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In this chapter, we introduce the concept of conserved quantity of a constrained Willmore surface in a space-form. In codimension 1, the existence of a conserved quantity for a constrained Willmore surface characterizes the constancy of the mean curvature of the surface in some space-form. In codimension 2, surfaces with holomorphic mean curvature vector in some space-form are examples of constrained Willmore surfaces admitting a conserved quantity. Both constrained Willmore spectral deformation and Bäcklund transformation preserve the existence of a conserved quantity of a constrained Willmore surface, defining, in particular, transformations within the class of constant mean curvature surfaces in 3-dimensional space-forms, with, furthermore, preservation of both the space-form and the mean curvature, in the latter case, as we shall prove.
Willmore surfaces in space-forms are characterized by the harmonicity of the mean curvature sphere congruence. In this chapter, we introduce the concept of perturbed harmonicity of a bundle, which will apply to the mean curvature sphere congruence to provide a characterization of constrained Willmore surfaces in space-forms. A generalization of the well-developed integrable systems theory of harmonic maps emerges. The starting point is a zero-curvature characterization of constrained Willmore surfaces, due to Burstall–Calderbank, which we derive in this chapter. Constrained Willmore surfaces come equipped with a family of flat metric connections. We then define a spectral deformation of perturbed harmonic bundles, by the action of a loop of flat metric connections, and Bäcklund transformations, defined by the application of a version of the Terng–Uhlenbeck dressing action by simple factors. Transformations on the level of perturbed harmonic bundles prove to give rise to transformations on the level of constrained Willmore surfaces, via the mean curvature sphere congruence. We establish a permutability between spectral deformation and Bäcklund transformation and show that all these transformations corresponding to the zero Lagrange multiplier preserve the class of Willmore surfaces. We define, more generally, transformations of complexified surfaces and prove that, for special choices of parameters, both spectral deformation and Bäcklund transformation preserve reality conditions.
This chapter is dedicated to the special case of surfaces in 4-space. Our approach is quaternionic, based on the model of the conformal 4-sphere on the quaternionic projective space. We extend the Darboux transformation of Willmore surfaces in 4-space presented by Burstall–Ferus–Leschke–Pedit–Pinkall, based on the solution of a Riccati equation, to a transformation of constrained Willmore surfaces in 4-space into new ones. We prove that non-trivial Darboux transformation of constrained Willmore surfaces in 4-space can be obtained as a particular case of Bäcklund transformation. This Darboux transformation of constrained Willmore surfaces displays a striking similarity with the description of isothermic Darboux transformation of constant mean curvature surfaces in Euclidean 3-space presented by Hertrich-Jeromin−Pedit, which, in fact, proves to be obtainable as a particular case of constrained Willmore Bäcklund transformation.
From Bäcklund to Darboux, this monograph presents a comprehensive journey through the transformation theory of constrained Willmore surfaces, a topic of great importance in modern differential geometry and, in particular, in the field of integrable systems in Riemannian geometry. The first book on this topic, it discusses in detail a spectral deformation, Bäcklund transformations and Darboux transformations, and proves that all these transformations preserve the existence of a conserved quantity, defining, in particular, transformations within the class of constant mean curvature surfaces in 3-dimensional space-forms, with, furthermore, preservation of both the space-form and the mean curvature, and bridging the gap between different approaches to the subject, classical and modern. Clearly written with extensive references, chapter introductions and self-contained accounts of the core topics, it is suitable for newcomers to the theory of constrained Wilmore surfaces. Many detailed computations and new results unavailable elsewhere in the literature make it also an appealing reference for experts.
We generalize Uhlenbeck’s generator theorem of ${\mathcal{L}}^{-}\operatorname{U}_{n}$ to the full rational loop group ${\mathcal{L}}^{-}\operatorname{GL}_{n}\mathbb{C}$ and its subgroups ${\mathcal{L}}^{-}\operatorname{GL}_{n}\mathbb{R}$, ${\mathcal{L}}^{-}\operatorname{U}_{p,q}$: they are all generated by just simple projective loops. Recall that Terng–Uhlenbeck studied the dressing actions of such projective loops as generalized Bäcklund transformations for integrable systems. Our result makes a nice supplement: any rational dressing is the composition of these Bäcklund transformations. This conclusion is surprising in the sense that Lie theory suggests the indispensable role of nilpotent loops in the case of noncompact reality conditions, and nilpotent dressings appear quite complicated and mysterious. The sacrifice is to introduce some extra fake singularities. So we also propose a set of generators if fake singularities are forbidden. A very geometric and physical construction of $\operatorname{U}_{p,q}$ is obtained as a by-product, generalizing the classical construction of unitary groups.
Consider the sixth Painlevé equation $({{\text{P}}_{6}})$ below where $\alpha ,\beta ,\gamma$ and $\delta$ are complex parameters. We prove the necessary and sufficient conditions for the existence of rational solutions of equation $({{\text{P}}_{6}})$ in term of special relations among the parameters. The number of distinct rational solutions in each case is exactly one or two or infinite. And each of them may be generated by means of transformation group found by Okamoto [7] and Bäcklund transformations found by Fokas and Yortsos [4]. A list of rational solutions is included in the appendix. For the sake of completeness, we collected all the corresponding results of other five Painlevé equations $({{\text{P}}_{1}})-({{\text{P}}_{5}})$ below, which have been investigated by many authors [1]–[7].
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