Josephson Junction Charge Sensing for Fast Low-Noise Quantum Readout

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Solution Overview

Problem

Existing methods for measuring localized charge states in quantum systems are slow and prone to noise, requiring multiple samples and sensitive amplification, which can cause local heating and noise generation.

Innovation Solution

Utilizing Josephson junctions with bias currents below critical current levels to measure voltage drops caused by charge changes in quantum dots, coupled through capacitors with varying capacitances, and employing shunt resistors to update critical currents.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If conventional FET-based charge sensing is used, then charge occupancy can be measured, but measurement speed is slow (microseconds) and requires multiple samples

Engineering Contradiction:
Improvecharge occupancy measurement accuracyVSAvoidmeasurement speed
Core Design Contradiction:
Measurement precisionVSProductivity

Solution Approach 1:

The patent changes the operating parameters by using a Josephson junction instead of a conventional FET, operating at cryogenic temperatures with bias currents below the critical current. This parameter change enables single-shot charge sensing with nanosecond response time, resolving the contradiction between measurement precision and productivity

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent replaces the conventional FET electrical measurement system with a quantum-based Josephson junction system. The Josephson junction's quantum tunneling properties provide inherently faster response and higher sensitivity, eliminating the need for slow integration and multiple sampling while maintaining or improving measurement accuracy

Inventive Principle:
Principle #28Mechanics substitution (Replace mechanical system)

2Measurement precision

If sensitive amplification is used to improve measurement accuracy, then charge occupancy can be measured accurately, but local heating and noise generation increase

Engineering Contradiction:
Improvecharge occupancy measurement accuracyVSAvoidlocal heating and noise
Core Design Contradiction:
Measurement precisionVSObject-affected harmful factors

Solution Approach 1:

The Josephson junction acts as an intermediary between the charge island and the measurement system. It transduces charge information into voltage signals through quantum tunneling effects, providing inherent signal amplification without requiring external sensitive amplifiers that would generate heat and noise

Inventive Principle:
Principle #24Intermediary (Mediator)

Solution Approach 2:

The patent replaces the need for sensitive external amplification hardware with a quantum-based measurement mechanism. The Josephson junction's intrinsic quantum properties provide the necessary signal sensitivity directly at the quantum device level, eliminating the harmful effects of external amplification equipment

Inventive Principle:
Principle #28Mechanics substitution (Replace mechanical system)

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

Enables rapid, single-shot charge sensing with high accuracy, reducing measurement time to nanoseconds and minimizing noise and heating effects.

Implementation Method 1

supplying a bias current through a Josephson junction, the bias current less than a first value of a critical current of the Josephson junction

Methodology Applied
Scientific EffectJosephson effect: Josephson Effect

Data Source

PatentEP4538722B1Josephson junction-based charge sensing in quantum systems
Publication Date: 2026.02.18 THE BOEING CO
  • EP4538722B1 patent drawingFigure 1~2
  • EP4538722B1 patent drawingFigure 3
  • EP4538722B1 patent drawingFigure 4~5

AI summary

The present disclosure provides a method of charge sensing in a quantum system. The method includes supplying a bias current through a Josephson junction. The bias current is less than a first value of a critical current of the Josephson junction. The method further includes measuring an output voltage of the Josephson junction. Responsive to a change in charge of one or more charge islands coupled to the Josephson junction, the critical current is reduced to a second value less than the bias current, causing a voltage drop across the Josephson junction.