Fiber-Based Picosecond Pulse Source for Coherent Raman Microscopy

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Solution Overview

Problem

Current technologies for generating optical pulses for coherent Raman microscopy face challenges in producing synchronized picosecond pulses with narrow spectral widths and high peak power, often requiring expensive and bulky solid-state lasers, which are difficult to maintain and align, and suffer from noise and pulse walk-off issues in optical fibers.

Innovation Solution

The use of nonlinear optical wave mixing in optical fibers, specifically through four-wave mixing in normal dispersion photonic crystal fibers, to generate synchronized optical pulses with narrow spectral widths and high peak power, utilizing a seed laser to initiate the idler signal and counteract group-velocity mismatch, resulting in compact, robust, and efficient fiber-based sources for coherent Raman microscopies.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Power

If solid-state lasers are used to generate optical pulses for coherent Raman microscopy, then high peak power and narrow spectral width can be achieved, but the device becomes expensive, bulky, and difficult to maintain and align

Engineering Contradiction:
Improvepeak powerVSAvoiddevice complexity
Core Design Contradiction:
PowerVSDevice complexity

Solution Approach 1:

The patent replaces solid-state laser systems with a fiber-based optical parametric oscillator system. This substitution eliminates the need for complex solid-state laser components while achieving the same functional output of high peak power picosecond pulses suitable for coherent Raman microscopy

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

Solution Approach 2:

The patent changes the operating parameters by using normal dispersion photonic crystal fibers instead of traditional anomalous dispersion fibers. This parameter change enables four-wave mixing to produce narrow spectral width at the signal wavelength while maintaining high peak power, resolving the contradiction between power and device complexity

Inventive Principle:
Principle #35Parameter changes

2Reliability

If traditional optical fiber systems are used, then transmission can be achieved, but noise and pulse walk-off issues occur

Engineering Contradiction:
Improvesignal qualityVSAvoidnoise and pulse walk-off
Core Design Contradiction:
ReliabilityVSObject-affected harmful factors

Solution Approach 1:

The patent applies local quality by using normal dispersion photonic crystal fibers specifically engineered for the signal wavelength region. This localized optimization eliminates noise and pulse walk-off issues that plague traditional optical fiber systems, while maintaining reliable signal transmission for coherent Raman microscopy

Inventive Principle:
Principle #3Local quality

3Manufacturing precision

If four wave mixing is used in optical fiber to generate optical pulses, then synchronized picosecond pulses with narrow spectral width can be produced, but the system requires precise alignment and control

Engineering Contradiction:
Improvepulse synchronization and spectral widthVSAvoidalignment and control
Core Design Contradiction:
Manufacturing precisionVSEase of operation

Solution Approach 1:

The patent implements self-service through the optical feedback mechanism in the optical parametric oscillator. The system automatically maintains precise alignment and control conditions for four-wave mixing without requiring external intervention, achieving synchronized picosecond pulses with narrow spectral width while simplifying operation

Inventive Principle:
Principle #25Self-service

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 the production of high-quality, synchronized picosecond pulses with stable power and timing, suitable for coherent Raman microscopies, offering improved signal-to-noise ratios and reduced maintenance costs compared to traditional solid-state systems, while maintaining high coherence and efficiency.

Implementation Method 1

a segment of fiber having an input port and an output port, the input port coupled to receive the pump laser beam and configured to exhibit normal optical dispersion as a nonlinear optical four wave mixing medium to convert energy at the pump laser wavelength into a four wave mixing signal at a signal wavelength shorter than the pump laser wavelength and an idler signal at an idler wavelength longer than the laser pump wavelength

Methodology Applied
Scientific EffectFour wave mixing:

Implementation Method 2

configured to exhibit normal optical dispersion as a nonlinear optical four wave mixing medium

Methodology Applied
Scientific EffectNormal optical dispersion: Dispersion (of waves)

Implementation Method 3

a seed laser coupled to the input port of the segment of fiber to inject seed laser light at the idler wavelength with a narrow spectral width into the segment of fiber to coexist with the pump laser pulses inside the segment of fiber as a seed for initiating the idler signal for the four wave mixing in the segment of fiber

Methodology Applied
Scientific EffectNonlinear optical four wave mixing:

Implementation Method 4

an optical feedback path that feeds a portion of generated light at the third laser wavelength back to the segment of fiber to mix with the light at the first wavelength, and the seed light at the second wavelength, wherein the optical feedback is configured to sustain an optical parametric oscillation

Methodology Applied
Scientific EffectOptical parametric oscillation:

Data Source

PatentUS10608400B2Fiber source of synchronized picosecond pulses for coherent Raman microscopy and other applications
Publication Date: 2020.03.31 CORNELL UNIVERSITY
  • US10608400B2 patent drawing
  • US10608400B2 patent drawing
  • US10608400B2 patent drawing

AI summary

Devices and techniques that use nonlinear optical effects in optical fiber to generate optical pulses via nonlinear optical wave mixing for various applications such as coherent Raman microscopic measurements and optical parametric oscillators. In some implementations, a tunable optical delay path is provided to cause an adjustable delay for synchronizing two optical beams of optical pulses.