Phase-Only Resonator Beam Mode Transformation

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Solution Overview

Problem

Existing laser technologies face energy losses when generating Gaussian beams due to the suppression of higher order modes, and methods to produce flat-top-like beams within optical resonators are limited by the need for complex calculations and sensitivity to environmental perturbations.

Innovation Solution

The use of phase-only optical elements, specifically diffractive optical elements with non-spherical curvature, to alter the beam mode within the optical resonator, allowing for the generation of Gaussian beams at one end and flat-top-like profiles at the other end, with closed-form solutions for the phase profiles using the stationary phase method.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Manufacturing precision

If amplitude elements are used to suppress higher order modes to generate a Gaussian beam, then the Gaussian beam quality is improved, but energy loss increases

Engineering Contradiction:
ImproveGaussian beam qualityVSAvoidenergy loss
Core Design Contradiction:
Manufacturing precisionVSLoss of energy

Solution Approach 1:

The patent changes the parameter type from amplitude modulation to phase modulation. Phase-only optical elements alter the phase distribution of the beam to suppress higher order modes and generate Gaussian beams without the energy losses associated with amplitude filtering. This parameter change resolves the contradiction by achieving the same beam quality improvement through a different physical mechanism that conserves energy.

Inventive Principle:
Principle #35Parameter changes

2Loss of energy

If phase-only elements are used for beam shaping, then energy loss is reduced, but sensitivity to environmental perturbations increases

Engineering Contradiction:
Improveenergy lossVSAvoidsensitivity to environmental perturbations
Core Design Contradiction:
Loss of energyVSReliability

Solution Approach 1:

The patent employs optical elements with specific curved surfaces (spherical or aspherical mirrors) combined with phase-only elements. The curved surfaces provide robustness against environmental perturbations while the phase-only elements maintain low energy loss. The combination of geometric curvature and phase modulation resolves the contradiction by providing both energy efficiency and environmental stability.

Inventive Principle:
Principle #14Spheroidality (Curvature)

3Quantity of substance

If intra-cavity beam shaping is used to generate flat-top beams, then mode volume is increased for higher energy extraction, but the beam profile cannot be achieved with conventional resonator designs

Engineering Contradiction:
Improvemode volumeVSAvoidresonator design complexity
Core Design Contradiction:
Quantity of substanceVSDevice complexity

Solution Approach 1:

The patent segments the resonator design by introducing separate phase-only optical elements within the cavity. These elements are added to conventional resonator designs to enable flat-top beam generation without completely redesigning the entire resonator. The segmentation approach allows achieving increased mode volume while managing design complexity through modular addition of functional elements.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

The patent changes the phase parameter distribution within the resonator using phase-only elements to create the desired flat-top beam profile. By modifying the phase parameter rather than the entire resonator geometry, the patent achieves increased mode volume for higher energy extraction while avoiding excessive design complexity.

Inventive Principle:
Principle #35Parameter changes

4Device complexity

If conventional resonator designs are used, then design simplicity is maintained, but Gaussian beam generation requires suppression of higher order modes causing energy loss

Engineering Contradiction:
Improvedesign simplicityVSAvoidenergy loss
Core Design Contradiction:
Device complexityVSLoss of energy

Solution Approach 1:

The patent introduces phase-only optical elements as intermediary components within the conventional resonator. These intermediaries modify the beam phase to suppress higher order modes without requiring complete redesign of the resonator, thus maintaining design simplicity while eliminating energy loss from amplitude-based mode suppression.

Inventive Principle:
Principle #24Intermediary (Mediator)

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 low-loss, efficient generation of Gaussian and flat-top beams, enhancing thermal characteristics and energy extraction while simplifying the calculation of mirror surfaces, achieving faster convergence to the fundamental mode with reduced round trip losses.

Implementation Method 1

each optical element is a phase-only optical element operable to alter a mode of the beam as it propagates along the length of the optical resonator

Methodology Applied
Scientific EffectPhase modulation: Phase Modulation

Implementation Method 2

specifically diffractive optical elements with non-spherical curvature, to alter the beam mode within the optical resonator

Methodology Applied
Scientific EffectDiffraction: Diffraction

Data Source

PatentUS9031113B2Resonator with intracavity transformation of a Gaussian into a top-hat beam
Publication Date: 2015.05.12 COUNCIL FOR SCI IND RES
  • US9031113B2 patent drawing
  • US9031113B2 patent drawing
  • US9031113B2 patent drawing

AI summary

The invention relates to an optical resonator, laser apparatus and a method of generating a laser beam inside an optical resonator. The optical resonator (100) includes an optical cavity (102) and an optical element (104.1, 104.2) at either end thereof, operable to sustain a light beam (108) therein, characterized in that each optical element (104.1, 104.2) is a phase-only optical element operable to alter a mode of the beam (108) as it propagates along the length of the optical resonator (100), such that in use the beam (108) at one end of the optical resonator (100) has a Gaussian profile while the beam (108) at the other end of the optical resonator (100) has a non-Gaussian profile.