Superconducting circuits based devices and methods

US10411713B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10411713-B2
Application numberUS-201715424832-A
CountryUS
Kind codeB2
Filing dateFeb 4, 2017
Priority dateFeb 4, 2017
Publication dateSep 10, 2019
Grant dateSep 10, 2019

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  1. Title

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  2. Abstract

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  3. Assignees and inventors

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  4. Key dates

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  5. First independent claim

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  6. CPC / IPC classifications

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  7. Citations and related patents

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Abstract

Official abstract text for this publication.

Superconducting circuits based devices and methods, including reciprocal quantum logic (RQL) based devices and methods are provided. In one example, a device comprising an output terminal, a first input terminal for receiving a first set of pulses, and a second input terminal for receiving a second set of pulses is provided. The first section may be configured to pass a single pulse received during a single clock cycle at any of the first input terminal or the second input terminal, but to not pass two or more positive pulses received during a single clock cycle at the first input terminal and the second input terminal. The second section, coupled to the first section, may be configured to, in response to the single pulse, generate a negative pulse after a predetermined fraction of a single clock cycle after providing a positive pulse at the output terminal.

First claim

Opening claim text (preview).

The invention claimed is: 1. A device comprising: an output terminal; a first input terminal for receiving a first set of pulses; a second input terminal for receiving a second set of pulses; a first section configured to pass a single pulse received during a single clock cycle at any of the first input terminal or the second input terminal, but to not pass two or more positive pulses received during a single clock cycle at the first input terminal and the second input terminal, wherein the first section comprises an unpowered stage comprising: (1) a first unpowered Josephson junction coupled between the first input terminal and a second terminal, and (2) a second unpowered Josephson junction coupled between the second input terminal and the second terminal, and wherein the unpowered stage is configured to pass pulses traveling in a first direction, wherein the first direction comprises a direction of travel of any pulses from any of the first input terminal or the second input terminal toward the output terminal and block pulses traveling in a second direction, opposite to the first direction; and a second section, coupled to the first section, wherein the second section is configured to, in response to the single pulse, generate a negative pulse after a predetermined fraction of a single clock cycle after providing a positive pulse at the output terminal. 2. The device of claim 1 , wherein the first section further comprises a central junction coupled between the second terminal and a third terminal, wherein the central junction is configured to pass a single pulse, received during a single clock cycle, but block two or more pulses, received during a single clock cycle. 3. The device of claim 2 , wherein the second section comprises a Josephson transmission line (JTL) network coupled between the third terminal and the output terminal, wherein the JTL network is configured to generate the negative pulse after the predetermined fraction of the single clock cycle after providing the positive pulse at the output terminal. 4. The device of claim 3 , wherein the predetermined fraction of the single clock cycle comprises one half of the single clock cycle. 5. The device of claim 3 , wherein the JTL network is configured to generate the negative pulse via a connection to ground. 6. The device of claim 3 , wherein each of the central junction and the JTL network is configured to receive a bias current from an alternating current (AC) clock. 7. The device of claim 2 , wherein the second section comprises an inductor coupled between the output terminal and a ground terminal. 8. The device of claim 1 , wherein each of the first set of the pulses and the second set of the pulses comprises single-flux quantum (SFQ) pulses, and wherein each of the SFQ pulses comprises one of a positive SFQ pulse or a negative SFQ pulse. 9. The device of claim 1 , wherein the device is configured to operate as one of an exclusive OR logic gate or an inverter. 10. The device of claim 1 , wherein the first section comprises a first stage comprising: (1) a first inductor coupled between the first input terminal and a second terminal, and (2) a second inductor coupled between the second input terminal and the second terminal. 11. The device of claim 10 , wherein the second section comprises an inductor coupled between the output terminal and a ground terminal. 12. A method of operating a device comprising a first input terminal for receiving a first set of pulses, a second input terminal for receiving a second set of pulses, and an output terminal, the method comprising: passing a single pulse received during a single clock cycle at any of the first input terminal or the second input terminal, but not passing two or more positive pulses received during a single clock cycle at the first input terminal and the second input terminal; passing pulses traveling in a first direction, wherein the first direction comprises a direction of travel of any pulses from any of the first input terminal or the second input terminal toward the output terminal and blocking pulses traveling in a second direction, opposite to the first direction; and in response to the single pulse, generating a negative pulse after a predetermined fraction of a single clock cycle after providing a positive pulse at the output terminal. 13. The method of claim 12 , wherein the predetermined fraction of the single clock cycle comprises one half of the single clock cycle. 14. An exclusive OR (XOR) logic gate comprising: an output terminal; a first input terminal for receiving a first set of pulses; a second input terminal for receiving a second set of pulses; an unpowered stage comprising: (1) a first unpowered Josephson junction coupled between the first input terminal and a second terminal, and (2) a second unpowered Josephson junction coupled between the second input terminal and the second terminal, wherein the unpowered stage is configured to pass pulses traveling in a first direction, wherein the first direction comprises a direction of travel of any pulses from any of the first input terminal or the second input terminal toward the output terminal and block pulses traveling in a second direction, opposite to the first direction; a central junction coupled between the second terminal and a third terminal, wherein the central junction is configured to pass a single pulse, received during a single clock cycle, but block two or more pulses, received during a single clock cycle; and a Josephson transmission line (JTL) network coupled between the third terminal and the output terminal, wherein the JTL network is configured to generate the negative pulse after the predetermined fraction of the single clock cycle after providing the positive pulse at the output terminal. 15. The XOR logic gate of claim 14 , wherein the predetermined fraction of the single clock cycle comprises one half of the single clock cycle. 16. The XOR logic gate of claim 14 , wherein each of the first set of the pulses and the second set of the pulses comprises single-flux quantum (SFQ) pulses, and wherein each of the SFQ pulses comprises one of a positive SFQ pulse or a negative SFQ pulse. 17. The XOR logic gate of claim 14 , wherein the JTL network is configured to generate the negative pulse via a connection to ground. 18. The XOR logic gate of claim 14 , wherein each of the central junction and the JTL network is configured to receive a bias current from an alternating current (AC) clock.

Assignees

Inventors

Classifications

  • EXCLUSIVE-OR circuits, i.e. giving output if input signal exists at only one input; COINCIDENCE circuits, i.e. giving output only if all input signals are identical · CPC title

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

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

  • H03K19/195Primary

    using superconductive devices · CPC title

  • Quantum computing, i.e. information processing based on quantum-mechanical phenomena · CPC title

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What does patent US10411713B2 cover?
Superconducting circuits based devices and methods, including reciprocal quantum logic (RQL) based devices and methods are provided. In one example, a device comprising an output terminal, a first input terminal for receiving a first set of pulses, and a second input terminal for receiving a second set of pulses is provided. The first section may be configured to pass a single pulse received du…
Who is the assignee on this patent?
Microsoft Technology Licensing Llc
What technology area does this patent fall under?
Primary CPC classification H03K19/195. Mapped technology areas include Electricity.
When was this patent published?
Publication date Tue Sep 10 2019 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 2 related publications on this page (citations in our corpus or others sharing the same primary CPC).