Pulsed Fiber Laser Amplifier Mitigates Nonlinear Impairments

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Solution Overview

Problem

Current pulsed fiber laser systems face challenges in simultaneously achieving high peak powers, narrow spectral bandwidth, and single spatial mode operation due to nonlinear impairments such as Stimulated Brillouin Scattering, Stimulated Raman Scattering, and Self Phase Modulation, which limit their performance in applications like nonlinear frequency conversion and LIDAR systems.

Innovation Solution

A fiber laser system is designed with a master oscillator and a polarization-maintaining fiber amplifier using Yb- or Er-doped gain fibers, coupled with diode pump lasers and a pump coupler, to generate linearly-polarized laser radiation with adjustable pulse parameters, including peak power, repetition rate, and spectral bandwidth, while minimizing nonlinear impairments through careful design of the power amplifier stage and delivery fiber length.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Power

If high peak power is increased in pulsed fiber laser systems, then output power capability is improved, but nonlinear impairments such as Stimulated Brillouin Scattering, Stimulated Raman Scattering, and Self Phase Modulation increase and limit performance

Engineering Contradiction:
Improvepeak powerVSAvoidnonlinear impairments
Core Design Contradiction:
PowerVSObject-generated harmful factors

Solution Approach 1:

The patent employs pulsed operation mode where the laser operates in periodic pulses rather than continuous wave. By controlling pulse duration and repetition rate, the system achieves high peak power during pulses while allowing the fiber to cool between pulses, thereby reducing cumulative nonlinear effects and thermal damage while maintaining high average power output capability

Inventive Principle:
Principle #19Periodic action

Solution Approach 2:

The patent utilizes large mode area fibers with modified geometric parameters (core diameter, cladding structure) to reduce peak intensity for a given power level. By changing the spatial distribution parameters of the optical field, the system maintains high total power while reducing the intensity-dependent nonlinear effects that limit performance

Inventive Principle:
Principle #35Parameter changes

2Measurement precision

If narrow spectral bandwidth is achieved, then spectral purity is improved, but susceptibility to Self Phase Modulation and other nonlinear effects increases

Engineering Contradiction:
Improvespectral bandwidthVSAvoidSelf Phase Modulation
Core Design Contradiction:
Measurement precisionVSObject-generated harmful factors

Solution Approach 1:

The pulsed operation with controlled pulse widths (nanosecond to picosecond range) and repetition rates creates a spectral broadening effect through pulse gating that counteracts the narrowing from filtering. The periodic modulation in time domain translates to frequency domain characteristics that maintain narrow effective bandwidth while reducing the impact of SPM through the temporal structure

Inventive Principle:
Principle #19Periodic action

Solution Approach 2:

The patent employs large mode area fibers that change the confining parameters of the optical field, reducing the peak intensity and thereby reducing the Kerr effect strength. This parameter change in the fiber geometry allows narrow spectral bandwidth to be maintained without the same level of SPM degradation that would occur in conventional single-mode fibers

Inventive Principle:
Principle #35Parameter changes

3Shape

If single spatial mode operation is maintained, then beam quality is improved, but power scaling capability is limited

Engineering Contradiction:
Improvespatial modeVSAvoidpower scaling
Core Design Contradiction:
ShapeVSPower

Solution Approach 1:

The patent transitions from conventional single-mode operation to large mode area fiber operation, effectively moving to a different dimensional regime. By increasing the transverse dimension (mode area) while maintaining single-spatial-mode operation through careful design of the fiber geometry and pumping scheme, the system achieves both good beam quality and high power scaling capability simultaneously

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

Solution Approach 2:

The invention fundamentally changes the fiber geometric parameters (core size, cladding structure, doping concentration) to create large mode area fibers that support single-spatial-mode operation at much higher power levels. This parameter change in the fiber structure enables power scaling while maintaining the spatial mode purity required for good beam quality

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

The system achieves high peak powers from 10 kW to 500 kW with narrow spectral bandwidth and single spatial mode operation, allowing for efficient harmonic conversion and improved performance in applications like LIDAR and micromachining without increasing nonlinear fiber impairments, enabling flexible adjustment of pulse width and repetition rate without altering average power.

Implementation Method 1

The pump laser light is absorbed by the dopants in the gain fiber, raising the dopants into an excited state

Methodology Applied
Scientific EffectOptical absorption: Absorption (EM radiation)

Implementation Method 2

The emission from the master oscillator is amplified through stimulated emission as it interacts with the excited dopants implanted in the fiber core

Methodology Applied
Scientific EffectStimulated emission:

Implementation Method 3

The optical isolator protects the master oscillator from any light counter propagating back through the amplifier section

Methodology Applied
Scientific EffectOptical isolation:

Implementation Method 4

The pump laser light is absorbed by the dopants in the gain fiber, raising the dopants into an excited state

Methodology Applied
Scientific EffectOptical coupling:

Data Source

PatentUS7764719B2Pulsed fiber laser
Publication Date: 2010.07.27 LADARSYST INC
  • US7764719B2 patent drawing
  • US7764719B2 patent drawing
  • US7764719B2 patent drawing

AI summary

A fiber laser system includes a master oscillator configured to generate linear polarized infrared laser radiation with wavelengths of 1015-1085 nm, pulses with durations of 100 ps to 10 ns, pulse train repetition rates of 1 kHz to 10 MHz, spectral bandwidth less than 0.5 nm, and a predominately single spatial mode and a polarization-maintaining optical isolator optically coupled to the master oscillator. The fiber laser system also includes a fiber amplifier system optically coupled to the optical isolator and including a power amplifier configured to amplify the laser radiation transmitted through the optical isolator. The power amplifier includes a polarization-maintaining, large-mode-area, multiple-clad Yb-doped gain fiber having a core, an inner cladding, and at least an outer cladding, one or more diode pump lasers emitting pump light of a nominal wavelength of 976 nm, and a pump coupler configured to couple the pump light into the gain fiber.