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Concept
Geometric measure theory
Summary
In mathematics, geometric measure theory (GMT) is the study of geometric properties of sets (typically in Euclidean space) through measure theory. It allows mathematicians to extend tools from differential geometry to a much larger class of surfaces that are not necessarily smooth.
Geometric measure theory was born out of the desire to solve Plateau's problem (named after Joseph Plateau) which asks if for every smooth closed curve in there exists a surface of least area among all surfaces whose boundary equals the given curve. Such surfaces mimic soap films.
The problem had remained open since it was posed in 1760 by Lagrange. It was solved independently in the 1930s by Jesse Douglas and Tibor Radó under certain topological restrictions. In 1960 Herbert Federer and Wendell Fleming used the theory of currents with which they were able to solve the orientable Plateau's problem analytically without topological restrictions, thus sparking geometric measure theory. Later Jean Taylor after Fred Almgren proved Plateau's laws for the kind of singularities that can occur in these more general soap films and soap bubbles clusters.
The following objects are central in geometric measure theory:
Hausdorff measure and Hausdorff dimension
Rectifiable sets (or Radon measures), which are sets with the least possible regularity required to admit approximate tangent spaces.
Characterization of rectifiability through existence of approximate tangents, densities, projections, etc.
Orthogonal projections, Kakeya sets, Besicovitch sets
Uniform rectifiability
Rectifiability and uniform rectifiability of (subsets of) metric spaces, e.g. SubRiemannian manifolds, Carnot groups, Heisenberg groups, etc.
Connections to singular integrals, Fourier transform, Frostman measures, harmonic measures, etc
Currents, a generalization of the concept of oriented manifolds, possibly with boundary.
Flat chains, an alternative generalization of the concept of manifolds, possibly with boundary.
Official source
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