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 require sensitive amplification, leading to noise and local heating due to the need for resistors near the measure island.

Innovation Solution

The method involves supplying a bias current through a Josephson junction, measuring the output voltage, and updating the critical current using a shunt resistor in response to changes in charge on coupled islands, allowing for rapid, single-shot charge sensing.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If conventional FET with measure island is used for charge sensing, then measurement accuracy can be achieved, but measurement speed is slow (microseconds) and requires sensitive amplification with resistors causing noise and heating

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

Solution Approach 1:

The patent replaces the conventional FET-based charge sensing mechanism with a Josephson junction-based single-electron transistor (SET). This substitution leverages quantum mechanical effects (Cooper pair tunneling, Josephson effect) to achieve charge sensing without requiring the bulky resistor-amplifier configuration of conventional FETs. The SET operates at quantum scales, enabling both high-speed operation and high sensitivity without the trade-off present in conventional systems.

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

Solution Approach 2:

The patent changes the operating parameters by using a bias current less than the critical current of the Josephson junction, enabling the device to operate in a superconducting state. This parameter change allows the SET to detect single-electron tunneling events through voltage pulses, achieving both high measurement precision and high speed (nanosecond timescale) without the noise and heating issues of conventional resistive amplification.

Inventive Principle:
Principle #35Parameter changes

2Measurement precision

If multiple samples of measure island current response are taken for accurate measurement, then measurement accuracy improves, but measurement time increases to microseconds

Engineering Contradiction:
Improvecharge occupancy measurement accuracyVSAvoidmeasurement time
Core Design Contradiction:
Measurement precisionVSLoss of time

Solution Approach 1:

The patent employs preliminary action by pre-biasing the Josephson junction with a current slightly below its critical current. This preparation allows the system to immediately respond to single-electron tunneling events with detectable voltage pulses, eliminating the need for time-consuming multiple sampling and integration processes required by conventional FET-based charge sensors.

Inventive Principle:
Principle #10Preliminary action

Solution Approach 2:

The patent skips the slow integration and multiple-sampling process by using the Josephson junction's inherent quantum response. When a single electron tunnels through the island, it causes an immediate, detectable change in the voltage across the junction. This allows the system to rush through the measurement process in nanoseconds, achieving both speed and accuracy simultaneously.

Inventive Principle:
Principle #21Skipping (Rushing through)

3Measurement precision

If resistors are placed near the measure island for signal amplification, then measurement sensitivity improves, but local heating and noise generation increase

Engineering Contradiction:
Improvecharge state detection sensitivityVSAvoidnoise and heating
Core Design Contradiction:
Measurement precisionVSObject-generated harmful factors

Solution Approach 1:

The patent substitutes the resistor-based amplification mechanism with a Josephson junction-based detection mechanism. The SET converts charge state changes directly into voltage pulses through quantum tunneling effects, eliminating the need for resistive amplification. This substitution removes the source of thermal noise and heating that plagues conventional charge sensing, while maintaining high measurement sensitivity.

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

Solution Approach 2:

The patent exploits the phase transition between superconducting and normal states in the Josephson junction. When charge on the island changes, it modulates the critical current, causing the junction to transition between states and produce detectable voltage pulses. This phase transition mechanism provides inherent signal amplification without requiring external resistors, thus avoiding the associated noise and heating problems.

Inventive Principle:
Principle #36Phase transitions

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 approach enables high-speed, accurate measurements of localized charge states in quantum systems, reducing measurement time to nanoseconds and minimizing noise and heating issues.

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

Implementation Method 2

Updating, using a shunt resistor coupled across the Josephson junction, the critical current of the Josephson junction to a second value responsive to the change in charge

Methodology Applied
Scientific EffectJoule heating: Joule Heating

Data Source

PatentUS20250124321A1Josephson junction-based charge sensing in quantum systems
Publication Date: 2025.04.17 THE BOEING CO
  • US20250124321A1 patent drawing
  • US20250124321A1 patent drawing
  • US20250124321A1 patent drawing

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.