Numerical observation of SPM rogue waves in normal dispersion cascaded supercontinuum generation

Rasmus Eilkœr Hansen; Rasmus Dybbro Engelsholm; Rasmus Dybbro Engelsholm; Christian Rosenberg Petersen; Christian Rosenberg Petersen; Ole Bang; Ole Bang; Ole Bang

doi:10.1364/JOSAB.428520

Journal of the Optical Society of America B
Vol. 38,
Issue 9,
pp. 2754-2764
(2021)
•https://doi.org/10.1364/JOSAB.428520

Numerical observation of SPM rogue waves in normal dispersion cascaded supercontinuum generation

Rasmus Eilkœr Hansen, Rasmus Dybbro Engelsholm, Christian Rosenberg Petersen, and Ole Bang

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Rasmus Eilkœr Hansen, Rasmus Dybbro Engelsholm, Christian Rosenberg Petersen, and Ole Bang, "Numerical observation of SPM rogue waves in normal dispersion cascaded supercontinuum generation," J. Opt. Soc. Am. B 38, 2754-2764 (2021)

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Abstract

Numerical modeling of cascaded mid-infrared (IR) supercontinuum generation (SCG) is used to study how an ensemble of spectrally and temporally distributed solitons from the long-wavelength part of an SC evolves when coupled into the normal dispersion regime of a highly nonlinear chalcogenide fiber. This has revealed a novel phenomenon—the generation of a high-energy rogue wave in the normal dispersion regime in the form of a strong self-phase-modulation (SPM) chirped pulse. This SPM rogue wave is generated by swallowing the energy of many sufficiently closely spaced pulses through inter-pulse Raman amplification and is a key effect behind efficient cascaded mid-IR SCG.

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Supplementary Material (2)

Name	Description
Supplement 1	We provide simulation parameters for reproduction, as well as additional simulated results.
Visualization 1	In this video we show the initial propagation of a single input pulse. The pulse undergoes self-phase-modulation and optical wave breaking.

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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Fiber	a $[µ m]$	NA	$n_{2} \cdot 10^{20}$ $[m^{2} / W]$	$f_{R}$	Company
ZBLAN	3.5	0.265	2.1	0.0969	FiberLabs
$A s_{2} S e_{3}$	6	0.76	1500	0.0103	IRflex

#	$P_{0}$ $[k W]$	$T_{F W H M}$ $[f s]$	$λ_{0}$ $[µ m]$	$γ$ $[1 / (W m)]$	$β_{2}$ $[p s^{2} / m]$	$z_{O W B}$ $[m m]$
1	42.8	50	2.55	0.58	523	1.3
2	78.6	30	2.72	0.54	476	0.6
3	44.2	90	2.68	0.55	487	2.5

Fiber	a $[µ m]$	NA	$n_{2} \cdot 10^{20}$ $[m^{2} / W]$	$f_{R}$	Company
ZBLAN	3.5	0.265	2.1	0.0969	FiberLabs
$A s_{2} S e_{3}$	6	0.76	1500	0.0103	IRflex

#	$P_{0}$ $[k W]$	$T_{F W H M}$ $[f s]$	$λ_{0}$ $[µ m]$	$γ$ $[1 / (W m)]$	$β_{2}$ $[p s^{2} / m]$	$z_{O W B}$ $[m m]$
1	42.8	50	2.55	0.58	523	1.3
2	78.6	30	2.72	0.54	476	0.6
3	44.2	90	2.68	0.55	487	2.5

Rasmus Eilkœr Hansen	https://orcid.org/0000-0001-8545-5765
Christian Rosenberg Petersen	https://orcid.org/0000-0002-2883-7908
Ole Bang	https://orcid.org/0000-0002-8041-9156

Abstract

Supplementary Material (2)

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Equations (7)

Journal of the Optical Society of America B