Inverse design of a Mamyshev oscillator with MW peak power by a particle swarm optimization algorithm

Alexander Perepelov; Alexander Perepelov; Evgeny Kuprikov; Alexey Kokhanovskiy

doi:10.1364/JOSAB.506416

Journal of the Optical Society of America B
Vol. 41,
Issue 2,
pp. A86-A91
(2024)
•https://doi.org/10.1364/JOSAB.506416

Inverse design of a Mamyshev oscillator with MW peak power by a particle swarm optimization algorithm

Alexander Perepelov, Evgeny Kuprikov, and Alexey Kokhanovskiy

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Alexander Perepelov, Evgeny Kuprikov, and Alexey Kokhanovskiy, "Inverse design of a Mamyshev oscillator with MW peak power by a particle swarm optimization algorithm," J. Opt. Soc. Am. B 41, A86-A91 (2024)

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Table of Contents Category
- Ultrafast Optics
Optics & Photonics Topics
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About this Article
History
- Original Manuscript: September 19, 2023
- Revised Manuscript: December 22, 2023
- Manuscript Accepted: December 27, 2023
- Published: January 24, 2024
Virtual Issues
JOSA B Feature Issue: Inverse Design in Photonics (2024)

Abstract

In this study we demonstrate implementation of a particle swarm optimization algorithm for inverse design of a fiber Mamyshev oscillator. We perform an extensive search in high-dimensional space of cavity parameters to maximize the output pulses’ peak power after external compression. The best obtained pulses have peak power exceeding 2 MW, energy ${\gt}{140}\;{\rm nJ}$, and duration ${\lt}{40}\;{\rm fs}$, and exhibit capabilities of handling ${\sim}75\pi$ nonlinear phase accumulation.

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Data availability

Data underlying the results presented in this paper are not publicly available at this time but may be obtained from the authors upon reasonable request.

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Passive Fibers
$β_{2}$	$22.2 {f s}^{2} / m m$
$β_{3}$	$63.8 {f s}^{3} / m m$
$γ$	$4 {k W}^{- 1} m^{- 1}$
Active Fibers
$β_{2}$	$24.9 {f s}^{2} / m m$
$β_{2}$	$59 {f s}^{3} / m m$
$γ$	$4 {k W}^{- 1} m^{- 1}$
$τ$	$850 µ s$
$N$	$4.8 \cdot 10^{25} m^{- 3}$
$r_{c o r e}$	$3 µ m$
Length	2.5 m
Filters
Transmittance	0.525

Parameter	Limits
Filter bandwidths	1–10 nm
Separation between filters	5–25 nm
PF spans $L_{3}$ and $L_{6}$	0–5 m
Output couplers’ ratios	0–1
AF pump powers	0–20 W
Multi-pass cell length	0–20 m

Parameter	Value	Tolerance
Filter 1 bandwidth	5.4 nm	0.1 nm
Filter 2 bandwidth	5.8 nm	0.1 nm
Separation between filters	10.6 nm	$> 1.1 n m$
PF length $L_{3}$	0 m	0.05 m
PF length $L_{6}$	0.6 m	0.09 m
Coupler 1 ratio	0.98	0.05
Coupler 2 ratio	0.57	$> 0.1$
AF1 pump power	9 W	0.25 W
AF2 pump power	2 W	$> 0.5 W$
Multi-pass cell length	6.6 m	0.3 m

Passive Fibers
$β_{2}$	$22.2 {f s}^{2} / m m$
$β_{3}$	$63.8 {f s}^{3} / m m$
$γ$	$4 {k W}^{- 1} m^{- 1}$
Active Fibers
$β_{2}$	$24.9 {f s}^{2} / m m$
$β_{2}$	$59 {f s}^{3} / m m$
$γ$	$4 {k W}^{- 1} m^{- 1}$
$τ$	$850 µ s$
$N$	$4.8 \cdot 10^{25} m^{- 3}$
$r_{c o r e}$	$3 µ m$
Length	2.5 m
Filters
Transmittance	0.525

Parameter	Limits
Filter bandwidths	1–10 nm
Separation between filters	5–25 nm
PF spans $L_{3}$ and $L_{6}$	0–5 m
Output couplers’ ratios	0–1
AF pump powers	0–20 W
Multi-pass cell length	0–20 m

Abstract

Data availability

Cited By

Figures (8)

Tables (3)

Equations (4)

Journal of the Optical Society of America B