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CounterexampleConstruction: AI-adaptedVerification: AI-generatedSession-authored (Fable 5 assisted)precheck passjudge pass (z-ai/glm-5.2)audited 2026-07-28
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{(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

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