium or liquid hydrogen.

18. The device of claim 17 wherein the superconductor is selected from a group consisting of superconducting compounds of YBaCuO, BiSrCaCuO, TlCaBaCuO.

19. The device of claim 16 wherein the superconductor forming the main conduction channel and the active weak link region is a metallic superconductor.

20. The device of claim 19 wherein the superconductor is niobium.

21. The device of claim 16 wherein the weak link region is formed of a thin film of superconductor with a series of spaced holes formed in the film in a row, the portions of the superconductor between the holes defining the weak links.

22. The device of claim 18 wherein the thickness of the superconducting film forming the weak links is about 100 nanometers or less.

23. The device of claim 18 wherein the thickness of the superconducting film forming the weak links is in the range of 20 to 100 nanometers.

24. The device of claim 19 wherein the thickness of the superconducting film forming the weak links is about 10 nanometers or less.

25. The device of claim 19 wherein the thickness of the superconducting film forming the weak links is in the range of about 5 to 10 nanometers.

26. The device of claim 16 wherein each weak link has a size in the range of about 5 to 10 microns wide and 5 to 10 microns long.

27. The device of claim 16 wherein the control line is formed with a portion thereof no more than about 15 microns from one end of the weak link region.

28. The device of claim 16 wherein the weak link region comprises an array of weak links spaced from one another in a row in a straight line with voids between them.

29. The device of claim 16 further including an impedance matching transformer having its secondary connected to the ends of the control line and having its primary available to be driven by an input signal.

30. The device of claim 16 further including means for feeding the output signal from the main conduction channel back to the control line to cause the output voltage across the weak link region of the main conduction channel to oscillate at a selected frequency.

31. The device of claim 16 further including means for applying a high carrier frequency signal to the main conduction channel across the active weak link region and further comprising means for applying a lower modulating frequency signal to the control line such that the output of the main conduction channel across the active weak link region is the carrier frequency signal phase modulated by the lower frequency signal applied to the control line.

33. The method of claim 21 wherein the step of applying magnetic flux to the weak link region is carried out by running current through a control line positioned adjacent to the weak link region such that the magnetic field from the current flowing in the control line will reach the weak link region and provide flux which will propagate across the weak link region.

32. A method of controlling the electrical quantities in superconducting circuits comprising the steps of:

(a) conducting current through a superconducting path including a main conduction channel formed of a film of superconductor on a substrate and an active weak link region interposed in the main conduction channel, with the active weak link region composed of a plurality of links formed of a thin film of superconductor separated by non-superconducting voids with the thickness and lateral dimensions of the links selected such that magnetic flux can propagate across the weak link region when it is superconducting;

(b) applying magnetic flux to the weak link region and propagating magnetic flux vortices across the weak links in the weak link region to control the resistance of the weak link region to the current flowing therethrough.