Quantum Enhanced Magneto-Optical Microscopy Squeezed States

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Solution Overview

Problem

Magneto-optical sensors face limitations in measurement sensitivity due to the photon shot noise limit, which can be exacerbated by increasing laser power, leading to potential sample damage or heating issues, and extended measurement times that suppress transient responses.

Innovation Solution

A nonlinear interferometer system incorporating an optical parametric amplifier and dual homodyne detection modules to generate and characterize squeezed joint states, allowing for improved sensitivity in magneto-optical measurements while maintaining low laser power and reducing sample heating.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If laser power is increased to improve measurement sensitivity, then measurement sensitivity is improved, but sample damage or heating occurs

Engineering Contradiction:
Improvemeasurement sensitivityVSAvoidsample damage or heating
Core Design Contradiction:
Measurement precisionVSObject-affected harmful factors

Solution Approach 1:

The patent changes the fundamental parameter of light statistics from classical Poissonian statistics to quantum sub-Poissonian statistics using squeezed vacuum states. This parameter change in the quantum regime allows achieving higher measurement sensitivity without increasing laser power, thereby avoiding sample damage and heating while maintaining low optical power operation

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent replaces the classical mechanical approach of increasing laser power with a quantum optical approach using squeezed vacuum states and homodyne detection. This substitution transitions from a classical intensity-based measurement system to a quantum phase-based measurement system, enabling sensitivity improvement without the harmful side effects of high power

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

2Measurement precision

If readout time is increased to improve measurement sensitivity, then measurement sensitivity is improved, but transient responses are suppressed

Engineering Contradiction:
Improvemeasurement sensitivityVSAvoidmeasurement time
Core Design Contradiction:
Measurement precisionVSLoss of time

Solution Approach 1:

The patent changes the measurement regime from classical shot-noise-limited detection to quantum-enhanced detection using squeezed states. This parameter change in the detection mechanism enables achieving high measurement sensitivity with reduced integration time, allowing transient responses to be captured before they are suppressed by long averaging times

Inventive Principle:
Principle #35Parameter changes

3Measurement precision

If laser power is increased to improve measurement sensitivity, then measurement sensitivity is improved, but unwanted heating in low temperature measurement occurs

Engineering Contradiction:
Improvemeasurement sensitivityVSAvoidsample temperature
Core Design Contradiction:
Measurement precisionVSTemperature

Solution Approach 1:

The patent transitions the measurement system to operate in the quantum regime using squeezed vacuum states, changing the fundamental parameter of light statistics. This enables achieving high measurement sensitivity with minimal laser power, preventing unwanted heating in low temperature measurements such as those performed in cryostats where quantum measurements are nearly impossible with classical approaches

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent substitutes the classical high-power heating-based measurement approach with a quantum low-power phase-based measurement approach. This substitution replaces intensity modulation with phase modulation detected through homodyne detection, enabling temperature-sensitive measurements without thermal interference

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

The system achieves enhanced sensitivity, reaching 10 nrad/√Hz with minimal optical power, enabling precise measurements without damaging the sample and maintaining low temperatures, thus overcoming the limitations of classical magneto-optical sensors.

Implementation Method 1

an optical parametric amplifier to generate a squeezed joint state where at least one interacts with a sample of interest

Methodology Applied
Scientific EffectOptical parametric amplification:

Implementation Method 2

generate a squeezed joint state where at least one interacts with a sample of interest

Methodology Applied
Scientific EffectSqueezed state generation:

Implementation Method 3

The sample imparts a Faraday polarization rotation or a Kerr polarization rotation to the light that interacts with the sample

Methodology Applied
Scientific EffectFaraday effect: Faraday Effect

Implementation Method 4

The sample imparts a Faraday polarization rotation or a Kerr polarization rotation to the light that interacts with the sample

Methodology Applied
Scientific EffectKerr effect: Kerr Effect

Implementation Method 5

The optical transduction module is configured to imparts to the interacted light an optical phase shift that is a 1:1 transduction of the polarization rotation caused by the sample on the light

Methodology Applied
Scientific EffectPolarization to phase transduction:

Implementation Method 6

dual homodyne detection modules are used to characterize a magneto-optical response of the sample

Methodology Applied
Scientific EffectHomodyne detection: Homodyne Detection

Data Source

PatentUS11953432B2Quantum enhanced magneto-optical microscopy and spectroscopy
Publication Date: 2024.04.09 UT BATTELLE LLC
  • US11953432B2 patent drawing
  • US11953432B2 patent drawing
  • US11953432B2 patent drawing

AI summary

A system comprising a nonlinear medium (NLM), an optical transduction module, a dual homodyne detector and a processor is provided. The NLM receives at least a pump beam and issues the pump, probe and conjugate beams, where the beams are linearly polarized. Optics route the probe, the conjugate or both beams to the sample. The sample imparts polarization rotation to light that interacts therewith. The optical transduction module imparts to the interacted light an optical phase shift that is a 1:1 transduction of the polarization rotation, where at least one of the probe light or the conjugate light carries the imparted optical phase shift. The processor obtains the optical-phase shift based on respective detection signals from the dual homodyne detector and determines, based on the obtained optical-phase shift, at least one of a Faraday polarization rotation, a Kerr polarization rotation or a spin noise spectrum.