Polarization-Insensitive Resonant Grating Filter Design

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Solution Overview

Problem

Resonant grating optical filters are sensitive to polarization, especially at oblique incidence, making them challenging to tune in wavelength due to their dependence on polarization and requiring complex configurations that are difficult to implement.

Innovation Solution

A polarization-insensitive optical filter design featuring two one-dimensional resonant gratings arranged with a 90-degree angle between their axes, each periodic along different axes, allowing for orthogonal mode excitation and decoupling regardless of polar angle, enabling wavelength tunability by varying the polar angle of incidence.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If a single resonant grating is used to achieve narrow bandwidth filtering, then wavelength selectivity is improved, but polarization sensitivity increases making the filter difficult to tune

Engineering Contradiction:
Improvewavelength selectivityVSAvoidwavelength tunability
Core Design Contradiction:
Measurement precisionVSEase of operation

Solution Approach 1:

The patent divides the single resonant grating into two separate gratings (first grating and second grating) with different orientations. Each grating couples to different waveguide modes, and by segmenting the function across multiple components, the system achieves polarization independence while maintaining narrow bandwidth filtering capability.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent combines two resonant grating structures working together to achieve a single functional outcome of polarization-independent wavelength filtering. The first grating couples to first waveguide modes while the second grating couples to second waveguide modes, and their combined effect provides both wavelength selectivity and polarization independence.

Inventive Principle:
Principle #5Merging (Combining)

2Adaptability or versatility

If oblique incidence is used to achieve wavelength tuning, then tunability is improved, but polarization dependence worsens

Engineering Contradiction:
Improvewavelength tunabilityVSAvoidpolarization sensitivity
Core Design Contradiction:
Adaptability or versatilityVSObject-affected harmful factors

Solution Approach 1:

The patent introduces asymmetric orientation between the two gratings (first grating and second grating are not aligned) to break the polarization dependence. By arranging the gratings at specific angles relative to each other and to the waveguide modes, the system achieves insensitivity to incident polarization while maintaining angular tunability.

Inventive Principle:
Principle #4Asymmetry

Solution Approach 2:

The patent adds an angular dimension to the grating arrangement by orienting the first grating at an angle θ1 and the second grating at an angle θ2 relative to the waveguide modes. This angular configuration in addition to the wavelength parameter enables simultaneous polarization independence and wavelength tunability.

Inventive Principle:
Principle #17Another dimension (Dimensionality change)

3Object-affected harmful factors

If complex grating patterns are used to achieve polarization insensitivity, then polarization independence is improved, but device complexity increases

Engineering Contradiction:
Improvepolarization sensitivityVSAvoidgrating configuration complexity
Core Design Contradiction:
Object-affected harmful factorsVSDevice complexity

Solution Approach 1:

Instead of using a single complex two-dimensional grating pattern, the patent segments the function into two separate one-dimensional gratings with simpler periodic structures. Each grating has a regular pattern along its respective axis, avoiding the need for complex arbitrary patterns while achieving the same polarization-independent effect.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

Instead of making the grating pattern complex to achieve polarization insensitivity, the patent inverts the approach by using simple periodic gratings and achieving polarization independence through their relative orientation and the resulting mode coupling geometry. The complexity is inverted from the grating pattern itself to the spatial arrangement of multiple simple components.

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

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 filter achieves polarization independence and wavelength tunability across a wide range of polar incidence angles, simplifying implementation and maintaining effectiveness over a broad spectral range.

Implementation Method 1

The grating enables coupling, via an evanescent diffraction order, of the energy of an incident beam in free space to an optical mode of the multi-layer structure which acts as a waveguide

Methodology Applied
Scientific EffectEvanescent diffraction: Diffraction

Implementation Method 2

Such filters are also known as guided mode resonance filters or Fano resonance filters

Methodology Applied
Scientific EffectGuided mode resonance: Resonance

Implementation Method 3

Resonant grating optical filters are optical components for filtering in wavelength making it possible to obtain a very narrow bandwidth

Methodology Applied
Scientific EffectResonance: Resonance

Data Source

PatentEP2661649B1Wavelength tunable polarisation independent optical resonant grating filter
Publication Date: 2017.02.15 CENT NAT DETUD SPATIALES (CNES)
  • EP2661649B1 patent drawing
  • EP2661649B1 patent drawing
  • EP2661649B1 patent drawing

AI summary

The invention relates to a polarization-insensitive optical filter centered on a wavelength (?0) measured in vacuum, comprising: first and second waveguides (21, 21') each having a propagation mode; a first grating (11) formed in or on the surface of the first waveguide (21), the first grating being periodical at least along a first axis Ox defining a first orthonormal base Oxyz; a second grating (11') formed in or on the surface of the second waveguide (21), the second grating being periodical at least along a second axis Oxy' defining a second orthonormal base Ox'y'z; wherein the first and second gratings are provided above each other and are such that the first axis Ox and the second axis Ox' define an angle ? different from ± p /2 radians so that, when the first grating is illuminated by a light beam, the first and second propagation modes are excited and have orthogonal fields for a predetermined angle of incidence of the light beam.