Optical Source Characterization Using Fixed Fabry-Perot Standards

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Solution Overview

Problem

Existing methods for characterizing optical sources, such as wavelength measurement, are either expensive due to the need for costly materials like InGaAs or PbSe for wavelengths beyond 1100 nm, or slow due to mechanical movement in tunable Fabry-Perot configurations, limiting their robustness and efficiency.

Innovation Solution

A method and device using a system with multiple Fabry-Perot standards without moving parts, where each sensor includes a photodiode and a Fabry-Perot with a transmission curve, forming an overall transmission curve to select wavelengths within a spectral zone, allowing for faster and more economical characterization by eliminating values outside the spectral zone interval using a least squares method.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Adaptability or versatility

If photodiode arrays are used for wavelength exploration, then measurement coverage is improved, but cost increases significantly

Engineering Contradiction:
Improvemeasurement coverageVSAvoidcost
Core Design Contradiction:
Adaptability or versatilityVSEase of manufacture

Solution Approach 1:

The spectral exploration function is segmented across multiple fixed Fabry-Perot interferometers, each tuned to a specific wavelength range. Instead of using a single expensive photodiode array that covers the entire spectrum, the system divides the spectral measurement task into multiple specialized interferometers operating at fixed wavelengths, reducing the need for expensive broadband detection materials.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

Fixed Fabry-Perot interferometers serve as intermediary devices between the optical source and the photodiode detectors. These interferometers filter and select specific wavelength components before they reach the photodiodes, enabling the use of simpler, less expensive photodiode materials while maintaining comprehensive spectral coverage through multiple intermediate filtering stages.

Inventive Principle:
Principle #24Intermediary (Mediator)

2Measurement precision

If tunable Fabry-Perot with moving parts is used, then measurement precision is improved, but measurement speed decreases

Engineering Contradiction:
Improvewavelength measurement precisionVSAvoidmeasurement speed
Core Design Contradiction:
Measurement precisionVSProductivity

Solution Approach 1:

Instead of using a single tunable Fabry-Perot interferometer with moving parts that scans through wavelengths sequentially, the invention inverts the approach by using multiple fixed Fabry-Perot interferometers with predetermined wavelengths. This eliminates the need for mechanical scanning while maintaining the ability to measure across a broad spectral range, thereby improving measurement speed without sacrificing precision.

Inventive Principle:
Principle #13The other way round (Inversion)

Solution Approach 2:

The mechanical scanning system of a tunable Fabry-Perot interferometer is replaced with a static array of multiple fixed Fabry-Perot interferometers. This substitution eliminates moving mechanical parts, removing the speed limitation imposed by sequential scanning while preserving the high precision wavelength measurement capability through parallel detection at multiple fixed wavelength points.

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

3Ease of manufacture

If silicon photodiodes are used, then cost is reduced, but wavelength measurement capability is limited to below 1100 nm

Engineering Contradiction:
ImprovecostVSAvoidwavelength range
Core Design Contradiction:
Ease of manufactureVSAdaptability or versatility

Solution Approach 1:

The wavelength measurement task is segmented into multiple fixed spectral bands, each handled by a dedicated Fabry-Perot interferometer. This segmentation allows the use of silicon photodiodes for each band, as each interferometer filters the incoming light to only the specific wavelength range that silicon can detect, effectively extending the overall system's wavelength capability beyond what a single silicon photodiode could achieve alone.

Inventive Principle:
Principle #1Segmentation

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 faster and more economical characterization of optical sources by eliminating the need for expensive materials and mechanical movement, achieving high precision and speed in wavelength measurement.

Implementation Method 1

each sensor (4) comprising a Fabry Perot standard (5) followed by a photodiode (6), each Fabry Perot standard having a transmission curve of the intensity of the first radiation, as a function of the wavelength of the first radiation

Methodology Applied
Scientific EffectFabry-Perot interference: Fabry-Perot Interferometer

Implementation Method 2

each sensor (4) comprising a Fabry Perot standard (5) followed by a photodiode (6)

Methodology Applied
Scientific EffectPhotoelectric effect: Photoelectric Effect

Data Source

PatentEP3485248B1Process and device for characterising an optical source
Publication Date: 2023.01.18 BLUE IND & SCI
  • EP3485248B1 patent drawingFigure 1~2
  • EP3485248B1 patent drawingFigure 3~6
  • EP3485248B1 patent drawingFigure 7~9

AI summary

The present invention relates to a process for characterising an optical source (1) comprising a fixed cavity (2) having a free spectral range, said process comprising: - generating a first radiation (3); receiving at least a portion of this first radiation by at least one sensor (4); measuring a signal by each sensor and for each scanned state of the source; on the basis of the signals measured, and for each scanned state of the source, calculating a first data item which represents the wavelength of the first radiation, the calculation comprising, for each scanned state of the source, a selection of a selected value of the first data item from a plurality of possible values, said selection comprising the elimination of the values of the first data item which do not correspond to a modulo constant of the free spectral range of the fixed cavity expressed according to the units of the first data item.