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2018 Geodesics on ${\rm SO}(n)$ and a class of spherically symmetric maps as solutions to a nonlinear generalised harmonic map problem
Stuart Day, Ali Taheri
Topol. Methods Nonlinear Anal. 51(2): 637-662 (2018). DOI: 10.12775/TMNA.2018.020

Abstract

We address questions on existence, multiplicity as well as qualitative features including rotational symmetry for certain classes of geometrically motivated maps serving as solutions to the nonlinear system $$ \begin{cases} -{\rm div}[ F'(|x|,|\nabla u|^2) \nabla u] = F'(|x|,|\nabla u|^2) |\nabla u|^2 u & \text{in } \mathbb{X}^n,\\ |u| = 1 &\text{in } \mathbb{X}^n ,\\ u = \varphi &\text{on } \partial \mathbb{X}^n. \end{cases} $$ Here $\varphi \in \mathscr{C}^\infty(\partial \mathbb X^n, \mathbb S^{n-1})$ is a suitable boundary map, $F'$ is the derivative of $F$ with respect to the second argument, $u \in W^{1,p}(\mathbb X^n, \mathbb S^{n-1})$ for a fixed $1<p<\infty$ and ${\mathbb{X}}^n=\{x \in \mathbb R^n : a<|x|<b\}$ is a generalised annulus. Of particular interest are spherical twists and whirls, where following [26], a spherical twist refers to a rotationally symmetric map of the form $u\colon x \mapsto {\rm Q}(|x|)x|x|^{-1}$ with ${\rm Q}$ some suitable path in $\mathscr{C}([a, b], {\rm SO}(n))$ and a whirl has a similar but more complex structure with only $2$-plane symmetries. We establish the existence of an infinite family of such solutions and illustrate an interesting discrepancy between odd and even dimensions.

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Stuart Day. Ali Taheri. "Geodesics on ${\rm SO}(n)$ and a class of spherically symmetric maps as solutions to a nonlinear generalised harmonic map problem." Topol. Methods Nonlinear Anal. 51 (2) 637 - 662, 2018. https://doi.org/10.12775/TMNA.2018.020

Information

Published: 2018
First available in Project Euclid: 24 May 2018

zbMATH: 06928852
MathSciNet: MR3829048
Digital Object Identifier: 10.12775/TMNA.2018.020

Rights: Copyright © 2018 Juliusz P. Schauder Centre for Nonlinear Studies

Vol.51 • No. 2 • 2018
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