Nonlinear Crystal Layout Within Rayleigh Length for Wavelength Conversion

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Solution Overview

Problem

Existing wavelength conversion systems face challenges in efficiently arranging nonlinear optical crystals due to hygroscopicity and the need for longer optical path lengths, leading to reduced efficiency and flexibility in design.

Innovation Solution

The proposed solution involves arranging nonlinear optical crystals within the Rayleigh length of the beam waist positions, using a light concentrating optical system to position the crystals optimally, and employing alternative polarization direction change methods like periscope mirrors to enhance efficiency and flexibility without relying on relay lens systems.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If nonlinear optical crystals are arranged with longer optical path lengths to address hygroscopicity, then reliability is improved, but wavelength conversion efficiency deteriorates

Engineering Contradiction:
Improvecrystal stabilityVSAvoidwavelength conversion efficiency
Core Design Contradiction:
ReliabilityVSProductivity

Solution Approach 1:

The patent changes the spatial parameter arrangement by positioning multiple nonlinear optical crystals within the Rayleigh length range of the beam waist position, rather than using longer optical path lengths. This parameter change maintains crystal stability while optimizing wavelength conversion efficiency through compact arrangement.

Inventive Principle:
Principle #35Parameter changes

Solution Approach 2:

The patent transitions from a linear optical path arrangement to a three-dimensional compact arrangement where crystals are positioned within the Rayleigh length volume around the beam waist. This dimensional reorganization allows simultaneous achievement of stability and efficiency.

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

2Ease of manufacture

If relay lens systems are used to arrange nonlinear optical crystals, then ease of manufacture is improved, but device complexity increases

Engineering Contradiction:
Improvecrystal arrangementVSAvoidoptical system complexity
Core Design Contradiction:
Ease of manufactureVSDevice complexity

Solution Approach 1:

The patent extracts and eliminates the relay lens system from the optical path, directly positioning nonlinear optical crystals within the Rayleigh length of the beam waist. This removal simplifies the overall device structure while maintaining manufacturing feasibility through precise crystal placement.

Inventive Principle:
Principle #2Taking out (Extraction)

3Ease of operation

If multiple nonlinear optical crystals are arranged outside the Rayleigh length, then ease of operation is improved, but wavelength conversion efficiency deteriorates

Engineering Contradiction:
Improvesystem operationVSAvoidwavelength conversion efficiency
Core Design Contradiction:
Ease of operationVSProductivity

Solution Approach 1:

The patent optimizes the spatial parameter by positioning crystals within the Rayleigh length range, changing the arrangement parameter from 'outside Rayleigh length' to 'within Rayleigh length'. This enables both efficient wavelength conversion and simplified operation through direct beam interaction.

Inventive Principle:
Principle #35Parameter changes

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 improves wavelength conversion efficiency and design flexibility by allowing multiple nonlinear optical crystals to be placed within the Rayleigh length, reducing the need for relay lenses and minimizing thermal effects.

Implementation Method 1

a first nonlinear optical crystal which first light having a first wavelength enters and from which second light having a second wavelength and being a second harmonic of the first light is output

Methodology Applied
Scientific EffectSecond harmonic generation: Second Harmonic Generation

Implementation Method 2

a second nonlinear optical crystal which the second light and third light having a third wavelength enter and from which the third light and fourth light having a fourth wavelength and being sum frequency light of the second light and the third light are output

Methodology Applied
Scientific EffectSum frequency generation:

Implementation Method 3

a third nonlinear optical crystal which the third light and the fourth light enter and from which fifth light having a fifth wavelength and being sum frequency light of the third light and the fourth light is output

Methodology Applied
Scientific EffectSum frequency generation:

Implementation Method 4

a light concentrating optical system configured to cause the first light to enter the first nonlinear optical crystal so that a beam waist position of the second light is located in the second nonlinear optical crystal

Methodology Applied
Scientific EffectOptical focusing: Focusing

Data Source

PatentUS20250208480A1Wavelength conversion system, solid-state laser system, and electronic device manufacturing method
Publication Date: 2025.06.26 GIGAPHOTON INC
  • US20250208480A1 patent drawing
  • US20250208480A1 patent drawing
  • US20250208480A1 patent drawing

AI summary

A wavelength conversion system includes a first nonlinear optical crystal which first light having a first wavelength enters and from which second light having a second wavelength is output, a second nonlinear optical crystal which the second light and third light having a third wavelength enter and from which the third light and fourth light having a fourth wavelength are output, a third nonlinear optical crystal which the third light and the fourth light enter and from which fifth light having a fifth wavelength is output, and a light concentrating optical system configured to cause the first light to enter the first nonlinear optical crystal. Here, the first nonlinear optical crystal is located in a range within a Rayleigh length of the second light, and the third nonlinear optical crystal is located in a range within a Rayleigh length of the fourth light.