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Main Author: Krechetnikov, R.
Format: Preprint
Published: 2022
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Online Access:https://arxiv.org/abs/2209.15391
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author Krechetnikov, R.
author_facet Krechetnikov, R.
contents Nonlinear Schrödinger equation was originally derived in nonlinear optics as a model for beam propagation, which naturally requires its application in cylindrical coordinates. However, the derivation was done in the Cartesian coordinates with the Laplacian $Δ_{\perp} = \partial_{x}^{2} + \partial_{y}^{2}$ transverse to the beam $z$-direction tacitly assumed to be covariant. As we show, first, with a simple example and, next, with a systematic derivation in cylindrical coordinates, $Δ_{\perp} = \partial_{r}^{2} + \frac{1}{r} \partial_{r}$ must be amended with a potential $V(r)=-\frac{1}{r^{2}}$, which leads to a Gross-Pitaevskii equation instead. Hence, the beam dynamics and collapse must be revisited.
format Preprint
id arxiv_https___arxiv_org_abs_2209_15391
institution arXiv
publishDate 2022
record_format arxiv
spellingShingle Nonlinear Schrödinger equation in cylindrical coordinates
Krechetnikov, R.
Pattern Formation and Solitons
Optics
Nonlinear Schrödinger equation was originally derived in nonlinear optics as a model for beam propagation, which naturally requires its application in cylindrical coordinates. However, the derivation was done in the Cartesian coordinates with the Laplacian $Δ_{\perp} = \partial_{x}^{2} + \partial_{y}^{2}$ transverse to the beam $z$-direction tacitly assumed to be covariant. As we show, first, with a simple example and, next, with a systematic derivation in cylindrical coordinates, $Δ_{\perp} = \partial_{r}^{2} + \frac{1}{r} \partial_{r}$ must be amended with a potential $V(r)=-\frac{1}{r^{2}}$, which leads to a Gross-Pitaevskii equation instead. Hence, the beam dynamics and collapse must be revisited.
title Nonlinear Schrödinger equation in cylindrical coordinates
topic Pattern Formation and Solitons
Optics
url https://arxiv.org/abs/2209.15391