The middle-third Cantor set has Hausdorff dimension
Its Lebesgue measure is zero, yet . These assertions measure different aspects of size: interval length is too coarse to distinguish this set from a null set, while the critical fractional measuring rule captures its remaining structure.
At level , the construction covers by intervals of diameter . Their total -cost is
For it tends to zero, proving the upper dimension bound. At it equals one, giving . For this particular cover's cost grows, but that alone would not prove a lower bound on Hausdorff measure.
Figure 1.
Cantor cover costs change trend at the critical exponent, and distributed mass supplies the lower bound
. Details.
For the matching lower bound, use the Cantor distribution, which assigns mass to each level- Cantor cylinder. An interval of length with meets at most two level- construction intervals, since their gaps are at least . Its mass is therefore at most
Every covering set of diameter in the line lies in an interval of length , so any small cover must have total -cost at least . This is the mass distribution principle in its interval form: , sufficient to prove the claimed dimension. The constants are convenient bounds, rather than an assertion of the exact critical Hausdorff measure. In the diagram, the right panel is a finite-stage approximation to the Cantor function, showing how probability is shared while the middle third receives none.
The reusable pattern is to obtain an upper bound by constructing covers and a lower bound by distributing mass. The same strategy underlies Cartesian powers of the Cantor set and the dimension formula for a finite similarity iterated function system satisfying the open set condition.
Let be the middle-third Cantor set and choose a positive integer with ; this is possible for every real , including negative . Set . It is closed and bounded since each factor is compact. If a subset of is connected, each coordinate projection is a connected subset of and hence a singleton; therefore the subset itself is a singleton. Thus is totally disconnected.
For completeness, the dimension of these Cartesian powers of the Cantor set can be checked directly. At stage there are cubes of side , giving vanishing -dimensional cover cost whenever . Conversely put independent equiprobable zero-or-two ternary digits on every coordinate. Each stage- cube has probability . If , a Euclidean ball of radius meets at most a constant depending on such cubes. Hence its probability is at most . For any sufficiently fine cover, summing this bound over covering sets shows that its cost at exponent is bounded below by a positive constant, since total probability is one. These upper and lower Hausdorff measure bounds prove
The construction does not claim arbitrarily large Hausdorff dimension in one fixed ambient Euclidean dimension.