Tangency properties of sets with finite geometric curvature energies

Sebastian Scholtes. "Tangency properties of sets with finite geometric curvature energies." Fundamenta Mathematicae 218.2 (2012): 165-191. <http://eudml.org/doc/282807>.

@article{SebastianScholtes2012,
abstract = {We investigate tangential regularity properties of sets of fractal dimension, whose inverse thickness or integral Menger curvature energies are bounded. For the most prominent of these energies, the integral Menger curvature $ℳ_\{p\}^\{α\}(X): = ∫_\{X\}∫_\{X\}∫_\{X\} κ^\{p\}(x,y,z) d ^\{α\}_\{X\}(x)d ^\{α\}_\{X\}(y)d ^\{α\}_\{X\}(z)$, where κ(x,y,z) is the inverse circumradius of the triangle defined by x,y and z, we find that $ℳ_\{p\}^\{α\}(X) < ∞$ for p ≥ 3α implies the existence of a weak approximate α-tangent at every point of the set, if some mild density properties hold. This includes the scale invariant case p = 3 for $ℳ ¹_\{p\}$, for which, to the best of our knowledge, no regularity properties have been established before. Furthermore we prove that for α = 1 these exponents are sharp, i.e., if p lies below the threshold value of scale invariance, then there exists a set containing points with no weak approximate 1-tangent, but such that the energy is still finite. Moreover we demonstrate that weak approximate tangents are the most we can expect. For the other curvature energies analogous results are shown.},
author = {Sebastian Scholtes},
journal = {Fundamenta Mathematicae},
keywords = {approximate tangent; Menger curvature; geometric curvature energy},
language = {eng},
number = {2},
pages = {165-191},
title = {Tangency properties of sets with finite geometric curvature energies},
url = {http://eudml.org/doc/282807},
volume = {218},
year = {2012},
}

TY - JOUR
AU - Sebastian Scholtes
TI - Tangency properties of sets with finite geometric curvature energies
JO - Fundamenta Mathematicae
PY - 2012
VL - 218
IS - 2
SP - 165
EP - 191
AB - We investigate tangential regularity properties of sets of fractal dimension, whose inverse thickness or integral Menger curvature energies are bounded. For the most prominent of these energies, the integral Menger curvature $ℳ_{p}^{α}(X): = ∫_{X}∫_{X}∫_{X} κ^{p}(x,y,z) d ^{α}_{X}(x)d ^{α}_{X}(y)d ^{α}_{X}(z)$, where κ(x,y,z) is the inverse circumradius of the triangle defined by x,y and z, we find that $ℳ_{p}^{α}(X) < ∞$ for p ≥ 3α implies the existence of a weak approximate α-tangent at every point of the set, if some mild density properties hold. This includes the scale invariant case p = 3 for $ℳ ¹_{p}$, for which, to the best of our knowledge, no regularity properties have been established before. Furthermore we prove that for α = 1 these exponents are sharp, i.e., if p lies below the threshold value of scale invariance, then there exists a set containing points with no weak approximate 1-tangent, but such that the energy is still finite. Moreover we demonstrate that weak approximate tangents are the most we can expect. For the other curvature energies analogous results are shown.
LA - eng
KW - approximate tangent; Menger curvature; geometric curvature energy
UR - http://eudml.org/doc/282807
ER -