The Fat Cantor Set

What if we dig out less? Removing only length 4−n4^{-n} per interval leaves a set that is compact, nowhere dense and perfect — yet keeps total length 12\frac12. Measure and topological size are independent notions.

∑n≥12n−14−n=12\sum_{n\ge 1} 2^{n-1} 4^{-n} = \frac12
m(C)=12,int C=∅m(C) = \frac12,\quad \mathrm{int}\,C = \varnothing

Part of these learning paths

Examples & Exercises

Consider the fat Cantor set: at stage nn, from each of the 2n−12^{n-1} surviving closed intervals remove the middle open interval of absolute length 4−n4^{-n}. Prove the total removed length over all stages is 12\tfrac12 via a geometric series, and check that the length remaining after NN stages is 1+2−N2\dfrac{1 + 2^{-N}}{2}.

∑n=1∞2n−1⋅4−n=∑n=1∞2−n−1=1/41−1/2=12\sum_{n=1}^{\infty} 2^{n-1} \cdot 4^{-n} = \sum_{n=1}^{\infty} 2^{-n-1} = \frac{1/4}{1 - 1/2} = \frac12
1−∑n=1N2−n−1=1−12(1−2−N)=12(1+2−N)  →N→∞  121 - \sum_{n=1}^{N} 2^{-n-1} = 1 - \tfrac12(1 - 2^{-N}) = \tfrac12(1 + 2^{-N}) \;\xrightarrow[N\to\infty]{}\; \tfrac12
Stage n=4n = 4: 16 intervals, remaining length 1732=0.53125→12\tfrac{17}{32} = 0.53125 \to \tfrac12 — the standard Cantor set has 16 intervals with (23)4=1681≈0.197531→0\left(\tfrac23\right)^4 = \tfrac{16}{81} \approx 0.197531 \to 0.
Show proof
  1. At stage nn there are 2n−12^{n-1} surviving closed intervals from stage n−1n-1, and exactly one middle open interval of length 4−n4^{-n} is removed from each. Removed open intervals from different stages and different parent intervals are all pairwise disjoint (each is carved out of the interior of a closed interval, and the surviving sets are nested). So the total length removed through stage NN is the sum of the per-stage contributions.
  2. The stage-nn contribution is 2n−1⋅4−n2^{n-1} \cdot 4^{-n}. Simplifying the exponent, 2n−14n=2n−122n=2−n−1\dfrac{2^{n-1}}{4^n} = \dfrac{2^{n-1}}{2^{2n}} = 2^{-n-1}, so the total removed length is the geometric series ∑n=1∞2−n−1\sum_{n=1}^{\infty} 2^{-n-1} with ratio 12\tfrac12. Its first term is 14\tfrac14, giving 1/41−1/2=12\dfrac{1/4}{1 - 1/2} = \tfrac12.
  3. The finite-stage version: through stage NN the total removed is the partial sum ∑n=1N2−n−1=14⋅1−2−N1−1/2=12(1−2−N)\sum_{n=1}^{N} 2^{-n-1} = \tfrac14 \cdot \dfrac{1 - 2^{-N}}{1 - 1/2} = \tfrac12(1 - 2^{-N}). Starting from [0,1][0,1], the length remaining after NN stages is 1−12(1−2−N)=12(1+2−N)1 - \tfrac12(1 - 2^{-N}) = \tfrac12(1 + 2^{-N}), tending to 12\tfrac12 as N→∞N \to \infty. For N=1N = 1 this is 1−14=34=12(1+12)1 - \tfrac14 = \tfrac34 = \tfrac12(1 + \tfrac12) — the surviving intervals [ 0,38 ][\,0, \tfrac38\,] and [ 58,1 ][\,\tfrac58, 1\,] with the middle (38,58)(\tfrac38, \tfrac58) carved out, exactly as the scene shows.
  4. Hence the pairwise-disjoint union GG of the removed open intervals has Lebesgue measure m(G)=12m(G) = \tfrac12, and since C=[0,1]∖GC = [0,1] \setminus G, we get m(C)=1−12=12>0m(C) = 1 - \tfrac12 = \tfrac12 > 0. This is where the fat Cantor set parts company with the standard Cantor set (middle third removed each stage, remaining length (2/3)n→0(2/3)^n \to 0).

Let the fat Cantor set be C=⋂n≥0FnC = \bigcap_{n \ge 0} F_n, where F0=[0,1]F_0 = [0,1] and FnF_n removes the middle open interval (length 4−n4^{-n}) from each closed interval of Fn−1F_{n-1}. Prove CC is compact, nowhere dense, and perfect (noting that its interior is empty yet m(C)=12m(C) = \tfrac12).

ℓn=ℓn−1−4−n2<2−n\ell_n = \frac{\ell_{n-1} - 4^{-n}}{2} < 2^{-n}
C=⋂n≥0Fn closed⊂[0,1] compactC = \bigcap_{n\ge 0} F_n\ \text{closed} \subset [0,1]\ \text{compact}
int⁡(C)=∅ (every open interval meets a removed piece)\operatorname{int}(C) = \varnothing\ \text{(every open interval meets a removed piece)}
x∈C⇒x=lim⁡zn, zn∈C∖{x}x \in C \Rightarrow x = \lim z_n,\ z_n \in C \setminus \{x\}
Stage n=4n = 4: 16 intervals with remaining length 0.531250.53125 — sixteen thin slivers, yet topologically the set is "hollow inside" (proof below: every open interval meets a removed piece).
Show proof
  1. Compact: each FnF_n is a finite union of closed intervals, hence closed, and C=⋂nFnC = \bigcap_n F_n is an intersection of closed sets, hence closed. Since C⊂[0,1]C \subset [0,1] is bounded, Heine–Borel makes CC compact.
  2. Length lemma: by symmetry every stage-nn interval has the same length. Calling it ℓn\ell_n, we have ℓ0=1\ell_0 = 1 and ℓn=(ℓn−1−4−n)/2\ell_n = (\ell_{n-1} - 4^{-n})/2, so ℓn<ℓn−1/2\ell_n < \ell_{n-1}/2. By induction ℓn<2−n\ell_n < 2^{-n}, and in particular ℓn→0\ell_n \to 0.
  3. Nowhere dense: since CC is closed, it suffices to show its closure — itself — has empty interior. Take a nonempty open interval II of length δ>0\delta > 0, shrinking it into (0,1)(0,1) if needed (otherwise I⊄CI \not\subset C trivially). Choose nn with 2−n<δ2^{-n} < \delta, so ℓn<δ\ell_n < \delta. Suppose II meets no removed open interval; then I⊂FnI \subset F_n. But FnF_n is a union of pairwise-disjoint closed intervals and II is connected, so II lies entirely inside exactly one of them, say JJ. Then δ=∣I∣≤∣J∣=ℓn<δ\delta = \lvert I \rvert \le \lvert J \rvert = \ell_n < \delta — contradiction.
  4. Hence II always meets a removed open interval, and the intersection is a nonempty open subset of I∖CI \setminus C. No nonempty open interval sits inside CC, so int⁡(C)=∅\operatorname{int}(C) = \varnothing — CC is nowhere dense.
  5. Perfect: let x∈Cx \in C. At each stage nn, xx lies in some stage-nn interval JnJ_n. At stage n+1n+1, JnJ_n splits into two closed children J′,J′′J', J'' separated by the removed open middle, and xx belongs to one of them, say J′J'. Choosing a nested chain of children, the nested-interval principle gives C∩J′′≠∅C \cap J'' \ne \varnothing, so pick zn∈C∩J′′z_n \in C \cap J''. The middle gap separates xx from znz_n, so zn≠xz_n \ne x, and ∣zn−x∣≤ℓn<2−n→0\lvert z_n - x \rvert \le \ell_n < 2^{-n} \to 0. Thus xx is a limit point of CC. This holds for every x∈Cx \in C, so CC is perfect.

Let U=[0,1]∖CU = [0,1] \setminus C be the complement of the fat Cantor set. Prove UU is (relatively) open, dense in [0,1][0,1], and has m(U)=12m(U) = \tfrac12. Then finish by completing this table: "empty interior, yet half the length" — measure and topological size are independent notions.

U=⋃stages(removed open intervals)U = \bigcup_{\text{stages}} \text{(removed open intervals)}
m(U)=12,m(C)=12m(U) = \tfrac12,\quad m(C) = \tfrac12
m=0m>0nowhere densestandard Cantorfat CantordenseQ∩[0,1]irrationals in [0,1]\begin{array}{c|cc} & m = 0 & m > 0 \\ \hline \text{nowhere dense} & \text{standard Cantor} & \textbf{fat Cantor} \\ \text{dense} & \mathbb{Q} \cap [0,1] & \text{irrationals in } [0,1] \end{array}
Stage n=4n = 4: the removed open intervals total 12(1−2−4)=0.46875\tfrac12(1 - 2^{-4}) = 0.46875 in length, leaving 0.531250.53125 — the complement is already nearly half, and in the limit exactly 12\tfrac12.
Show proof
  1. UU is the complement of the closed set CC, hence relatively open in [0,1][0,1]. Concretely, UU is the union of the removed open intervals over all stages — a countable union of pairwise-disjoint open intervals.
  2. Dense: the previous problem showed that every nonempty open interval meets a removed open interval. Hence every open interval contains a point of UU, so UU is dense in [0,1][0,1].
  3. Measure: the removed open intervals are pairwise disjoint, so m(U)=∑n=1∞2n−14−n=12m(U) = \sum_{n=1}^{\infty} 2^{n-1} 4^{-n} = \tfrac12 (the geometric series from the first problem). Hence m(C)=m([0,1])−m(U)=1−12=12m(C) = m([0,1]) - m(U) = 1 - \tfrac12 = \tfrac12.
  4. To summarize: CC is closed, has empty interior (nowhere dense), is perfect, and has length 12\tfrac12; its complement UU is open, dense, and has length 12\tfrac12. The table above fills all four cells — the standard Cantor set (nowhere dense, measure 0), the fat Cantor set (nowhere dense, measure 12\tfrac12), the rationals in [0,1][0,1] (dense, measure 0), the irrationals (dense, measure 1). There are even sets that are open and dense with arbitrarily small measure (around each rational qkq_k take an open interval of radius ε/2k\varepsilon/2^k: total measure ≤2ε\le 2\varepsilon). The punchline: the topological statement "has empty interior" and the measure-theoretic statement "has such-and-such length" impose nothing on each other — and the fat Cantor set is the most dramatic witness to their independence.

4. Topology