Angled Waveguide Interfaces Reduce Coherent Backscatter

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Solution Overview

Problem

Fiber optic gyroscope (FOG) systems experience corruption of electro-optic modulation due to ionic migration along electric fields near electrodes, leading to operational failures in non-atmospheric conditions, particularly when using proton-exchange waveguides.

Innovation Solution

The integration of Titanium-diffused waveguides in regions susceptible to electrical fields, coupled with proton-exchange waveguides, where the angles of incidence exceed the Brewster's angle to prevent light trapping and coherent back reflection, while maintaining the benefits of proton-exchange waveguides for polarization and precision.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Measurement precision

If proton-exchange waveguides are used in regions with electric fields, then polarization precision is improved, but ionic migration occurs leading to operational failure

Engineering Contradiction:
Improvepolarization precisionVSAvoidoperational reliability
Core Design Contradiction:
Measurement precisionVSReliability

Solution Approach 1:

The waveguide circuit is divided into distinct sections: proton-exchange waveguide sections for polarization-critical regions and Titanium-diffused waveguide sections for electric field-exposed regions. This segmentation allows each material to be used where it provides the most benefit while avoiding its drawbacks.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

Different waveguide materials are used in different locations based on local requirements. Proton-exchange waveguides are used where polarization precision is critical and electric field exposure is minimal, while Titanium-diffused waveguides are used in regions susceptible to electrical fields where ionic migration would occur.

Inventive Principle:
Principle #3Local quality

2Ease of manufacture

If waveguide sections are coupled at straight interfaces, then manufacturing is simplified, but coherent back reflection occurs corrupting modulation

Engineering Contradiction:
Improvewaveguide coupling simplicityVSAvoidcoherent back reflection
Core Design Contradiction:
Ease of manufactureVSObject-generated harmful factors

Solution Approach 1:

The waveguide interfaces are designed with angled surfaces rather than straight perpendicular couplings. This asymmetric geometry causes light to exit at angles greater than the Brewster's angle, preventing coherent back reflection while maintaining manufacturing feasibility through standard angled polishing techniques.

Inventive Principle:
Principle #4Asymmetry

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 configuration reduces errors in rotational rate measurements by minimizing the effects of ion migration and coherent back reflected light, ensuring stable and precise FOG operation in demanding navigation conditions.

Implementation Method 1

a first waveguide section of a first material having a first index of refraction, the first material configured to polarize light traveling in the first waveguide section

Methodology Applied
Scientific EffectPhotoelastic effect: Photoelasticity

Implementation Method 2

The first angle is selected such that the angle of incidence of light exiting the first waveguide section is greater than the Brewster's angle at the first interface

Methodology Applied
Scientific EffectBrewster's angle: Brewster's Angle

Data Source

PatentEP2995978B1System and method for reducing coherent backscatter in a stitched waveguide integrated optic circuit
Publication Date: 2017.08.23 HONEYWELL INTERNATIONAL INC
  • EP2995978B1 patent drawingFigure 1
  • EP2995978B1 patent drawingFigure 2
  • EP2995978B1 patent drawingFigure 3

AI summary

An integrated optical circuit comprises a first waveguide section of a first material having a first index of refraction, a second waveguide section diffused with a second material, different from the first material, the second waveguide section having a second index of refraction; and a third waveguide section of the first material. A portion of the first waveguide section at a first interface is angled at a first angle and a portion of the second waveguide section is angled at the first angle. A portion of the first waveguide section at a second interface is angled at a second angle and a portion of the third waveguide section is angled at the second angle. The first angle and second angle are selected such that the angle of incidence of light at the first and second interfaces is greater than the Brewster's angle.