Flux Qubit XX Coupler for Pure Tunable X-Basis Coupling

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Solution Overview

Problem

Current quantum computing technologies face challenges in effectively coupling X basis states of flux qubits, particularly in achieving high-fidelity XX interactions without introducing unwanted single qubit effects or coupling along other axes, which limits their application in quantum annealing and noise suppression schemes.

Innovation Solution

A quantum circuit assembly utilizing an XX coupler with tunable Josephson junctions and control mechanisms to create specific tunneling paths between energy minima, allowing for adjustable XX interactions while suppressing ZZ and YY couplings, enabling coupling of degenerate energy states and achieving high coupling strengths up to two gigahertz.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If conventional coupling methods are used for flux qubits, then coupling between qubits can be achieved, but unwanted single qubit effects and coupling along other axes (ZZ and YY) are introduced, reducing interaction fidelity

Engineering Contradiction:
Improveinteraction fidelityVSAvoidunwanted single qubit effects and off-axis coupling
Core Design Contradiction:
ReliabilityVSObject-generated harmful factors

Solution Approach 1:

The patent introduces a coupler circuit as an intermediary element between two flux qubits. This coupler contains a nonlinear Josephson element that mediates the interaction between qubits, enabling selective XX coupling while suppressing unwanted ZZ and YY couplings. The intermediary structure allows controlled quantum interaction without direct qubit-to-qubit coupling that would generate harmful effects.

Inventive Principle:
Principle #24Intermediary (Mediator)

Solution Approach 2:

The patent employs tunable Josephson junctions within the coupler circuit that allow dynamic adjustment of coupling parameters. By changing the Josephson energy of the coupler element, the system can selectively enhance XX coupling while suppressing other interaction channels. This parameter control enables high-fidelity interactions by optimizing coupling strength and selectivity.

Inventive Principle:
Principle #35Parameter changes

2Reliability

If tunable Josephson junctions are added to achieve selective XX coupling, then coupling selectivity and fidelity improve, but device complexity increases

Engineering Contradiction:
Improvecoupling selectivityVSAvoidnumber of Josephson junctions and control mechanisms
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The coupler circuit is designed to perform multiple functions: it mediates XX coupling between qubits, provides tunability through Josephson junctions, and suppresses unwanted interaction channels. This multi-functional design consolidates several requirements into a single circuit element, reducing overall system complexity despite the presence of tunable elements.

Inventive Principle:
Principle #6Universality (Multi-functionality)

Solution Approach 2:

The patent uses dynamically tunable Josephson junctions that can adjust their coupling strength in real-time. This dynamic capability allows the system to optimize performance for different operating conditions without requiring multiple static circuit configurations, thereby managing complexity through adaptability rather than proliferation of components.

Inventive Principle:
Principle #15Dynamics

3Productivity

If high coupling strengths are achieved through the XX coupler, then quantum gate performance improves, but controlling the coupling to be purely XX without ZZ and YY components becomes more difficult

Engineering Contradiction:
Improvequantum gate performanceVSAvoidcoupling axis purity
Core Design Contradiction:
ProductivityVSManufacturing precision

Solution Approach 1:

The coupler circuit introduces asymmetry through the nonlinear Josephson element, which breaks the symmetry between different coupling channels. This asymmetric design inherently suppresses ZZ and YY coupling while enhancing XX coupling, allowing high coupling strength to be achieved with maintained axis purity. The asymmetric potential landscape created by the Josephson element selectively favors the desired interaction channel.

Inventive Principle:
Principle #4Asymmetry

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

The solution enables efficient XX coupling between flux qubits, allowing for non-stoquastic Hamiltonian generation and passive noise suppression, with tunable coupling strengths and the ability to maintain pure XX interactions, enhancing the performance of quantum logic gates and noise resilience.

Implementation Method 1

A quantum circuit assembly comprising a first flux qubit, a second flux qubit, and an XX coupler operatively coupling the first flux qubit to the second flux qubit. The XX coupler comprises a plurality of Josephson junctions, with at least one being tunable.

Methodology Applied
Scientific EffectJosephson effect: Josephson Effect

Data Source

PatentEP3583554B1Xx coupler for flux qubits
Publication Date: 2024.03.20 NORTHROP GRUMMAN SYSTEMS CORP
  • EP3583554B1 patent drawingFigure 1~2
  • EP3583554B1 patent drawingFigure 3~5
  • EP3583554B1 patent drawingFigure 4

AI summary

Systems and methods are provided for coupling two flux qubits. A quantum circuit assembly includes a first flux qubit, having at least two potential energy minima, and a second flux qubit, having at least two potential energy minima. A system formed by the first and second qubits has at least four potential energy minima prior to coupling, each of the four potential energy minima containing at least one eigenstate of a system comprising the first flux qubit and the second flux qubit. A coupler creates a first tunneling path between a first potential energy minimum of the system and a second potential energy minimum of the system, and a second tunneling path between a third potential energy minimum of the system and a fourth potential energy minimum of the system. The coupler creates the first and second tunneling paths between potential energy minima representing states of equal bit parity.