Isothermic hypersurfaces in R^{n+1}

TL;DR

This paper explores the geometry of isothermic hypersurfaces in R^{n+1}, establishing their connection to integrable systems and conformal invariance, and providing methods to construct and analyze these hypersurfaces using soliton theory.

Contribution

It introduces a correspondence between Combescure sequences of isothermic hypersurfaces and solutions of specific integrable systems, extending classical surface theory to higher dimensions.

Findings

Establishes a link between isothermic hypersurfaces and integrable systems.

Provides a framework for constructing hypersurfaces via soliton theory.

Describes the moduli space and symmetries of these geometric objects.

Abstract

A diagonal metric sum_{i=1}^n g_{ii} dx_i^2 is termed Guichard_k if sum_{i=1}^{n-k}g_{ii}-sum_{i=n-k+1}^n g_{ii}=0. A hypersurface in R^{n+1} is isothermic_k if it admits line of curvature co-ordinates such that its induced metric is Guichard_k. Isothermic_1 surfaces in R^3 are the classical isothermic surfaces in R^3. Both isothermic_k hypersurfaces in R^{n+1} and Guichard_k orthogonal co-ordinate systems on R^n are invariant under conformal transformations. A sequence of n isothermic_k hypersurfaces in R^{n+1} (Guichard_k orthogonal co-ordinate systems on R^n resp.) is called a Combescure sequence if the consecutive hypersurfaces (orthogonal co-ordinate systems resp.) are related by Combescure transformations. We give a correspondence between Combescure sequences of Guichard_k orthogonal co-ordinate systems on R^n and solutions of the O(2n-k,k)/O(n)xO(n-k,k)-system, and a correspondence between Combescure sequences of isothermic_k hypersurfaces in R^{n+1} and solutions of the O(2n+1-k,k)/O(n+1)xO(n-k,k)-system, both being integrable systems. Methods from soliton theory can therefore be used to construct Christoffel, Ribaucour, and Lie transforms, and to describe the moduli spaces of these geometric objects and their loop group symmetries.