Spatial Chirped Cavity for Optical Pulse Dispersion

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Solution Overview

Problem

Existing optical fiber-based systems for pulse stretching and compression are limited by restricted wavelength operation ranges, non-tunability, spatial inefficiency, and material-induced optical nonlinearity, which restrict their applications in telecommunications, imaging, and beam scanning.

Innovation Solution

A spatially-chirped cavity with non-parallel mirrors in an air-filled optical cavity is used to achieve flexible and scalable pulse stretching or compression across a wide wavelength spectrum, from ultraviolet to infrared, without material dispersion, allowing for dynamic adjustment of group delay dispersion and eliminating mechanical limitations.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Adaptability or versatility

If optical fiber is used for pulse stretching/compression, then chromatic dispersion provides pulse stretching, but the wavelength range is restricted by material loss

Engineering Contradiction:
Improvewavelength operation rangeVSAvoidoptical loss
Core Design Contradiction:
Adaptability or versatilityVSLoss of energy

Solution Approach 1:

The patent extracts the dispersive function from material-based optical fibers and implements it through a spatial chirped cavity using geometric optics. The cavity uses non-parallel mirrors to create wavelength-dependent path lengths, achieving dispersion without material constraints. This allows operation across UV, visible, and infrared wavelengths without the loss limitations of silica glass fibers.

Inventive Principle:
Principle #2Taking out (Extraction)

Solution Approach 2:

The patent replaces the material-based dispersion mechanism (chromatic dispersion in optical fiber) with a geometric/mechanical dispersion mechanism (spatial chirped cavity with non-parallel mirrors). The dispersion is achieved through different optical path lengths for different wavelengths rather than through material refractive index variations, enabling broader wavelength operation.

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

2Manufacturing precision

If optical fiber length is increased to achieve sufficient GDD, then pulse stretching improves, but spatial efficiency deteriorates

Engineering Contradiction:
Improvegroup delay dispersionVSAvoidfiber length
Core Design Contradiction:
Manufacturing precisionVSVolume of moving object

Solution Approach 1:

The patent transitions from one-dimensional pulse propagation in optical fiber to two-dimensional spatial manipulation in a chirped cavity. The cavity uses angular dispersion and spatial separation of wavelengths, allowing sufficient GDD to be achieved in a compact three-dimensional volume rather than requiring long fiber lengths.

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

Solution Approach 2:

The patent changes the fundamental parameter for achieving dispersion from material properties (refractive index) and propagation length to geometric parameters (mirror angles, cavity dimensions). This allows high GDD to be achieved in a compact configuration by optimizing the geometric path differences for different wavelengths.

Inventive Principle:
Principle #35Parameter changes

3Manufacturing precision

If optical fiber is used for pulse stretching, then chromatic dispersion provides the effect, but optical nonlinearity distorts the pulse

Engineering Contradiction:
Improvepulse stretching accuracyVSAvoidoptical nonlinearity
Core Design Contradiction:
Manufacturing precisionVSObject-generated harmful factors

Solution Approach 1:

The patent extracts the dispersion function from the material medium and implements it through geometric optics in a chirped cavity. This eliminates the optical nonlinearity inherent in material-based dispersion while preserving the linear chromatic dispersion effect needed for pulse stretching.

Inventive Principle:
Principle #2Taking out (Extraction)

4Ease of operation

If optical fiber is used for pulse compression, then dispersion provides compression, but the system cannot be dynamically tuned

Engineering Contradiction:
ImprovetunabilityVSAvoidfiber length
Core Design Contradiction:
Ease of operationVSLength of stationary object

Solution Approach 1:

The patent implements dynamic tunability by making the cavity geometry adjustable. The mirror angles, cavity dimensions, and optical path lengths can be modified to change the dispersion characteristics and group delay, enabling the system to be tuned for different pulse compression ratios and wavelengths.

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 high-speed, flexible, and efficient pulse stretching or compression with significantly increased group delay dispersion, overcoming the limitations of traditional methods, and supports high-speed beam scanning and ultrafast imaging across a broad wavelength range.

Implementation Method 1

a spatial disperser arranged to divide a collimated optical pulsed beam into an array of beamlets with equally spaced angles

Methodology Applied
Scientific EffectSpatial dispersion: Dispersion (of waves)

Implementation Method 2

a cavity to sequentially reflect the individual beams within the beam array

Methodology Applied
Scientific EffectReflection: Reflection

Data Source

PatentUS10211587B2Spatial chirped cavity for temporally stretching/compressing optical pulses
Publication Date: 2019.02.19 VERSITECH LTD
  • US10211587B2 patent drawing
  • US10211587B2 patent drawing
  • US10211587B2 patent drawing

AI summary

Systems and methods for optical pulse stretching or compression in time are provided. An apparatus of the subject invention can operate as an optical dispersive element for optical pulse stretching or compression in time, as well as laser scanning in space. An apparatus can include a spatial disperser arranged to divide a collimated optical pulsed beam into an array of collimated beams with equally spaced angles, a beam shaper configured to control the spreading angle of the beam array, and a cavity to sequentially reflect the individual beams within the beam array. The cavity can include two non-parallel surfaces, such as two non-parallel mirrors.