Adiabatic Tapering Optical Fiber Mode Field Expander

Solution Overview

Problem

Existing methods for expanding the fundamental mode field of single-mode fibers face limitations, such as requiring precise alignment, high temperature processing, and limited expansion factors, which are not compatible with high numerical aperture fiber rods and are not suitable for mass production.

Innovation Solution

An apparatus comprising a fusion splice between a single mode fiber and a fiber rod, both without a cladding, followed by adiabatic tapering to achieve a normalized frequency of less than 0.5, allowing the fundamental mode to be guided by the cladding-air interface and expanded without coupling to higher order modes.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Area of moving object

If microlenses (GRIN lenses) are used to expand the fundamental mode field, then the mode field diameter is expanded, but precise alignment and critical lens length control are required, increasing device complexity and manufacturing difficulty

Engineering Contradiction:
Core Design Contradiction:
Area of moving objectVSDevice complexity

Solution Approach 1:

The patent removes the microlens component entirely from the system. Instead of using GRIN lenses that require precise alignment and critical length control, the invention uses direct adiabatic tapering of the fiber itself to achieve mode field expansion, thereby eliminating the complex alignment and manufacturing tolerances associated with lens-based expanders

Inventive Principle:
Principle #2Taking out (Extraction)

Solution Approach 2:

The patent combines the mode field expansion function directly into the fiber structure through adiabatic tapering, merging what were previously separate components (fiber + lens) into a single integrated tapered fiber structure. This eliminates the need for separate alignment of multiple components

Inventive Principle:
Principle #5Merging (Combining)

2Area of moving object

If core dopant diffusion (TEC techniques) is used to expand the mode field, then the fundamental mode size is increased, but extremely high temperatures and very long processing times are required, reducing manufacturing efficiency and potentially weakening the fiber

Engineering Contradiction:
Core Design Contradiction:
Area of moving objectVSProductivity

Solution Approach 1:

The patent replaces the thermal/chemical process of dopant diffusion with a mechanical/structural process of adiabatic tapering. Instead of using extreme temperatures and long chemical diffusion times, the invention uses controlled mechanical drawing to create a tapered fiber structure that achieves mode field expansion through geometric transformation alone

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

Solution Approach 2:

The patent changes the geometric parameters of the fiber (radius, cross-sectional area) through adiabatic tapering to achieve mode field expansion. By changing the physical dimensions rather than chemical composition, the process avoids high temperature requirements and long processing times while achieving the same functional result

Inventive Principle:
Principle #35Parameter changes

3Area of moving object

If high temperature processing is used for mode field expansion, then the mode field diameter is increased, but the fiber strength is reduced and shape distortion occurs

Engineering Contradiction:
Core Design Contradiction:
Area of moving objectVSStrength

Solution Approach 1:

The patent replaces thermal processing with mechanical drawing processes. The adiabatic tapering is achieved through controlled mechanical drawing that gradually reduces the fiber radius while maintaining structural integrity, avoiding the high temperatures that cause fiber weakening and shape distortion

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

4Device complexity

If conventional single mode fibers are used, then the fiber structure is simple, but the mode field diameter is limited and cannot match high numerical aperture fiber rods

Engineering Contradiction:
Core Design Contradiction:
Device complexityVSArea of moving object

Solution Approach 1:

The patent introduces dynamic geometric variation along the fiber length through adiabatic tapering. The fiber transitions from a uniform cross-section to a gradually varying cross-section, allowing the mode field diameter to continuously expand along the taper while maintaining single-mode operation throughout the transition

Inventive Principle:
Principle #15Dynamics

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 efficient expansion of the mode field to match high numerical aperture fiber rods, minimizing coupling losses and enabling high-quality beam output with reduced power density, suitable for applications like fiber Bragg gratings and high-powered fiber lasers.

Implementation Method 1

adiabatic tapering of the spliced single mode fiber and fiber rod

Methodology Applied
Scientific EffectAdiabatic tapering:

Implementation Method 2

the fundamental mode to be guided by the cladding-air interface and expanded without coupling to higher order modes

Methodology Applied
Scientific EffectTotal internal reflection: Total Internal Reflection

Implementation Method 3

a fusion splice of the single mode fiber and fiber rod

Methodology Applied
Scientific EffectFusion welding: Welding

Data Source

PatentUS7606452B2Optical fiber fundamental mode field expander
Publication Date: 2009.10.20
  • US7606452B2 patent drawing
  • US7606452B2 patent drawing
  • US7606452B2 patent drawing

AI summary

A device for providing an expanded mode field from a single mode optical waveguide is formed by fusing a length of single mode optical fiber with a length of fiber rod absent a cladding and adiabatically tapering the fused region. The length of single mode fiber has a core having a refractive index nco and a cladding having a refractive index ncl, wherein ncl<nco and wherein the cladding has an outer diameter ρ. The length of fiber rod absent the cladding has a refractive index of the fiber rod is substantially the same as the cladding index ncl of the single mode optical fiber. The outer diameter of the length of fiber rod is ρ, the same as the cladding diameter of the single mode fiber.