Equality of critical thresholds for diffeomorphism groups

For a group of diffeomorphisms, define the distance threshold by

sdist=sup{sR:ds(g1,g2)=0 for all g1,g2},s^*_{\operatorname{dist}}=\sup\{s\in\mathbb R:d_s(g_1,g_2)=0\text{ for all }g_1,g_2\},

the smoothness threshold by

ssmooth=inf{sR:exp is C1},s^*_{\operatorname{smooth}}=\inf\{s\in\mathbb R:\operatorname{exp}\text{ is }C^1\},

and the Fredholm threshold by

sFred=inf{sR:vadvu0 is compact}.s^*_{\operatorname{Fred}}=\inf\{s\in\mathbb R:v\mapsto\operatorname{ad}_v^{\star}u_0\text{ is compact}\}.

Here dsd_s is the HsH^s geodesic distance, exp\operatorname{exp} is the Riemannian exponential map of the HsH^s metric, and vadvu0v\mapsto\operatorname{ad}_v^{\star}u_0 is the operator describing the Euler–Arnold equation. The critical-threshold conjecture. On any group of diffeomorphisms,

ssmooth=sFredsdist.s^*_{\operatorname{smooth}}=s^*_{\operatorname{Fred}}\leq s^*_{\operatorname{dist}}.

The relation holds in all cases known to the authors, including diffeomorphism, volume-preserving, and symplectomorphism groups, but remains conjectural in general; behavior at the critical index can differ between properties.

Sources & referencesView supporting material

Primary source

Martin Bauer, Philipp Harms and Stephen C. Preston, “Vanishing distance phenomena and the geometric approach to SQG”, arXiv:1805.04401 (2019).

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