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The indicator of the Smith-Volterra-Cantor set is discontinuous exactly on a nowhere dense set, and is not Riemann integrable, because that set does not have measure zero

Statement refuted

Refuted: that a bounded function on [a,b] is Riemann integrable whenever its set of discontinuities is nowhere dense (FALSE: a bounded function on [a,b] is Riemann integrable exactly when its set of discontinuities is nowhere dense, Nowhere dense, meager (first category), residual, and second category subsets of R).

The witness is the indicator g of the Smith-Volterra-Cantor set S⊆[0,1] (The Smith-Volterra-Cantor set: the same construction removing, at stage n≥1, an open middle interval of length 4−n from each of the 2n−1 remaining intervals). Its set of discontinuities is exactly S, which is closed, nowhere dense and not of measure zero (The Smith-Volterra-Cantor set is compact, perfect and nowhere dense, and does not have measure zero); and g is not Riemann integrable, with

∫01‾g  =  0,∫01‾g  ≥  12.

The contrast with the Cantor set is the whole point. The Cantor set is also closed and nowhere dense, and its indicator is integrable, with integral 0 (The indicator of the Cantor set is discontinuous exactly on the Cantor set, which is null, so it is Riemann integrable with integral 0 even though it is discontinuous at uncountably many points). The two sets differ only in measure, and that is what decides (Lebesgue's criterion for Riemann integrability: a bounded f on [a,b] is Riemann integrable if and only if its set of discontinuities has measure zero).

The proof below is direct, from claim 4 of The Smith-Volterra-Cantor set is compact, perfect and nowhere dense, and does not have measure zero; it does not go through the forward half of Lebesgue's criterion for Riemann integrability: a bounded f on [a,b] is Riemann integrable if and only if its set of discontinuities has measure zero and so uses no choice principle.

Facts & Assumptions

Given: The Smith-Volterra-Cantor set S⊆[0,1] and its indicator g:[0,1]→R, with g(x)=1 for x∈S and g(x)=0 otherwise.

[A1]

The refuted claim: a bounded function on a closed bounded interval with distinct endpoints whose set of discontinuities is nowhere dense is Riemann integrable.

[L5]

A set with a least element has it as its infimum and one with a greatest element has it as its supremum; an infimum of a set all of whose members are ≥c is ≥c (Greatest lower bound (infimum), Maximum and minimum of a set, Complete ordered field (least-upper-bound property)).

[L6]

Finite sums: scaling, splitting, monotonicity in the terms, ∑i<n0=0; and a finite list of closed intervals extends to a sequence by degenerate intervals of length 0 without changing any partial total (Finite sums and finite products, by recursion, Laws of finite sums and finite products, Measure zero (a countable cover by intervals of total length below every ε) and content zero (a finite such cover)).

[L7]

Ordered-field arithmetic: for 0≤x≤1 and a real ρ>0 the reals u:=max⁡{0,x−ρ} and v:=min⁡{1,x+ρ} satisfy u<v and (u,v)⊆Nρ(x)∩[0,1]; and 0<2−1<1 (Maximum and minimum of a set, Order is preserved by adding a constant and by adding inequalities, Sign rules for products and monotonicity of multiplication, Ordered field, Complete ordered field (least-upper-bound property), The ε-neighbourhood and the punctured ε-neighbourhood of a point of R, Intervals of R: the nine order-convex forms, nondegeneracy, and length). These order-arithmetic facts are stated by their sources for the strict order only; the nonstrict forms used below follow by adjoining the equality case, in which the two sides coincide.

Counterexample

technique · direct
1.1

g takes only the values 0 and 1, so it is bounded on [0,1] and its Darboux sums and integrals are defined by [L4].

givenL4
1.2

Discontinuity on S. Let x∈S, so g(x)=1, and let a real ρ>0 be given. By [L7] the interval (u,v)⊆Nρ(x)∩[0,1] is nonempty and open, so by [L1] it contains a point y∉S; then ∣y−x∣<ρ, y∈[0,1] and ∣g(x)−g(y)∣=1, so continuity fails at x for ε:=1 (Continuity of f:A→R at a point of A and on A: the ε-δ condition, its agreement with lim⁡x→cf(x)=f(c) at a limit point, and continuity at an isolated point, Discontinuity of f at a point of its domain, and its classification: removable discontinuity, jump discontinuity and essential discontinuity, equivalently Rudin's discontinuities of the first and of the second kind).

givenL1L7
1.3

Continuity off S. Let x∈[0,1] with x∉S. Since S is closed, [L2] gives a real ρ>0 with Nρ(x)∩S=∅, so g vanishes on Nρ(x)∩[0,1] and continuity holds at x.

givenL1L2
2.1

So the set of discontinuities of g in [0,1] is exactly S, which is nowhere dense by [L1].

step 1.2step 1.3L1
2.2

Every lower sum is 0. Let P=(n,t) be a partition of [0,1] and i<n. By [L3] the interval (ti,ti+1) is a nonempty open subset of [0,1], so by [L1] it contains a point outside S, at which g takes the value 0; as g≥0, that value is the least element of g[Ii] and mi=0 by [L5]. Hence L(g,P)=0 by [L4] and [L6].

step 1.1L1L3L4L5L6
2.3

Every upper sum is at least 2−1. With P as above put B:={ i<n:Ii∩S≠∅ }. For i∈B the set g[Ii] contains 1, so Mi=1 by [L5]; for i∉B one has g[Ii]={0} and Mi=0. Hence U(g,P) is the sum of the Δi with i∈B, by [L4] and [L6].

step 1.1L4L5L6
3.1

The intervals Ii with i∈B cover S, since S⊆[0,1]=⋃i<nIi by [L3]. Extending that finite list to a sequence by degenerate intervals [0,0] ([L6]) gives a cover of S all of whose partial total lengths are at most U(g,P), so [L1] gives U(g,P)≥2−1.

step 2.3L1L3L6
4.1

By [L5] and step 2.2, ∫01‾g=0; by [L5] and step 3.1, ∫01‾g≥2−1>0. The two differ, so g is not Riemann integrable by [L4].

step 2.2step 3.1L4L5L7
5.1

So g is bounded on [0,1], an interval with 0<1, its set of discontinuities is nowhere dense by step 2.1, and it is not Riemann integrable: [A1] is refuted.

step 2.1step 4.1A1∎

Remarks

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