Alphabeta Math
Session-authored (Fable 5 assisted)
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced — the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted — a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated — a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

8 results · all verified · 7 also independently AI-judged
Every result on this page is machine-checked by a proof checker and read in full and owner-audited; the judge is an additional, independent cross-model AI review of the proofs. The 1 not AI-judged were verified by owner audit (typically over a confirmed judge false positive), not failures.

Bases and Dimension: Examples and Counterexamples

1 · Prerequisites

2 · Summary

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

ExampleConstruction: AI-generatedVerification: AI-generatedprecheck passjudge pass (z-ai/glm-5.2)audited 2026-07-28Open item page →

The vector (1,2)R2(1,2) \in \mathbb{R}^{2} has coordinate list (1,2)(1,2) in the standard ordered basis, (2,1)(2,1) in its reversal, and (2,1)(2,-1) in the ordered basis ((1,1),(1,0))\bigl((1,1),(1,0)\bigr)

Example

Let R\mathbb{R} be the real numbers (The real numbers), a field (The reals form a field), and let R2\mathbb{R}^{2} be the function space on the von Neumann natural 2={0,1}2 = \{0,1\} with the pointwise operations (The vector space FXF^{X} of all functions XFX \to F with pointwise operations, and FnF^{n} as the case X=n={0,1,,n1}X = n = \{0, 1, \dots, n-1\}, The natural numbers N\mathbb{N} (von Neumann), On N\mathbb{N} the order is membership: m<n    mnm < n \iff m \in n). We write (y0,y1)(y_0, y_1) for the element yy of R2\mathbb{R}^{2} with y(0)=y0y(0) = y_0 and y(1)=y1y(1) = y_1, so that e0=(1,0)e_0 = (1,0) and e1=(0,1)e_1 = (0,1) are the standard unit vectors (The standard list e:nFne : n \to F^{n} with ei(i)=1Fe_i(i) = 1_F and ei(j)=0Fe_i(j) = 0_F for jij \ne i is an ordered basis of FnF^{n}; hence dimFFn=n\dim_F F^{n} = n, and F0F^{0} is the zero space with basis \varnothing and dimension 00).

Put x:=(1,2)x := (1,2) and consider three ordered bases of R2\mathbb{R}^{2} (Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis):

  • e=(e0,e1)e = (e_0, e_1), the standard ordered basis;
  • e=(e1,e0)e' = (e_1, e_0), its reversal, which has the same image {e0,e1}\{e_0, e_1\};
  • v=(v0,v1)v = (v_0, v_1) with v0:=(1,1)v_0 := (1,1) and v1:=(1,0)v_1 := (1,0).

Then the coordinate list of xx (A finite list v:nVv : n \to V is an ordered basis if and only if every xVx \in V equals i<nλivi\sum_{i<n} \lambda_i v_i for exactly one λ:nF\lambda : n \to F; those scalars are the coordinates of xx in that ordered basis) is

(1,2)  in e,(2,1)  in e,(2,1)  in v.(1,2) \ \text{ in } e, \qquad (2,1) \ \text{ in } e', \qquad (2,-1) \ \text{ in } v .

Three different lists for one vector, and the first two differ although the two ordered bases have the same image. Coordinates are attached to an ordered basis, not to a basis.

Facts & Assumptions

Given: The field R\mathbb{R}, the vector space R2\mathbb{R}^{2} with pointwise operations, the vector x=(1,2)x = (1,2), and the three lists ee, ee' and vv above.

[L1]
[L2]

e:2R2e : 2 \to \mathbb{R}^{2} is an ordered basis, and (i<2λiei)(j)=λj\bigl(\sum_{i<2}\lambda_i e_i\bigr)(j) = \lambda_j for every λ:2R\lambda : 2 \to \mathbb{R} and j<2j < 2 (The standard list e:nFne : n \to F^{n} with ei(i)=1Fe_i(i) = 1_F and ei(j)=0Fe_i(j) = 0_F for jij \ne i is an ordered basis of FnF^{n}; hence dimFFn=n\dim_F F^{n} = n, and F0F^{0} is the zero space with basis \varnothing and dimension 00, claims 2 and 3).

[L5]

The vector space axioms and the field axioms of R\mathbb{R}: (V2) λ(y+z)=λy+λz\lambda(y+z) = \lambda y + \lambda z, (V3) (λ+μ)y=λy+μy(\lambda+\mu)y = \lambda y + \mu y, (V5) 1y=y1y = y; (V,+,0V)(V,+,0_V) is abelian; 0y=0V0y = 0_V; and R\mathbb{R} is a field (Vector space over a field, In any vector space 0Fv=0V0_F v = 0_V, λ0V=0V\lambda 0_V = 0_V, (λ)v=(λv)(-\lambda)v = -(\lambda v), (1F)v=v(-1_F)v = -v, and λv=0V\lambda v = 0_V forces λ=0F\lambda = 0_F or v=0Vv = 0_V, Field, The reals form a field).

[L6]

Injectivity and images are as in Injection, surjection, bijection.

Verification

technique · direct
1.1

Coordinates in ee. By the standard basis lemma, ee is an ordered basis of R2\mathbb{R}^{2} and the coordinate list of yR2y \in \mathbb{R}^{2} is iy(i)i \mapsto y(i); for x=(1,2)x = (1,2) that list is (1,2)(1,2).

L2L3
1.2

ee' is an ordered basis. The list e=(e1,e0)e' = (e_1, e_0) is injective, since e0e1e_0 \ne e_1 (e0e_0 takes the value 11 at 00 and e1e_1 takes the value 00 there), and its image is {e0,e1}=e[2]\{e_0, e_1\} = e[2], which is a basis of R2\mathbb{R}^{2}; so ee' is an injective list whose image is a basis.

L1L2L6
1.3

Coordinates in ee'. For λ:2R\lambda : 2 \to \mathbb{R}, i<2λiei=λ0e1+λ1e0=λ1e0+λ0e1=i<2μiei\sum_{i<2}\lambda_i e'_i = \lambda_0 e_1 + \lambda_1 e_0 = \lambda_1 e_0 + \lambda_0 e_1 = \sum_{i<2}\mu_i e_i with μ0=λ1\mu_0 = \lambda_1 and μ1=λ0\mu_1 = \lambda_0; evaluating with the standard basis, this vector is (λ1,λ0)(\lambda_1, \lambda_0). It equals x=(1,2)x = (1,2) exactly when λ1=1\lambda_1 = 1 and λ0=2\lambda_0 = 2, so the coordinate list of xx in ee' is (2,1)(2,1).

L2L4L5
1.4

vv is an ordered basis and the coordinates of a general vector in it. Note v0=(1,1)=e0+e1v_0 = (1,1) = e_0 + e_1 and v1=(1,0)=e0v_1 = (1,0) = e_0. For λ:2R\lambda : 2 \to \mathbb{R}, i<2λivi=λ0(e0+e1)+λ1e0=(λ0e0+λ0e1)+λ1e0=(λ0+λ1)e0+λ0e1\sum_{i<2}\lambda_i v_i = \lambda_0(e_0+e_1) + \lambda_1 e_0 = (\lambda_0 e_0 + \lambda_0 e_1) + \lambda_1 e_0 = (\lambda_0 + \lambda_1)e_0 + \lambda_0 e_1, using (V2), (V3) and the abelian group laws; by the standard basis this vector is (λ0+λ1, λ0)(\lambda_0 + \lambda_1,\ \lambda_0). Given y=(y0,y1)y = (y_0, y_1), the equations λ0+λ1=y0\lambda_0 + \lambda_1 = y_0 and λ0=y1\lambda_0 = y_1 have the unique solution λ0=y1\lambda_0 = y_1, λ1=y0y1\lambda_1 = y_0 - y_1, so every yy is i<2λivi\sum_{i<2}\lambda_i v_i for exactly one λ\lambda and vv is an ordered basis.

L2L3L4L5
2.1

Coordinates of xx in vv. Taking y=x=(1,2)y = x = (1,2) in step 1.4 gives λ0=2\lambda_0 = 2 and λ1=12=1\lambda_1 = 1 - 2 = -1, so the coordinate list of xx in vv is (2,1)(2,-1); and 2(1,1)+(1)(1,0)=(2,2)+(1,0)=(1,2)=x2(1,1) + (-1)(1,0) = (2,2) + (-1,0) = (1,2) = x confirms it.

step 1.4L1L5
3.1

The three coordinate lists of the single vector xx are therefore (1,2)(1,2), (2,1)(2,1) and (2,1)(2,-1), computed in steps 1.1, 1.3 and 2.1; the first two are different although ee and ee' have the same image, so the coordinate list depends on the ordered basis and not merely on the underlying set.

step 1.1step 1.3step 2.1

Remarks

  • What is and is not being said. Uniqueness of the coordinate list (A finite list v:nVv : n \to V is an ordered basis if and only if every xVx \in V equals i<nλivi\sum_{i<n} \lambda_i v_i for exactly one λ:nF\lambda : n \to F; those scalars are the coordinates of xx in that ordered basis) is uniqueness for a fixed ordered basis. Nothing there says that different ordered bases give the same list, and this example shows they do not, even when they differ only in the order. Reordering the list permutes the coordinates of every vector at once.

  • The third basis is not a reordering of the first. Its image {(1,1),(1,0)}\{(1,1),(1,0)\} is a different set from {(1,0),(0,1)}\{(1,0),(0,1)\}, and its coordinates differ for a further reason: the vectors themselves are different. The passage between coordinate lists of two ordered bases is a change of basis, taken up on a later page once linear maps are available; the point here is only that the two lists differ.

  • The arithmetic was recomputed, not copied. With v0=(1,1)v_0 = (1,1) and v1=(1,0)v_1 = (1,0), matching (1,2)(1,2) forces the second coordinate first: λ0\lambda_0 is the second entry, so λ0=2\lambda_0 = 2, and then λ1=12=1\lambda_1 = 1 - 2 = -1. Reading the pair off in the other order would give (1,2)(-1,2), which is wrong.

ExampleConstruction: AI-adaptedVerification: AI-generatedprecheck passjudge pass (z-ai/glm-5.2)audited 2026-07-28Open item page →

The standard unit families ekFNe_k \in F^{\mathbb{N}} form a basis of the linear subspace of eventually zero families: an explicit infinite basis, built with no choice principle

Example

Let FF be a field (Field) and let FNF^{\mathbb{N}} be the function space of all families x:NFx : \mathbb{N} \to F with the pointwise operations (The vector space FXF^{X} of all functions XFX \to F with pointwise operations, and FnF^{n} as the case X=n={0,1,,n1}X = n = \{0, 1, \dots, n-1\}); N\mathbb{N} contains 00 (The natural numbers N\mathbb{N} (von Neumann)). Put

E  :=  {xFN  :  there is NN with x(n)=0F for every nN},E \;:=\; \{\, x \in F^{\mathbb{N}} \;:\; \text{there is } N \in \mathbb{N} \text{ with } x(n) = 0_F \text{ for every } n \ge N \,\},

the eventually zero families, and for kNk \in \mathbb{N} let ekFNe_k \in F^{\mathbb{N}} be the standard unit family with ek(k)=1Fe_k(k) = 1_F and ek(n)=0Fe_k(n) = 0_F for nkn \ne k. Write B:={ek:kN}B := \{\, e_k : k \in \mathbb{N} \,\}. Then:

  1. EE is a linear subspace of FNF^{\mathbb{N}} (Linear subspace of a vector space);
  2. BEB \subseteq E and span(B)=E\operatorname{span}(B) = E (Linear combination of a finite list, and the span span(S)\operatorname{span}(S) as the smallest linear subspace containing SS);
  3. BB is linearly independent (Linear independence: a finite list v:nVv : n \to V is independent when i<nλivi=0V\sum_{i<n} \lambda_i v_i = 0_V forces every λi=0F\lambda_i = 0_F, and a subset SVS \subseteq V is independent when every injective finite list into SS is independent), hence a basis of EE (Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis), and kekk \mapsto e_k is a bijection NB\mathbb{N} \to B, so BNB \approx \mathbb{N} (Equinumerous sets, ABA \approx B and ABA \preceq B);
  4. EE is infinite-dimensional over FF (Finite-dimensional vector space, and its dimension dimFV\dim_F V; infinite-dimensional means having no finite basis): it has no finite basis.

No choice principle is used anywhere below: the basis is written down.

Facts & Assumptions

Given: A field FF, the vector space FNF^{\mathbb{N}} with pointwise operations, the set EE of eventually zero families, the families eke_k, and B={ek:kN}B = \{\, e_k : k \in \mathbb{N}\,\}.

[L1]

FXF^{X} is a vector space over FF with (x+y)(n)=x(n)+y(n)(x+y)(n) = x(n)+y(n), (λx)(n)=λx(n)(\lambda x)(n) = \lambda\,x(n) and zero the constant family at 0F0_F; two elements are equal exactly when they agree at every point (The vector space FXF^{X} of all functions XFX \to F with pointwise operations, and FnF^{n} as the case X=n={0,1,,n1}X = n = \{0, 1, \dots, n-1\}, Vector space over a field).

[L2]

One-step test: a nonempty WVW \subseteq V with λu+vW\lambda u + v \in W for all λF\lambda \in F, u,vWu, v \in W is a linear subspace; a linear subspace is a vector space in its own right, and independence and spans of its subsets agree with those computed in the ambient space (One-step subspace test: a nonempty WVW \subseteq V is a linear subspace if and only if λu+vW\lambda u + v \in W for all λF\lambda \in F and u,vWu, v \in W, Linear subspace of a vector space, Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis, section on bases of a linear subspace).

[L4]

A finite sum in a function space is pointwise: (k<puk)(n)=k<puk(n)\bigl(\sum_{k<p}u_k\bigr)(n) = \sum_{k<p}u_k(n) (The standard list e:nFne : n \to F^{n} with ei(i)=1Fe_i(i) = 1_F and ei(j)=0Fe_i(j) = 0_F for jij \ne i is an ordered basis of FnF^{n}; hence dimFFn=n\dim_F F^{n} = n, and F0F^{0} is the zero space with basis \varnothing and dimension 00, claim 1). Finite sums obey k<0uk=0\sum_{k<0}u_k = 0 and k<σ(p)uk=(k<puk)+up\sum_{k<\sigma(p)}u_k = \bigl(\sum_{k<p}u_k\bigr) + u_p (The product g0g1gn1g_0 g_1 \cdots g_{n-1} of a finite list in a monoid, by recursion, with the empty product (n=0n = 0) equal to the identity).

[L5]

FF is a vector space over itself (A field is a vector space over itself, and over any subfield KFK \subseteq F every FF-vector space is a KK-vector space by restricting the scalars, claim 1), so (F1) and (F3) apply to lists of scalars: an all-0F0_F list sums to 0F0_F, and a list vanishing off a single index sums to its value at that index (The sum U+WU + W of two linear subspaces and the sum i<nUi\sum_{i<n} U_i of a finite family).

[L9]

The order of N\mathbb{N} is total, m<σ(N)    mNm < \sigma(N) \iff m \le N, and m<nm < n implies mnm \ne n (\le is a linear order on N\mathbb{N}, Order on the natural numbers, On N\mathbb{N} the order is membership: m<n    mnm < n \iff m \in n); induction (The principle of mathematical induction); injectivity and images (Injection, surjection, bijection).

Verification

technique · direct
1.1

Claim 1. EE is nonempty: the zero family has value 0F0_F everywhere, so N=0N = 0 witnesses that it lies in EE. And EE is closed under the one-step expression: for λF\lambda \in F and u,vEu, v \in E with witnesses N1N_1 and N2N_2, let NN be the larger of the two, which exists because the order of N\mathbb{N} is total; then for nNn \ge N we have nN1n \ge N_1 and nN2n \ge N_2, so (λu+v)(n)=λu(n)+v(n)=λ0F+0F=0F(\lambda u + v)(n) = \lambda u(n) + v(n) = \lambda 0_F + 0_F = 0_F, and NN witnesses λu+vE\lambda u + v \in E. So EE is a linear subspace of FNF^{\mathbb{N}} by the one-step test.

L1L2L6L9
1.2

Each eke_k lies in EE, so BEB \subseteq E: if nσ(k)n \ge \sigma(k) then k<nk < n, hence nkn \ne k and ek(n)=0Fe_k(n) = 0_F, so σ(k)\sigma(k) is a witness.

L9
1.3

For xFNx \in F^{\mathbb{N}} and NNN \in \mathbb{N} put sN:=k<Nx(k)eks_N := \sum_{k<N} x(k)\,e_k. Then sN(n)=x(n)s_N(n) = x(n) for n<Nn < N and sN(n)=0Fs_N(n) = 0_F for nNn \ge N. Indeed sN(n)=k<N(x(k)ek)(n)=k<Nx(k)ek(n)s_N(n) = \sum_{k<N}\bigl(x(k)e_k\bigr)(n) = \sum_{k<N} x(k)\,e_k(n) by pointwise evaluation and pointwise scalar multiplication; the scalar list kx(k)ek(n)k \mapsto x(k)e_k(n) has the value x(k)0F=0Fx(k)0_F = 0_F at every knk \ne n. If n<Nn < N this list vanishes off the single index nn, where its value is x(n)1F=x(n)x(n)1_F = x(n), so the sum is x(n)x(n); if nNn \ge N then no k<Nk < N equals nn, the list is all 0F0_F, and the sum is 0F0_F.

L1L4L5L6L9
1.4

Claim 3, independence. The map kekk \mapsto e_k is injective, since ek(k)=1F0F=el(k)e_k(k) = 1_F \ne 0_F = e_l(k) for lkl \ne k. Let w:mBw : m \to B be an injective finite list and λ:mF\lambda : m \to F with j<mλjwj=0\sum_{j<m}\lambda_j w_j = 0 in FNF^{\mathbb{N}}. Each wjw_j is eije_{i_j} for exactly one ijNi_j \in \mathbb{N}, and jijj \mapsto i_j is injective because ww is. Fix j<mj < m and evaluate at iji_j: pointwise evaluation gives 0F=l<mλleil(ij)0_F = \sum_{l<m}\lambda_l\,e_{i_l}(i_j), and eil(ij)=0Fe_{i_l}(i_j) = 0_F unless il=iji_l = i_j, that is unless l=jl = j, where it is 1F1_F. So the scalar list vanishes off the single index jj and sums to λj1F=λj\lambda_j 1_F = \lambda_j, giving λj=0F\lambda_j = 0_F. Hence every injective finite list into BB is independent, that is BB is linearly independent.

L1L4L5L6L7L9
2.1

BNB \approx \mathbb{N}: the map kekk \mapsto e_k is injective by step 1.4 and its image is BB by definition, so it is a bijection NB\mathbb{N} \to B.

step 1.4L9
2.2

Claim 2. Each eke_k lies in EE and EE is a linear subspace, so span(B)E\operatorname{span}(B) \subseteq E by minimality of the span. Conversely let xEx \in E with witness NN; then xx and sNs_N of step 1.3 agree at every nn, since for n<Nn < N both take the value x(n)x(n) and for nNn \ge N both take the value 0F0_F, so x=sN=k<Nx(k)ekx = s_N = \sum_{k<N} x(k)e_k, a linear combination of elements of BB. Hence Espan(B)E \subseteq \operatorname{span}(B).

step 1.1step 1.2step 1.3L1L3
3.1

Claim 4. Suppose EE had a finite basis CC, say with pp elements. Then CC is a spanning set of EE with pp elements, so no linearly independent subset of EE is equinumerous with N\mathbb{N}. But BEB \subseteq E is linearly independent by step 1.4 and BNB \approx \mathbb{N} by step 2.1. So no finite basis exists and EE is infinite-dimensional over FF.

step 1.4step 2.1L8
4.1

Claim 3, that BB is a basis of EE. By step 1.4 the set BB is linearly independent and by step 2.2 it spans EE; independence and spans computed in the linear subspace EE agree with those computed in FNF^{\mathbb{N}}, so BB is a basis of the vector space EE.

step 1.4step 2.2L2

Remarks

ExampleConstruction: AI-adaptedVerification: AI-generatedprecheck passjudge pass (deepseek-v4-pro + gpt-5.6-terra)verified 2026-08-03 (gpt-5.6-sol-codex-subscription)Open item page →

R\mathbb{R} as a vector space over Q\mathbb{Q} has a basis, and every such basis is infinite; the existence proof exhibits none

Example

Assume the Axiom of Choice (The Axiom of Choice). Let R\mathbb{R} be the real numbers (The real numbers), a field (The reals form a field) and an ordered field (The reals form a totally ordered field, Ordered field), with the least-upper-bound property and hence complete as an ordered field (The Cauchy-sequence reals have the least-upper-bound property, Complete ordered field (least-upper-bound property)), and let Q\mathbb{Q} be the rationals (The rationals as equivalence classes of pairs of integers), a field (The rationals form a field). Let ι:QR\iota : \mathbb{Q} \to \mathbb{R} be the unique field homomorphism (The unique embedding of ℚ into an ordered field, Field homomorphism and embedding), which is injective, and put QR:=ι[Q]\mathbb{Q}_{\mathbb{R}} := \iota[\mathbb{Q}]. Then:

  1. QR\mathbb{Q}_{\mathbb{R}} is a subfield of R\mathbb{R} (Subfield: a subring of a field closed under inverses of its nonzero elements, and therefore a field with the restricted operations) and R\mathbb{R} is a vector space over QR\mathbb{Q}_{\mathbb{R}} by restriction of scalars (A field is a vector space over itself, and over any subfield KFK \subseteq F every FF-vector space is a KK-vector space by restricting the scalars); setting qx:=ι(q)xq \cdot x := \iota(q)\,x also makes R\mathbb{R} a vector space over Q\mathbb{Q} itself;
  2. R\mathbb{R} has a basis over QR\mathbb{Q}_{\mathbb{R}} (Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis, Every vector space has a basis);
  3. R\mathbb{R} is infinite-dimensional over QR\mathbb{Q}_{\mathbb{R}} (Finite-dimensional vector space, and its dimension dimFV\dim_F V; infinite-dimensional means having no finite basis): no basis of R\mathbb{R} over QR\mathbb{Q}_{\mathbb{R}} is finite;
  4. the two structures of claim 1 have the same linearly independent subsets, the same spans and the same bases, so claims 2 and 3 hold verbatim for R\mathbb{R} as a Q\mathbb{Q}-vector space.

The existence proof exhibits no basis. Claim 2 comes from Every vector space has a basis, which runs through Zorn's lemma and therefore through the Axiom of Choice; nothing in it names a real number belonging to the basis it produces. That is a statement about this proof. It is not claimed here that no basis can be exhibited by any means: that would be a metamathematical assertion about what is definable, and this library has established nothing of the kind.

Facts & Assumptions

Given: The Axiom of Choice; the complete ordered field R\mathbb{R}, the field Q\mathbb{Q}, the unique field homomorphism ι:QR\iota : \mathbb{Q} \to \mathbb{R}, and QR=ι[Q]\mathbb{Q}_{\mathbb{R}} = \iota[\mathbb{Q}].

[L1]

There is a unique field homomorphism ι:QR\iota : \mathbb{Q} \to \mathbb{R} and it is injective (The unique embedding of ℚ into an ordered field); a field homomorphism satisfies φ(x+y)=φ(x)+φ(y)\varphi(x+y) = \varphi(x)+\varphi(y), φ(xy)=φ(x)φ(y)\varphi(xy) = \varphi(x)\varphi(y), φ(1)=1\varphi(1) = 1, φ(0)=0\varphi(0) = 0, φ(x)=φ(x)\varphi(-x) = -\varphi(x) and φ(x1)=φ(x)1\varphi(x^{-1}) = \varphi(x)^{-1} for x0x \ne 0 (Field homomorphism and embedding); a subfield is a subset containing 11, closed under aba - b and abab, and containing x1x^{-1} for each nonzero xx in it (Subfield: a subring of a field closed under inverses of its nonzero elements, and therefore a field with the restricted operations).

[L2]

A field is a vector space over itself, and an FF-vector space is a KK-vector space for every subfield KFK \subseteq F by restricting the scalar multiplication (A field is a vector space over itself, and over any subfield KFK \subseteq F every FF-vector space is a KK-vector space by restricting the scalars, Vector space over a field, Field).

[L5]

QN\mathbb{Q} \approx \mathbb{N} (Q\mathbb{Q} is countably infinite); a product of two at most countable sets is at most countable (A product of two at most countable sets is at most countable); a subset of an at most countable set is at most countable (Every subset of an at most countable set is at most countable); the Cauchy-sequence reals have the least-upper-bound property and hence form a complete ordered field (The Cauchy-sequence reals have the least-upper-bound property, Complete ordered field (least-upper-bound property)), so R\mathbb{R} is uncountable (R\mathbb{R} is uncountable (Cantor's nested intervals, 1874)); a finite set is equinumerous with exactly one natural (The pigeonhole principle on N\mathbb{N}); "at most countable" means finite or equinumerous with N\mathbb{N}, and this property transfers along a bijection (Finite, countably infinite, countable, uncountable, Equinumerous sets, ABA \approx B and ABA \preceq B, Injection, surjection, bijection).

Verification

technique · direct
1.1

Claim 1. QR=ι[Q]\mathbb{Q}_{\mathbb{R}} = \iota[\mathbb{Q}] is a subfield of R\mathbb{R}: it contains ι(1)=1\iota(1) = 1; for p,qQp, q \in \mathbb{Q} it contains ι(p)ι(q)=ι(pq)\iota(p) - \iota(q) = \iota(p-q) and ι(p)ι(q)=ι(pq)\iota(p)\iota(q) = \iota(pq); and if ι(q)0\iota(q) \ne 0 then q0q \ne 0, since ι(0)=0\iota(0) = 0, so ι(q)1=ι(q1)QR\iota(q)^{-1} = \iota(q^{-1}) \in \mathbb{Q}_{\mathbb{R}}. Since R\mathbb{R} is a vector space over itself, restriction of scalars makes it a vector space over QR\mathbb{Q}_{\mathbb{R}}, with the field multiplication restricted to QR×R\mathbb{Q}_{\mathbb{R}} \times \mathbb{R}. The operation (q,x)ι(q)x(q,x) \mapsto \iota(q)x is a map Q×RR\mathbb{Q} \times \mathbb{R} \to \mathbb{R}, and it satisfies (V2) to (V5) because ι\iota preserves sums and products and ι(1)=1\iota(1) = 1, while (V1) is the abelian group (R,+,0)(\mathbb{R},+,0); so it makes R\mathbb{R} a vector space over Q\mathbb{Q}.

L1L2
1.2

QR\mathbb{Q}_{\mathbb{R}} is at most countable: ι\iota is injective with image QR\mathbb{Q}_{\mathbb{R}}, hence a bijection QQR\mathbb{Q} \to \mathbb{Q}_{\mathbb{R}}, and QN\mathbb{Q} \approx \mathbb{N}; composing bijections gives QRN\mathbb{Q}_{\mathbb{R}} \approx \mathbb{N}.

L1L5
1.3

If KK is at most countable then so is KnK^{n}, the set of functions nKn \to K, for every nNn \in \mathbb{N}. By induction on nn: at n=0n = 0 the set K0K^{0} has exactly one element, the empty function, so it is finite; and the map Kσ(n)Kn×KK^{\sigma(n)} \to K^{n} \times K sending ff to the pair consisting of its restriction to nn and its value at nn is a bijection, since σ(n)=n{n}\sigma(n) = n \cup \{n\} and nnn \notin n, so a function on σ(n)\sigma(n) is determined by, and may be assembled from, those two data. Hence Kσ(n)Kn×KK^{\sigma(n)} \approx K^{n} \times K, which is at most countable by the inductive hypothesis and the product theorem, and countability transfers along the bijection.

L5L6
1.4

Claim 4. For a list v:nRv : n \to \mathbb{R} and scalars λ:nQ\lambda : n \to \mathbb{Q}, the vector i<nλivi\sum_{i<n}\lambda_i \cdot v_i computed in the Q\mathbb{Q}-structure is by definition i<nι(λi)vi\sum_{i<n}\iota(\lambda_i)v_i, computed in the QR\mathbb{Q}_{\mathbb{R}}-structure; the two structures have the same underlying set, the same addition and the same zero, so their finite sums agree. Since ι\iota is a bijection QQR\mathbb{Q} \to \mathbb{Q}_{\mathbb{R}}, the scalar lists λ:nQ\lambda : n \to \mathbb{Q} and ιλ:nQR\iota \circ \lambda : n \to \mathbb{Q}_{\mathbb{R}} correspond bijectively, and λi=0\lambda_i = 0 for all ii exactly when ι(λi)=0\iota(\lambda_i) = 0 for all ii. So a vanishing combination exists on one side exactly when it does on the other, and likewise for representations of an arbitrary vector; hence the two structures have the same linearly independent subsets, the same spans and the same bases.

L1L3L4
2.1

Claim 2. R\mathbb{R} is a vector space over QR\mathbb{Q}_{\mathbb{R}} by step 1.1, and every vector space has a basis, so a basis BB of R\mathbb{R} over QR\mathbb{Q}_{\mathbb{R}} exists.

step 1.1L3
2.2

Claim 3. Suppose some basis BB of R\mathbb{R} over QR\mathbb{Q}_{\mathbb{R}} were finite, say BnB \approx n. A bijection nBn \to B is an injective list whose image is a basis, hence an ordered basis, so every xRx \in \mathbb{R} is i<nλibi\sum_{i<n}\lambda_i b_i for exactly one λ:nQR\lambda : n \to \mathbb{Q}_{\mathbb{R}}. The resulting map Φ:R(QR)n\Phi : \mathbb{R} \to (\mathbb{Q}_{\mathbb{R}})^{n}, sending xx to that λ\lambda, is injective, since Φ(x)=Φ(y)\Phi(x) = \Phi(y) makes xx and yy the same sum. By steps 1.2 and 1.3 the set (QR)n(\mathbb{Q}_{\mathbb{R}})^{n} is at most countable, hence so is its subset Φ[R]\Phi[\mathbb{R}]; and Φ\Phi is a bijection RΦ[R]\mathbb{R} \to \Phi[\mathbb{R}], so R\mathbb{R} is at most countable, contradicting the uncountability of R\mathbb{R}. So no basis of R\mathbb{R} over QR\mathbb{Q}_{\mathbb{R}} is finite, and R\mathbb{R} is infinite-dimensional over QR\mathbb{Q}_{\mathbb{R}}.

step 1.1step 1.2step 1.3L3L4L5
3.1

Claim 1 is step 1.1, claim 2 is step 2.1, claim 3 is step 2.2, and claim 4 is step 1.4; by claim 4 the last two transfer to R\mathbb{R} as a Q\mathbb{Q}-vector space.

step 1.1step 1.4step 2.1step 2.2

Remarks

CounterexampleConstruction: AI-adaptedVerification: AI-generatedprecheck passjudge pass (z-ai/glm-5.2)audited 2026-07-28Open item page →

The standard unit families {ei:iN}\{\, e_i : i \in \mathbb{N} \,\} are linearly independent in FNF^{\mathbb{N}} but do not span it: the constant family 1F1_F is not a finite linear combination of them

Statement refuted

False claim: if VV is an infinite-dimensional vector space over a field FF (Finite-dimensional vector space, and its dimension dimFV\dim_F V; infinite-dimensional means having no finite basis) and BVB \subseteq V is a linearly independent subset that is not finite, then span(B)=V\operatorname{span}(B) = V.

Take FF any field, V:=FNV := F^{\mathbb{N}} the function space of all families x:NFx : \mathbb{N} \to F with the pointwise operations (The vector space FXF^{X} of all functions XFX \to F with pointwise operations, and FnF^{n} as the case X=n={0,1,,n1}X = n = \{0, 1, \dots, n-1\}), and B:={ei:iN}B := \{\, e_i : i \in \mathbb{N} \,\} the standard unit families, where ei(i)=1Fe_i(i) = 1_F and ei(n)=0Fe_i(n) = 0_F for nin \ne i. Then BB is linearly independent and not finite, VV is infinite-dimensional, and yet span(B)=E\operatorname{span}(B) = E, the linear subspace of eventually zero families, which is not all of VV: the constant family cc with c(n)=1Fc(n) = 1_F for every nn lies outside it.

So BB is an infinite linearly independent set that is not a basis of VV (Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis), although it is a basis of EE.

Facts & Assumptions

Given: A field FF, the vector space FNF^{\mathbb{N}}, the set EE of eventually zero families, the families eie_i, and B={ei:iN}B = \{\, e_i : i \in \mathbb{N} \,\} as above.

[L1]

EE is a linear subspace of FNF^{\mathbb{N}}; BEB \subseteq E and span(B)=E\operatorname{span}(B) = E; BB is linearly independent; and BNB \approx \mathbb{N} (The standard unit families ekFNe_k \in F^{\mathbb{N}} form a basis of the linear subspace of eventually zero families: an explicit infinite basis, built with no choice principle, claims 1, 2 and 3).

[L3]

N≉p\mathbb{N} \not\approx p for every pNp \in \mathbb{N} (The pigeonhole principle on N\mathbb{N}, claim 4); a set is finite when it is equinumerous with some natural number; \approx is symmetric and transitive (Finite, countably infinite, countable, uncountable, Equinumerous sets, ABA \approx B and ABA \preceq B).

Counterexample

technique · direct
1.1

BB is linearly independent, span(B)=E\operatorname{span}(B) = E, and BNB \approx \mathbb{N}.

L1
1.2

BB is not finite: if BpB \approx p for some pNp \in \mathbb{N} then, since BNB \approx \mathbb{N}, symmetry and transitivity of \approx would give Np\mathbb{N} \approx p, which is impossible.

L1L3
1.3

The constant family cc with c(n)=1Fc(n) = 1_F for every nn lies in FNF^{\mathbb{N}} and not in EE: for any candidate witness NN we have NNN \ge N and c(N)=1F0Fc(N) = 1_F \ne 0_F, so no NN witnesses that cc is eventually zero.

L2L5
1.4

FNF^{\mathbb{N}} is infinite-dimensional. If it had a finite basis, that basis would be a spanning set with pp elements for some pp, and then no linearly independent subset of FNF^{\mathbb{N}} would be equinumerous with N\mathbb{N}; but BB is such a subset.

L1L4
2.1

So BB is a linearly independent subset of the infinite-dimensional space FNF^{\mathbb{N}}, it is not finite, and span(B)=EFN\operatorname{span}(B) = E \ne F^{\mathbb{N}}, since cc lies in the second and not the first. The false claim therefore fails, and BB is not a basis of FNF^{\mathbb{N}}, its span not being the whole space.

step 1.1step 1.2step 1.3step 1.4

Remarks

CounterexampleConstruction: AI-adaptedVerification: AI-generatedprecheck passjudge pass (z-ai/glm-5.2)audited 2026-07-28Open item page →

{(1,0),(0,1),(1,1)}\{(1,0), (0,1), (1,1)\} spans F2F^{2} and is linearly dependent, so a spanning set need not be a basis; each of its three two-element subsets is a basis

Statement refuted

False claim: a spanning subset of a vector space is linearly independent, and hence a basis.

Let FF be any field (Field) and let F2F^{2} be the function space on 2={0,1}2 = \{0,1\} (The vector space FXF^{X} of all functions XFX \to F with pointwise operations, and FnF^{n} as the case X=n={0,1,,n1}X = n = \{0, 1, \dots, n-1\}), whose elements we write (y0,y1)(y_0,y_1). Put

e0:=(1F,0F),e1:=(0F,1F),d:=(1F,1F)=e0+e1,e_0 := (1_F, 0_F), \qquad e_1 := (0_F, 1_F), \qquad d := (1_F, 1_F) = e_0 + e_1,

and S:={e0,e1,d}S := \{e_0, e_1, d\}, a set with exactly three elements. Then

  1. span(S)=F2\operatorname{span}(S) = F^{2};
  2. SS is linearly dependent (Linear independence: a finite list v:nVv : n \to V is independent when i<nλivi=0V\sum_{i<n} \lambda_i v_i = 0_V forces every λi=0F\lambda_i = 0_F, and a subset SVS \subseteq V is independent when every injective finite list into SS is independent), so SS is not a basis of F2F^{2} (Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis);
  3. each of the three two-element subsets {e0,e1}\{e_0,e_1\}, {e0,d}\{e_0,d\}, {e1,d}\{e_1,d\} is a basis of F2F^{2}.

The field is arbitrary; over a field in which 1F+1F=0F1_F + 1_F = 0_F the identity 1F=1F-1_F = 1_F holds and changes nothing below, the three displayed vectors still being distinct because 1F0F1_F \ne 0_F.

Facts & Assumptions

Given: A field FF, the vector space F2F^{2} with pointwise operations, and the vectors e0e_0, e1e_1, d=e0+e1d = e_0+e_1 and the set S={e0,e1,d}S = \{e_0,e_1,d\}.

[L1]

e:2F2e : 2 \to F^{2} is an ordered basis of F2F^{2}, e[2]={e0,e1}e[2] = \{e_0,e_1\} is a basis, (i<2λiei)(j)=λj\bigl(\sum_{i<2}\lambda_i e_i\bigr)(j) = \lambda_j, and dimFF2=2\dim_F F^{2} = 2 (The standard list e:nFne : n \to F^{n} with ei(i)=1Fe_i(i) = 1_F and ei(j)=0Fe_i(j) = 0_F for jij \ne i is an ordered basis of FnF^{n}; hence dimFFn=n\dim_F F^{n} = n, and F0F^{0} is the zero space with basis \varnothing and dimension 00, claims 2, 3 and 4).

[L5]

(V,+,0V)(V,+,0_V) is an abelian group; 1Fy=y1_F y = y, (1F)y=y(-1_F)y = -y, 0Fy=0V0_F y = 0_V; (V2) and (V3); and 1F0F1_F \ne 0_F, with 1F0F-1_F \ne 0_F (Vector space over a field, In any vector space 0Fv=0V0_F v = 0_V, λ0V=0V\lambda 0_V = 0_V, (λ)v=(λv)(-\lambda)v = -(\lambda v), (1F)v=v(-1_F)v = -v, and λv=0V\lambda v = 0_V forces λ=0F\lambda = 0_F or v=0Vv = 0_V, Field).

Counterexample

technique · direct
1.1

SS has exactly three elements. e0e1e_0 \ne e_1 because their values at 00 are 1F1_F and 0F0_F; e0de_0 \ne d because their values at 11 are 0F0_F and 1F1_F; and e1de_1 \ne d because their values at 00 are 0F0_F and 1F1_F. All three inequalities use only 1F0F1_F \ne 0_F.

L5L7
1.2

Claim 1. From {e0,e1}S\{e_0,e_1\} \subseteq S and monotonicity, F2=span{e0,e1}span(S)F2F^{2} = \operatorname{span}\{e_0,e_1\} \subseteq \operatorname{span}(S) \subseteq F^{2}, so span(S)=F2\operatorname{span}(S) = F^{2}.

L1L3
1.3

The pair (e0,d)(e_0, d) is an ordered basis. For λ:2F\lambda : 2 \to F, i<2λivi\sum_{i<2}\lambda_i v_i with v0=e0v_0 = e_0, v1=dv_1 = d is λ0e0+λ1(e0+e1)=(λ0+λ1)e0+λ1e1\lambda_0 e_0 + \lambda_1(e_0+e_1) = (\lambda_0 + \lambda_1)e_0 + \lambda_1 e_1 by (V2), (V3) and the abelian group laws, which evaluates to (λ0+λ1, λ1)(\lambda_0+\lambda_1,\ \lambda_1). Given y=(y0,y1)y = (y_0,y_1), the equations λ0+λ1=y0\lambda_0 + \lambda_1 = y_0 and λ1=y1\lambda_1 = y_1 have the unique solution λ1=y1\lambda_1 = y_1, λ0=y0y1\lambda_0 = y_0 - y_1; so every yy has exactly one representation and (e0,d)(e_0,d) is an ordered basis, whence {e0,d}\{e_0, d\} is a basis of F2F^{2}.

L1L2L4L5
1.4

The pair (e1,d)(e_1, d) is an ordered basis. Likewise λ0e1+λ1d=λ1e0+(λ0+λ1)e1\lambda_0 e_1 + \lambda_1 d = \lambda_1 e_0 + (\lambda_0 + \lambda_1)e_1 evaluates to (λ1, λ0+λ1)(\lambda_1,\ \lambda_0 + \lambda_1), and λ1=y0\lambda_1 = y_0, λ0=y1y0\lambda_0 = y_1 - y_0 is the unique solution; so {e1,d}\{e_1, d\} is a basis of F2F^{2}.

L1L2L4L5
2.1

Claim 2. The list v:3Sv : 3 \to S with v0=e0v_0 = e_0, v1=e1v_1 = e_1, v2=dv_2 = d is injective by step 1.1, and with λ0=λ1=1F\lambda_0 = \lambda_1 = 1_F and λ2=1F\lambda_2 = -1_F we get i<3λivi=((0V+1Fe0)+1Fe1)+(1F)d=(e0+e1)+(d)=d+(d)=0V\sum_{i<3}\lambda_i v_i = ((0_V + 1_F e_0) + 1_F e_1) + (-1_F)d = (e_0 + e_1) + (-d) = d + (-d) = 0_V, while λ0=1F0F\lambda_0 = 1_F \ne 0_F. So vv is a dependent injective list into SS and SS is linearly dependent; a basis is independent, so SS is not a basis of F2F^{2}.

step 1.1L4L5L6
3.1

Claim 3, and the conclusion. {e0,e1}\{e_0,e_1\} is a basis by the standard basis lemma, and {e0,d}\{e_0,d\} and {e1,d}\{e_1,d\} are bases by steps 1.3 and 1.4; these are the three two-element subsets of the three-element set SS of step 1.1. Together with step 1.2 and step 2.1, the set SS spans F2F^{2} and is dependent, refuting the false claim.

step 1.1step 1.2step 1.3step 1.4step 2.1L1

Remarks

CounterexampleConstruction: AI-adaptedVerification: AI-generatedprecheck passverified 2026-08-03 (gpt-5.6-sol-codex-subscription)Open item page →

Inside the space of eventually zero families, the linear subspace spanned by {ei:i1}\{\, e_i : i \ge 1 \,\} is proper and has a basis equinumerous with a basis of the whole space, so "equal dimension forces equality" fails without finite dimension

Statement refuted

False claim: if UU is a linear subspace of a vector space VV over FF and some basis of UU is equinumerous with some basis of VV, then U=VU = V.

Let FF be any field, let EFNE \subseteq F^{\mathbb{N}} be the linear subspace of eventually zero families and let eke_k be the standard unit families (The standard unit families ekFNe_k \in F^{\mathbb{N}} form a basis of the linear subspace of eventually zero families: an explicit infinite basis, built with no choice principle). Put

B:={ek:kN},B:={ek:kN, k1},U:=span(B).B := \{\, e_k : k \in \mathbb{N} \,\}, \qquad B' := \{\, e_k : k \in \mathbb{N},\ k \ge 1 \,\}, \qquad U := \operatorname{span}(B') .

Then

  1. UU is a linear subspace of EE and BB' is a basis of UU, while BB is a basis of EE;
  2. BBB' \approx B (Equinumerous sets, ABA \approx B and ABA \preceq B), both being equinumerous with N\mathbb{N};
  3. UEU \ne E: the family e0e_0 lies in EE and not in UU.

So a proper linear subspace can carry a basis equinumerous with a basis of the whole space, and the equality clause of If dimFV=n\dim_F V = n and UU is a linear subspace of VV, then UU is finite-dimensional, dimFUn\dim_F U \le n, and dimFU=n\dim_F U = n if and only if U=VU = V — which is stated only for a finite-dimensional ambient space — really does need its hypothesis.

No dimension is assigned to either space. EE and UU are both infinite-dimensional (Finite-dimensional vector space, and its dimension dimFV\dim_F V; infinite-dimensional means having no finite basis assigns no number to such a space): for EE this is claim 4 of The standard unit families ekFNe_k \in F^{\mathbb{N}} form a basis of the linear subspace of eventually zero families: an explicit infinite basis, built with no choice principle, and for UU it follows from claims 1 and 2 below, since the basis BB' of UU is linearly independent and equinumerous with N\mathbb{N}, so UU can have no finite spanning set and hence no finite basis, by claim 2 of If VV has a spanning set with nn elements, then every linearly independent subset of VV is finite with at most nn elements; in particular VV has no linearly independent subset equinumerous with N\mathbb{N}. And claim 2 compares two specific bases through an explicit bijection, not two cardinal numbers.

Facts & Assumptions

Given: A field FF, the vector space FNF^{\mathbb{N}}, the subspace EE of eventually zero families, the families eke_k, and the sets BB, BB' and U=span(B)U = \operatorname{span}(B') as above.

[L1]

EE is a linear subspace of FNF^{\mathbb{N}}; BEB \subseteq E; span(B)=E\operatorname{span}(B) = E; BB is linearly independent and is a basis of EE; kekk \mapsto e_k is a bijection NB\mathbb{N} \to B; and EE is infinite-dimensional (The standard unit families ekFNe_k \in F^{\mathbb{N}} form a basis of the linear subspace of eventually zero families: an explicit infinite basis, built with no choice principle, claims 1 to 4).

Counterexample

technique · direct
1.1

BBEB' \subseteq B \subseteq E, so BB' is linearly independent, and U=span(B)U = \operatorname{span}(B') is a linear subspace of FNF^{\mathbb{N}} contained in EE, hence a linear subspace of EE; since BB' is independent and spans UU by definition, BB' is a basis of UU.

L1L2L3L4
1.2

Claim 2. The map keσ(k)k \mapsto e_{\sigma(k)} is a bijection NB\mathbb{N} \to B': it is injective, being the composite of the injective σ\sigma with the injective kekk \mapsto e_k, and every element of BB' is eje_j with j0j \ne 0, hence eσ(k)e_{\sigma(k)} for the unique kk with σ(k)=j\sigma(k) = j. So BNB' \approx \mathbb{N}, and BNB \approx \mathbb{N} as well, whence BBB' \approx B by symmetry and transitivity of \approx.

L1L7
1.3

Every xUx \in U satisfies x(0)=0Fx(0) = 0_F. Indeed x=l<pλlwlx = \sum_{l<p}\lambda_l w_l for some pp, some λ:pF\lambda : p \to F and some w:pBw : p \to B'; evaluating pointwise at 00 gives x(0)=l<pλlwl(0)x(0) = \sum_{l<p}\lambda_l\,w_l(0), and each wlw_l is ejle_{j_l} with jl1j_l \ge 1, so wl(0)=0Fw_l(0) = 0_F and λlwl(0)=0F\lambda_l w_l(0) = 0_F; a list of scalars all equal to 0F0_F sums to 0F0_F.

L3L5L6
2.1

Claim 3. The family e0e_0 lies in EE and e0(0)=1F0Fe_0(0) = 1_F \ne 0_F, so by step 1.3 it does not lie in UU; hence UEU \ne E, and UU is a proper linear subspace of EE.

step 1.3L1L6
3.1

Steps 1.1, 1.2 and 2.1 give claims 1, 2 and 3: UU is a proper linear subspace of EE, BB' is a basis of UU, BB is a basis of EE, and BBB' \approx B. So a basis of a proper subspace can be equinumerous with a basis of the whole space, refuting the false claim.

step 1.1step 1.2step 2.1

Remarks

  • The finite case is a theorem, and this shows why it is one. If dimFV=n\dim_F V = n and UU is a linear subspace of VV, then UU is finite-dimensional, dimFUn\dim_F U \le n, and dimFU=n\dim_F U = n if and only if U=VU = V proves that in a finite-dimensional ambient space equality of dimensions forces equality of the spaces; its proof enlarges a basis of the subspace by a vector outside it and contradicts the bound on independent sets. Here the same enlargement is possible — B{e0}=BB' \cup \{e_0\} = B is independent — and contradicts nothing, because there is no finite bound to violate.

  • No cardinal arithmetic is used or implied. The comparison in claim 2 is a named bijection, keσ(k)k \mapsto e_{\sigma(k)}, between two specific sets. This item does not assign a dimension to EE or to UU, and it says nothing about whether any two bases of EE are equinumerous; that question needs cardinal arithmetic, which is not available at this point in the reading order.

  • The subspace is spanned by "all but one" basis vector. Deleting a single element from an infinite basis leaves a set that is still equinumerous with the original, which is exactly the phenomenon The pigeonhole principle on N\mathbb{N} rules out for finite sets and for natural numbers.

CounterexampleConstruction: AI-adaptedVerification: AI-generatedprecheck passjudge pass (z-ai/glm-5.2)audited 2026-07-28Open item page →

Three distinct lines U0,U1,U2U_0, U_1, U_2 in F2F^{2} have dimF(U0+U1+U2)=2\dim_F(U_0+U_1+U_2) = 2 while the inclusion-exclusion analogue of the dimension formula predicts 33, so the two-subspace formula does not extend

Statement refuted

False claim: for finite-dimensional linear subspaces U0,U1,U2U_0, U_1, U_2 of a vector space VV over FF,

dimF(j<3Uj)+dimF(U0U1)+dimF(U0U2)+dimF(U1U2)  =  dimFU0+dimFU1+dimFU2+dimF(U0U1U2).\dim_F\Bigl(\sum_{j<3}U_j\Bigr) + \dim_F(U_0 \cap U_1) + \dim_F(U_0 \cap U_2) + \dim_F(U_1 \cap U_2) \;=\; \dim_F U_0 + \dim_F U_1 + \dim_F U_2 + \dim_F(U_0 \cap U_1 \cap U_2).

This is the inclusion-exclusion analogue of The dimension formula: for finite-dimensional linear subspaces UU and WW of VV, the subspaces U+WU + W and UWU \cap W are finite-dimensional and dimF(U+W)+dimF(UW)=dimFU+dimFW\dim_F(U+W) + \dim_F(U \cap W) = \dim_F U + \dim_F W, written without subtraction so that both sides are natural numbers; for two subspaces the same rearrangement is exactly that theorem.

Let FF be any field, let F2F^{2} be the function space on 2={0,1}2 = \{0,1\} (The vector space FXF^{X} of all functions XFX \to F with pointwise operations, and FnF^{n} as the case X=n={0,1,,n1}X = n = \{0, 1, \dots, n-1\}) with e0=(1F,0F)e_0 = (1_F,0_F), e1=(0F,1F)e_1 = (0_F,1_F) and d:=e0+e1=(1F,1F)d := e_0 + e_1 = (1_F,1_F), and put

U0:=span{e0},U1:=span{e1},U2:=span{d}.U_0 := \operatorname{span}\{e_0\}, \qquad U_1 := \operatorname{span}\{e_1\}, \qquad U_2 := \operatorname{span}\{d\} .

Then dimFUj=1\dim_F U_j = 1 for each jj, all three pairwise intersections and the triple intersection equal {0V}\{0_V\} and so have dimension 00, and j<3Uj=F2\sum_{j<3}U_j = F^{2} has dimension 22. The left-hand side is 2+0+0+0=22 + 0 + 0 + 0 = 2 and the right-hand side is 1+1+1+0=31 + 1 + 1 + 0 = 3, so the claimed identity fails.

The three sets are called lines informally, as on the order-69 examples page; the word carries no separate definition here.

Facts & Assumptions

Given: A field FF, the vector space F2F^{2}, the vectors e0e_0, e1e_1, d=e0+e1d = e_0+e_1, and the linear subspaces U0,U1,U2U_0, U_1, U_2 above.

[L1]

span{v}={λv:λF}\operatorname{span}\{v\} = \{\, \lambda v : \lambda \in F \,\}; if v0Vv \ne 0_V then λv=0V\lambda v = 0_V only for λ=0F\lambda = 0_F and span{v}{0V}\operatorname{span}\{v\} \ne \{0_V\} (span{v}={λv:λF}\operatorname{span}\{v\} = \{\, \lambda v : \lambda \in F \,\}, which is {0V}\{0_V\} when v=0Vv = 0_V, and when v0Vv \ne 0_V contains 0V0_V only as the multiple 0Fv0_F v, claims 1 and 3).

[L2]

e:2F2e : 2 \to F^{2} is an ordered basis with (i<2λiei)(j)=λj\bigl(\sum_{i<2}\lambda_i e_i\bigr)(j) = \lambda_j, and dimFF2=2\dim_F F^{2} = 2 (The standard list e:nFne : n \to F^{n} with ei(i)=1Fe_i(i) = 1_F and ei(j)=0Fe_i(j) = 0_F for jij \ne i is an ordered basis of FnF^{n}; hence dimFFn=n\dim_F F^{n} = n, and F0F^{0} is the zero space with basis \varnothing and dimension 00, claims 2, 3 and 4).

[L7]

Counterexample

technique · direct
1.1

Each of e0e_0, e1e_1, dd is nonzero, since each takes the value 1F0F1_F \ne 0_F somewhere, and the three are pairwise distinct: e0e_0 and dd differ at 11, e1e_1 and dd differ at 00, and e0e_0 and e1e_1 differ at 00.

L6
1.2

dimFUj=1\dim_F U_j = 1 for each j<3j < 3. Take vv to be e0e_0, e1e_1 or dd; then {v}\{v\} spans span{v}\operatorname{span}\{v\}, and it is linearly independent, since an injective list into {v}\{v\} has length 00 or is the one-term list vv, and λv=0V\lambda v = 0_V forces λ=0F\lambda = 0_F because v0Vv \ne 0_V. So {v}\{v\} is a basis with exactly one element.

L1L4L5L6
1.3

The pairwise intersections are {0V}\{0_V\}. An element of U0U1U_0 \cap U_1 is λe0=μe1\lambda e_0 = \mu e_1; evaluating at 00 gives λ1F=μ0F\lambda 1_F = \mu 0_F, that is λ=0F\lambda = 0_F, so the element is 0Fe0=0V0_F e_0 = 0_V. An element of U0U2U_0 \cap U_2 is λe0=μd\lambda e_0 = \mu d; evaluating at 11 gives 0F=μ0_F = \mu, so it is 0V0_V. An element of U1U2U_1 \cap U_2 is λe1=μd\lambda e_1 = \mu d; evaluating at 00 gives 0F=μ0_F = \mu, so it is 0V0_V. Each intersection also contains 0V0_V, being an intersection of linear subspaces, so all three equal {0V}\{0_V\}.

L1L4L6
1.4

j<3Uj=F2\sum_{j<3}U_j = F^{2}. The sum contains each UjU_j, hence contains e0e_0 and e1e_1; being a linear subspace it contains span{e0,e1}=F2\operatorname{span}\{e_0,e_1\} = F^{2}, and it is contained in F2F^{2}.

L2L3L4
2.1

The two sides. The triple intersection U0U1U2U_0 \cap U_1 \cap U_2 is contained in U0U1={0V}U_0 \cap U_1 = \{0_V\} by step 1.3 and contains 0V0_V, so it is {0V}\{0_V\}; hence all four intersection terms have dimension 00 by step 1.3. By step 1.4 and the standard basis, dimF(j<3Uj)=dimFF2=2\dim_F\bigl(\sum_{j<3}U_j\bigr) = \dim_F F^{2} = 2, and by step 1.2 each dimFUj=1\dim_F U_j = 1. So the left-hand side of the claimed identity is 2+0+0+0=22 + 0 + 0 + 0 = 2 and the right-hand side is 1+1+1+0=31 + 1 + 1 + 0 = 3.

step 1.2step 1.3step 1.4L2L4L5L7
3.1

Since 232 \ne 3, the claimed identity fails for these three finite-dimensional linear subspaces of F2F^{2}, so the two-subspace dimension formula has no inclusion-exclusion extension to three subspaces.

step 2.1L5

Remarks

False statementConstruction: AI-adaptedVerification: AI-generatedprecheck passjudge pass (z-ai/glm-5.2)audited 2026-07-28Open item page →

FALSE: the union of two linearly independent subsets of a vector space is linearly independent

Facts & Assumptions

Given: A field FF, the vector space F2F^{2} with pointwise operations, and the vectors e0=(1F,0F)e_0 = (1_F,0_F), e1=(0F,1F)e_1 = (0_F,1_F) and d=e0+e1=(1F,1F)d = e_0 + e_1 = (1_F,1_F).

[L2]

{e0,e1,d}\{e_0,e_1,d\} has exactly three elements and is linearly dependent ({(1,0),(0,1),(1,1)}\{(1,0), (0,1), (1,1)\} spans F2F^{2} and is linearly dependent, so a spanning set need not be a basis; each of its three two-element subsets is a basis: the three-element count is stated there and claim 2 is that the set is linearly dependent).

[L3]

span{v}={λv:λF}\operatorname{span}\{v\} = \{\, \lambda v : \lambda \in F \,\}, and for v0Vv \ne 0_V the equation λv=0V\lambda v = 0_V forces λ=0F\lambda = 0_F (span{v}={λv:λF}\operatorname{span}\{v\} = \{\, \lambda v : \lambda \in F \,\}, which is {0V}\{0_V\} when v=0Vv = 0_V, and when v0Vv \ne 0_V contains 0V0_V only as the multiple 0Fv0_F v, claims 1 and 3).

Refutation

technique · direct
1.1

Take V:=F2V := F^{2} over an arbitrary field FF, A:={e0,e1}A := \{e_0, e_1\} and C:={d}C := \{d\}. Then AA is linearly independent, being a basis of F2F^{2}.

L1
1.2

CC is linearly independent. Its only injective finite lists are the empty one, which is independent, and the one-term list v0=dv_0 = d; for the latter, i<1λivi=λ0d\sum_{i<1}\lambda_i v_i = \lambda_0 d, and d0Vd \ne 0_V because d(0)=1F0Fd(0) = 1_F \ne 0_F, so λ0d=0V\lambda_0 d = 0_V forces λ0=0F\lambda_0 = 0_F.

L3L4L5L6
1.3

AC={e0,e1,d}A \cup C = \{e_0, e_1, d\}, which is linearly dependent.

L2
2.1

So AA and CC are linearly independent subsets of F2F^{2} whose union is linearly dependent, and the statement above is false.

step 1.1step 1.2step 1.3L4

Remarks

Sources