Minimax eversion
In geometry, minimax eversions are a class of sphere eversions, constructed by using half-way models. It is a variational method, and consists of special homotopies (they are shortest paths with respect to Willmore energy); contrast with Thurston's corrugations, which are generic.
The original method of half-way models was not optimal: the regular homotopies passed through the midway models, but the path from the round sphere to the midway model was constructed by hand, and was not gradient ascent/descent.
Eversions via half-way models are called tobacco-pouch eversions by Francis and Morin.[1]
Half-way models
A half-way model is an immersion of the sphere [math]\displaystyle{ S^2 }[/math] in [math]\displaystyle{ \R^3 }[/math], which is so-called because it is the half-way point of a sphere eversion. This class of eversions has time symmetry: the first half of the regular homotopy goes from the standard round sphere to the half-way model, and the second half (which goes from the half-way model to the inside-out sphere) is the same process in reverse.
Explanation
File:Minimax Sphere Eversion.webm Rob Kusner proposed optimal eversions using the Willmore energy on the space of all immersions of the sphere [math]\displaystyle{ S^2 }[/math] in [math]\displaystyle{ \mathbf{R}^3 }[/math]. The round sphere and the inside-out round sphere are the unique global minima for Willmore energy, and a minimax eversion is a path connecting these by passing over a saddle point (like traveling between two valleys via a mountain pass).[2]
Kusner's half-way models are saddle points for Willmore energy, arising (according to a theorem of Bryant) from certain complete minimal surfaces in 3-space; the minimax eversions consist of gradient ascent from the round sphere to the half-way model, then gradient descent down (gradient descent for Willmore energy is called Willmore flow). More symmetrically, start at the half-way model; push in one direction and follow Willmore flow down to a round sphere; push in the opposite direction and follow Willmore flow down to the inside-out round sphere.
There are two families of half-way models (this observation is due to Francis and Morin):
- odd order: generalizing Boy's surface: 3-fold, 5-fold, etc., symmetry; half-way model is a double-covered projective plane (generically 2-1 immersed sphere).
- even order: generalizing Morin surface: 2-fold, 4-fold, etc., symmetry; half-way model is a generically 1-1 immersed sphere, and a twist by half a symmetry interchanges sheets of the sphere
History
The first explicit sphere eversion was by Shapiro and Phillips in the early 1960s, using Boy's surface as a half-way model. Later Morin discovered the Morin surface and used it to construct other sphere eversions. Kusner conceived the minimax eversions in the early 1980s: historical details.
References
- ↑ J. Scott Carter (2012). An Excursion in Diagrammatic Algebra: Turning a Sphere from Red to Blue. World Scientific. pp. 17–. ISBN 978-981-4374-50-7. https://books.google.com/books?id=UWS6CgAAQBAJ&pg=PA17.
- ↑ Michele Emmer (2005). The Visual Mind II. MIT Press. pp. 485–. ISBN 978-0-262-05076-0. https://archive.org/details/visualmindiileon00mich.
- Bending Energy and the Minimax Eversions (in John M. Sullivan's "The Optiverse" and Other Sphere Eversions)
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