Besicovitch's function #
Besicovitch's purely unrectifiable set with lower density 1/2 is the graph of the function
g = ∑ₙ fₙ, where fₙ is a square wave of period 2 * 2^(-n²) and amplitude
2^(-n²) / n. This file defines the function and proves the two estimates that everything
else rests on: inside a level-n cell g varies by at most 4 * 2^(-(n+1)²) / (n+1), and
across a level-n cell boundary it jumps by at least 2^(-n²) / n.
The construction follows Capdevila, Besicovitch's example in higher dimensions, arXiv:2607.05206, §2, which in turn follows Besicovitch (1938) and Dickinson (1939).
The length 2^(-n²) of a level-n cell.
Equations
- LeanPool.Besicovitch.Example.cellLength n = (1 / 2) ^ n ^ 2
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The amplitude 2^(-n²) / n of the level-n square wave.
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The index of the level-n cell [i * cellLength n, (i + 1) * cellLength n) containing x.
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The level-n square wave: -jumpHeight n on even cells, +jumpHeight n on odd cells.
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Besicovitch's function, the sum of the square waves of every level n ≥ 1.
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The cell lengths #
Consecutive cell lengths shrink by a factor of at least two.
At level n ≥ 1 consecutive cell lengths shrink by a factor of at least eight.
A coarser cell length is a natural multiple of a finer one.
The square waves #
Summability and the tail bound #
The amplitudes beyond level n sum to at most 2 * cellLength (n+1) / (n+1).
The two estimates #
The difference of g at two points, with the first n levels separated off.
The tail beyond level n contributes at most 4 * cellLength (n+1) / (n+1).
(E1) Inside a level-n cell, g varies by at most 4 * cellLength (n+1) / (n+1).