Josephson current source systems and method

Patent metadata

Field	Value
Publication number	US-9780765-B2
Application number	US-201414564962-A
Country	US
Kind code	B2
Filing date	Dec 9, 2014
Priority date	Dec 9, 2014
Publication date	Oct 3, 2017
Grant date	Oct 3, 2017

Abstract

One embodiment describes a Josephson current source system. The system includes a flux-shuttle loop that is inductively coupled with an AC input signal. The flux-shuttle loop includes a plurality of Josephson junctions spaced about the flux-shuttle loop and being configured, when activated, to sequentially trigger the plurality of Josephson junctions about the flux-shuttle loop in response to the AC input signal to generate a DC output current provided through an output inductor. The system also includes a flux injector that is configured to selectively activate and deactivate the flux-shuttle loop in response to an input signal to control an amplitude of the DC output current.

First claim

What is claimed is:

1. A Josephson current source system comprising:
a flux-shuttle loop comprising a plurality of Josephson junctions spaced about the flux-shuttle loop and being configured to sequentially trigger the plurality of Josephson junctions about the flux-shuttle loop, in response to an inductively-coupled AC input signal, to generate a DC output current provided through an output inductor; and
a flux injector coupled to said flux-shuttle loop and configured to selectively activate and deactivate the flux-shuttle loop to control an amplitude of the DC output current.

2. The system of claim 1 , wherein the flux injector is configured to activate the flux-shuttle loop to initiate sequential triggering of the plurality of Josephson junctions about the flux-shuttle loop in response to a single-flux quantum (SFQ) pulse, and is configured to deactivate the flux-shuttle loop in response to reciprocal SFQ pulse.

3. The system of claim 1 , wherein flux-shuttle loop comprises a superconducting quantum interference device (SQUID) comprising a flux state corresponding to one of activation and deactivation of the flux-shuttle loop, and wherein the flux injector is configured to change the flux state in response to an input signal to one of activate and deactivate the flux-shuttle loop.

4. The system of claim 3 , wherein the SQUID comprises a SQUID Josephson junction that forms part of the flux-shuttle loop, and wherein the flux injector further comprises a transformer comprising a first inductor configured to propagate a DC bias current, a second inductor that is magnetically coupled with the first inductor and is configured to propagate the input signal, and a third inductor that is magnetically coupled with the first and second inductors and which forms part of the SQUID, such that the SQUID Josephson junction triggers in response to the input signal to activate and deactivate the flux-shuttle loop.

5. The system of claim 4 , wherein the flux-shuttle loop comprises a plurality of stages that are each associated with a respective phase of the AC input signal, wherein each of the plurality of stages comprises a storage inductor interconnecting the respective one of the plurality of stages with the output inductor and being configured to provide a voltage pulse to the output inductor to increase the DC output current in response to the sequential triggering of the plurality of Josephson junctions, wherein one of the plurality of stages comprises the flux injector, such that the third inductor is configured as the storage inductor associated with the respective one of the plurality of stages.

6. The system of claim 1 , wherein the AC input signal comprises an in-phase AC input signal and a quadrature-phase AC input signal.

7. The system of claim 6 , wherein the flux-shuttle loop further comprises a plurality of transformers configured to inductively couple the flux-shuttle loop with each of the in-phase AC input signal and the quadrature-phase AC input signal, wherein the in-phase AC input signal is provided through a primary winding of a first portion of the plurality of transformers to induce a bias current in a secondary winding of the first portion of the plurality of transformers, and wherein the quadrature-phase AC input signal is provided through a primary winding of a second portion of the plurality of transformers to induce a bias current in a secondary winding of the second portion of the plurality of transformers to facilitate the sequential triggering of the plurality of Josephson junctions.

8. The system of claim 1 , wherein the flux-shuttle loop comprises a plurality of stages, wherein the flux injector is configured as one of the plurality of stages, each of the plurality of stages comprising:
a transformer configured to generate a bias current based on inductive coupling of the AC input signal;
a Josephson junction configured to trigger to generate a voltage pulse in response to the bias current; and
a storage inductor interconnecting the respective one of the plurality of stages with the output inductor and being configured to provide the voltage pulse to the output inductor.

9. The system of claim 1 , wherein the flux injector is a first flux injector that is configured to selectively activate and deactivate the flux-shuttle loop in response to a first input signal to selectively increase the amplitude of the DC output current based on sequential triggering of the plurality of Josephson junctions about the flux-shuttle loop when the flux-shuttle loop is activated by the first flux injector, the system further comprising a second flux injector that is configured to selectively activate and deactivate the flux-shuttle loop in response to a second input signal to selectively decrease the amplitude of the DC output current based on sequential triggering of the plurality of Josephson junctions about the flux-shuttle loop when the flux-shuttle loop is activated by the second flux injector.

10. A superconducting current source comprising the Josephson current source system of claim 1 , wherein the Josephson current source system is configured to increase the amplitude of the DC output current in response to activation of the flux-shuttle loop, the superconducting current source further comprising:
a controller configured to set the amplitude of the DC output current in response to a programmable current register and to generate a first input signal and a second input signal, the first input signal being provided to the flux injector to activate the flux-shuttle loop; and
a second Josephson current source system comprising:
a second flux-shuttle loop comprising a second plurality of Josephson junctions spaced about the second flux-shuttle loop and being configured, when activated, to sequentially trigger the second plurality of Josephson junctions about the second flux-shuttle loop in response to the inductively-coupled AC input signal to decrease the DC output current provided through the output inductor; and
a second flux injector that is configured to selectively activate and deactivate the second flux-shuttle loop in response to the second input signal.

11. A superconducting circuit system comprising a plurality of the Josephson current source system of claim 1 , the plurality of Josephson current source systems being configured to generate a respective plurality of DC output currents.

12. A method for controlling an amplitude of a DC output current, the method comprising:
providing a first single-flux quantum (SFQ) pulse to a first flux injector coupled to at least one flux-shuttle loop to generate a first fluxon that propagates around the at least one flux-shuttle loop via sequential triggering of a plurality of Josephson junctions based on an AC input signal to increase the amplitude of the DC output current in an output inductor coupled to the at least one flux-shuttle loop;
providing a first reciprocal SFQ pulse to the first flux injector to generate a first anti-fluxon that substantially cancels the first fluxon to maintain the amplitude of the DC output current;
providing a second SFQ pulse to a second flux injector coupled to the at least one flux-shuttle loop to generate a second fluxon that propagates around the at least one flux-shuttle loop via sequential triggering of the plurality of Josephson junctions based on the AC input signal to decrease the amplitude of the DC output current in the output inductor; and
providing a second reciprocal SFQ pulse to the second flux injector to generate a second anti-fluxon that substantially cancels the second fluxon to maintain the amplitude of the DC output current.

13. The method of claim 12 , fu

Assignees

• Naaman Ofer
• Herr Quentin P
• Northrop Grumman Systems Corp

Inventors

• Naaman Ofer
• Herr Quentin P

Classifications

• H03K3/38 Primary

  by the use, as active elements, of superconductive devices · CPC title

• H01L39/223

  Electricity · mapped topic

• G06N99/002

  Physics · mapped topic

• H10N60/12

  Josephson-effect devices · CPC title