Flux Qubit Coupler Using Equal-Parity Tunneling Paths

Resolve Bottlenecks,
Find Innovative Solutions
Generate Solutions

Solution Overview

Problem

Current quantum computing technologies face challenges in effectively coupling X basis states of flux qubits, which limits the ability to generate non-stoquastic Hamiltonians and efficient quantum logic gates, particularly in achieving high-purity XX interactions without introducing single qubit effects or coupling along other axes.

Innovation Solution

A quantum circuit assembly with tunable Josephson junctions creates specific tunneling paths between potential energy minima representing states of equal bit parity, allowing for controlled XX coupling between flux qubits, enabling the alignment of quantum states along the X-axis and adjustable interaction strengths.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If conventional coupling methods are used to couple flux qubits, then qubit coupling is achieved, but single qubit effects and coupling along other axes are introduced, reducing interaction purity

Engineering Contradiction:
Improvecoupling purityVSAvoidsingle qubit effects
Core Design Contradiction:
ReliabilityVSObject-generated harmful factors

Solution Approach 1:

A coupler consisting of two Josephson junctions is introduced as an intermediary element between the two flux qubits. This coupler mediates the interaction by creating a four-state system with specific potential energy minima, enabling XX coupling while filtering out unwanted single qubit effects and other-axis couplings. The coupler acts as a selective mediator that only permits the desired XX interaction channel.

Inventive Principle:
Principle #24Intermediary (Mediator)

2Adaptability or versatility

If standard quantum computing architectures are used, then basic quantum operations are possible, but generation of non-stoquastic Hamiltonians and efficient quantum logic gates is limited

Engineering Contradiction:
ImproveHamiltonian generation capabilityVSAvoidcircuit architecture complexity
Core Design Contradiction:
Adaptability or versatilityVSDevice complexity

Solution Approach 1:

The system employs dynamic control of the coupler's Josephson junctions to enable generation of non-stoquastic Hamiltonians. By dynamically adjusting the coupling strength and phase relationships in the coupler, the system can generate diverse interaction types (XX, YY, ZZ couplings) and implement efficient quantum logic gates without requiring complex static circuit architectures.

Inventive Principle:
Principle #15Dynamics

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

This solution enables efficient XX coupling between flux qubits, facilitating faster problem-solving capabilities and allowing for the generation of non-stoquastic Hamiltonians and quantum logic gates, while maintaining control over coupling strengths and avoiding single qubit effects.

Implementation Method 1

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

Methodology Applied
Scientific EffectQuantum tunneling:

Implementation Method 2

A quantum circuit assembly with tunable Josephson junctions creates specific tunneling paths between potential energy minima representing states of equal bit parity

Methodology Applied
Scientific EffectJosephson effect: Josephson Effect

Data Source

PatentUS10650323B2XX coupler for flux qubits
Publication Date: 2020.05.12 NORTHROP GRUMMAN SYSTEMS CORP
  • US10650323B2 patent drawing
  • US10650323B2 patent drawing
  • US10650323B2 patent drawing

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.