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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][a,b] is Riemann integrable whenever its set of discontinuities is nowhere dense (FALSE: a bounded function on [a,b][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\mathbb{R}).

The witness is the indicator gg of the Smith-Volterra-Cantor set S[0,1]S \subseteq [0,1] (The Smith-Volterra-Cantor set: the same construction removing, at stage n1n \ge 1, an open middle interval of length 4n4^{-n} from each of the 2n12^{n-1} remaining intervals). Its set of discontinuities is exactly SS, 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 gg is not Riemann integrable, with

01g  =  0,01g    12.\underline{\int_0^1} g \;=\; 0, \qquad \overline{\int_0^1} g \;\ge\; \tfrac12 .

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 00 (The indicator of the Cantor set is discontinuous exactly on the Cantor set, which is null, so it is Riemann integrable with integral 00 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 ff on [a,b][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 ff on [a,b][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]S \subseteq [0,1] and its indicator g:[0,1]Rg : [0,1] \to \mathbb{R}, with g(x)=1g(x) = 1 for xSx \in S and g(x)=0g(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.

[L1]

SS is closed, bounded and nowhere dense, so SS contains no nonempty open set; and if (ak)(a_k), (bk)(b_k) are sequences of reals with akbka_k \le b_k, Sk[ak,bk]S \subseteq \bigcup_k[a_k,b_k] and k<i(bkak)M\sum_{k<i}(b_k-a_k) \le M for every iNi \in \mathbb{N}, then M21M \ge 2^{-1} (The Smith-Volterra-Cantor set is compact, perfect and nowhere dense, and does not have measure zero, The Smith-Volterra-Cantor set: the same construction removing, at stage n1n \ge 1, an open middle interval of length 4n4^{-n} from each of the 2n12^{n-1} remaining intervals, Nowhere dense, meager (first category), residual, and second category subsets of R\mathbb{R}, Interior, closure, boundary and exterior of a subset of R\mathbb{R}, Measure zero (a countable cover by intervals of total length below every ε\varepsilon) and content zero (a finite such cover)).

[L3]

For a partition P=(n,t)P = (n,t) of [0,1][0,1]: n1n \ge 1, ti<ti+1t_i < t_{i+1}, Δi>0\Delta_i > 0, Ii=[ti,ti+1]I_i = [t_i,t_{i+1}], [0,1]=i<nIi[0,1] = \bigcup_{i<n}I_i, and (ti,ti+1)(t_i,t_{i+1}) is a nonempty open subset of [0,1][0,1] (Partition of [a,b][a,b] as a finite strictly increasing list a=t0<t1<<tn=ba = t_0 < t_1 < \dots < t_n = b, its subintervals and their lengths, its mesh, refinement, and the common refinement of two partitions, Intervals of R\mathbb{R}: the nine order-convex forms, nondegeneracy, and length, Open subset of R\mathbb{R} (every point has a neighbourhood inside it), closed subset (complement open), and clopen).

[L4]

mi=infg[Ii]m_i = \inf g[I_i], Mi=supg[Ii]M_i = \sup g[I_i], L(g,P)=i<nmiΔiL(g,P) = \sum_{i<n}m_i\Delta_i, U(g,P)=i<nMiΔiU(g,P) = \sum_{i<n}M_i\Delta_i; 01g\underline{\int_0^1}g is the supremum of the lower sums and 01g\overline{\int_0^1}g the infimum of the upper sums; gg is integrable exactly when they agree (For bounded ff on [a,b][a,b] and a partition PP: the infimum mim_i and supremum MiM_i of ff on the ii-th subinterval, and the lower and upper Darboux sums L(f,P)=imiΔiL(f,P) = \sum_i m_i \Delta_i and U(f,P)=iMiΔiU(f,P) = \sum_i M_i \Delta_i, The lower and upper Darboux integrals of a bounded ff on [a,b][a,b] as supPL(f,P)\sup_P L(f,P) and infPU(f,P)\inf_P U(f,P), Darboux integrability as their equality, and the notation abf\int_a^b f, Lower bound, bounded below, bounded set).

[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\ge c is c\ge 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\sum_{i<n}0 = 0; and a finite list of closed intervals extends to a sequence by degenerate intervals of length 00 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\varepsilon) and content zero (a finite such cover)).

[L7]

Ordered-field arithmetic: for 0x10 \le x \le 1 and a real ρ>0\rho > 0 the reals u:=max{0,xρ}u := \max\{0,x-\rho\} and v:=min{1,x+ρ}v := \min\{1,x+\rho\} satisfy u<vu < v and (u,v)Nρ(x)[0,1](u,v) \subseteq N_\rho(x)\cap[0,1]; and 0<21<10 < 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\varepsilon-neighbourhood and the punctured ε\varepsilon-neighbourhood of a point of R\mathbb{R}, Intervals of R\mathbb{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

gg takes only the values 00 and 11, so it is bounded on [0,1][0,1] and its Darboux sums and integrals are defined by [L4].

givenL4
1.2

Discontinuity on SS. Let xSx \in S, so g(x)=1g(x) = 1, and let a real ρ>0\rho > 0 be given. By [L7] the interval (u,v)Nρ(x)[0,1](u,v) \subseteq N_\rho(x)\cap[0,1] is nonempty and open, so by [L1] it contains a point ySy \notin S; then yx<ρ|y-x| < \rho, y[0,1]y \in [0,1] and g(x)g(y)=1|g(x)-g(y)| = 1, so continuity fails at xx for ε:=1\varepsilon := 1 (Continuity of f:ARf : A \to \mathbb{R} at a point of AA and on AA: the ε\varepsilon-δ\delta condition, its agreement with limxcf(x)=f(c)\lim_{x \to c} f(x) = f(c) at a limit point, and continuity at an isolated point, Discontinuity of ff 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 SS. Let x[0,1]x \in [0,1] with xSx \notin S. Since SS is closed, [L2] gives a real ρ>0\rho > 0 with Nρ(x)S=N_\rho(x)\cap S = \varnothing, so gg vanishes on Nρ(x)[0,1]N_\rho(x)\cap[0,1] and continuity holds at xx.

givenL1L2
2.1

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

step 1.2step 1.3L1
2.2

Every lower sum is 00. Let P=(n,t)P = (n,t) be a partition of [0,1][0,1] and i<ni < n. By [L3] the interval (ti,ti+1)(t_i,t_{i+1}) is a nonempty open subset of [0,1][0,1], so by [L1] it contains a point outside SS, at which gg takes the value 00; as g0g \ge 0, that value is the least element of g[Ii]g[I_i] and mi=0m_i = 0 by [L5]. Hence L(g,P)=0L(g,P) = 0 by [L4] and [L6].

step 1.1L1L3L4L5L6
2.3

Every upper sum is at least 212^{-1}. With PP as above put B:={i<n:IiS}B := \{\, i < n : I_i \cap S \ne \varnothing \,\}. For iBi \in B the set g[Ii]g[I_i] contains 11, so Mi=1M_i = 1 by [L5]; for iBi \notin B one has g[Ii]={0}g[I_i] = \{0\} and Mi=0M_i = 0. Hence U(g,P)U(g,P) is the sum of the Δi\Delta_i with iBi \in B, by [L4] and [L6].

step 1.1L4L5L6
3.1

The intervals IiI_i with iBi \in B cover SS, since S[0,1]=i<nIiS \subseteq [0,1] = \bigcup_{i<n}I_i by [L3]. Extending that finite list to a sequence by degenerate intervals [0,0][0,0] ([L6]) gives a cover of SS all of whose partial total lengths are at most U(g,P)U(g,P), so [L1] gives U(g,P)21U(g,P) \ge 2^{-1}.

step 2.3L1L3L6
4.1

By [L5] and step 2.2, 01g=0\underline{\int_0^1}g = 0; by [L5] and step 3.1, 01g21>0\overline{\int_0^1}g \ge 2^{-1} > 0. The two differ, so gg is not Riemann integrable by [L4].

step 2.2step 3.1L4L5L7
5.1

So gg is bounded on [0,1][0,1], an interval with 0<10 < 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

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