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LemmaStatement: AI-adaptedProof: AI-adaptedSession-authored (Fable 5 assisted)precheck passverified 2026-08-02 (claude-opus-5)
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  • 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.
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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

Statement

Let VV be a vector space over a field FF (Vector space over a field). For all λF\lambda \in F and vVv \in V:

  1. 0Fv=0V0_F v = 0_V;
  2. λ0V=0V\lambda 0_V = 0_V;
  3. (λ)v=(λv)(-\lambda)v = -(\lambda v), and also λ(v)=(λv)\lambda(-v) = -(\lambda v);
  4. (1F)v=v(-1_F)v = -v;
  5. if λv=0V\lambda v = 0_V then λ=0F\lambda = 0_F or v=0Vv = 0_V.

Here 0F0_F and 1F1_F are the additive and multiplicative identities of FF, 0V0_V is the zero vector, λ-\lambda is the additive inverse of λ\lambda in FF, and v-v is the additive inverse of vv in the abelian group (V,+,0V)(V,+,0_V).

Facts & Assumptions

Given: A field FF, a vector space VV over FF with axioms (V1)–(V5) (Vector space over a field), a scalar λF\lambda \in F and a vector vVv \in V.

[L1]

The four scalar axioms: λ(u+w)=λu+λw\lambda(u+w) = \lambda u + \lambda w (V2); (λ+μ)w=λw+μw(\lambda+\mu)w = \lambda w + \mu w (V3); (λμ)w=λ(μw)(\lambda\mu)w = \lambda(\mu w) (V4); 1Fw=w1_F w = w (V5) (Vector space over a field).

[L2]

(V,+,0V)(V,+,0_V) is an abelian group (V1): addition is associative and commutative, 0V0_V is a two-sided identity, and each wVw \in V has an additive inverse w-w with w+(w)=0V=(w)+ww + (-w) = 0_V = (-w) + w (Vector space over a field, Group and abelian group).

[L3]
[L4]

Field arithmetic (Field): 0F+0F=0F0_F + 0_F = 0_F; μ+(μ)=0F\mu + (-\mu) = 0_F for every μF\mu \in F; 1F1_F is the multiplicative identity; multiplication is associative; and every μ0F\mu \ne 0_F has a multiplicative inverse μ1\mu^{-1} with μ1μ=1F\mu^{-1}\mu = 1_F.

[L5]

The identities 0F0_F, 1F1_F and the inverses μ-\mu, μ1\mu^{-1} of a field are unique, so those notations denote well-defined elements (Identities and inverses in a field are unique).

Proof

technique · direct
1.1

By (V3) applied to 0F0_F and 0F0_F, and 0F+0F=0F0_F + 0_F = 0_F in FF: 0Fv+0Fv=(0F+0F)v=0Fv0_F v + 0_F v = (0_F + 0_F)v = 0_F v.

L1L4
1.2

Since 0V0_V is a two-sided identity for ++: 0Fv=0V+0Fv0_F v = 0_V + 0_F v.

L2
1.3

By (V2) applied to 0V0_V and 0V0_V, and 0V+0V=0V0_V + 0_V = 0_V in VV: λ0V+λ0V=λ(0V+0V)=λ0V\lambda 0_V + \lambda 0_V = \lambda(0_V + 0_V) = \lambda 0_V.

L1L2
1.4

Since 0V0_V is a two-sided identity for ++: λ0V=0V+λ0V\lambda 0_V = 0_V + \lambda 0_V.

L2
1.5

The vector λv\lambda v has an additive inverse (λv)-(\lambda v) with λv+((λv))=0V\lambda v + (-(\lambda v)) = 0_V.

L2
2.1

Combining steps 1.1 and 1.2 gives 0Fv+0Fv=0V+0Fv0_F v + 0_F v = 0_V + 0_F v; cancelling 0Fv0_F v on the right yields 0Fv=0V0_F v = 0_V, which is claim 1.

step 1.1step 1.2L3
2.2

Combining steps 1.3 and 1.4 gives λ0V+λ0V=0V+λ0V\lambda 0_V + \lambda 0_V = 0_V + \lambda 0_V; cancelling λ0V\lambda 0_V on the right yields λ0V=0V\lambda 0_V = 0_V, which is claim 2.

step 1.3step 1.4L3
3.1

By (V3) applied to λ\lambda and λ-\lambda, then λ+(λ)=0F\lambda + (-\lambda) = 0_F, then claim 1: λv+(λ)v=(λ+(λ))v=0Fv=0V\lambda v + (-\lambda)v = (\lambda + (-\lambda))v = 0_F v = 0_V.

step 2.1L1L4
3.2

By (V2) applied to vv and v-v, then v+(v)=0Vv + (-v) = 0_V, then claim 2: λv+λ(v)=λ(v+(v))=λ0V=0V\lambda v + \lambda(-v) = \lambda(v + (-v)) = \lambda 0_V = 0_V.

step 2.2L1L2
3.3

Suppose λv=0V\lambda v = 0_V and λ0F\lambda \ne 0_F. Then λ1F\lambda^{-1} \in F exists with λ1λ=1F\lambda^{-1}\lambda = 1_F, so v=1Fv=(λ1λ)v=λ1(λv)=λ10V=0Vv = 1_F v = (\lambda^{-1}\lambda)v = \lambda^{-1}(\lambda v) = \lambda^{-1} 0_V = 0_V, using (V5), (V4) and claim 2 in turn.

step 2.2L1L4L5
4.1

Steps 3.1 and 1.5 exhibit both (λ)v(-\lambda)v and (λv)-(\lambda v) as vectors xx with λv+x=0V\lambda v + x = 0_V; cancelling λv\lambda v on the left gives (λ)v=(λv)(-\lambda)v = -(\lambda v).

step 3.1step 1.5L3
5.1

Likewise steps 3.2 and 1.5 give λv+λ(v)=0V=λv+((λv))\lambda v + \lambda(-v) = 0_V = \lambda v + (-(\lambda v)), and cancelling λv\lambda v on the left gives λ(v)=(λv)\lambda(-v) = -(\lambda v); with step 4.1 this is claim 3.

step 3.2step 1.5L3
5.2

Taking λ=1F\lambda = 1_F in step 4.1 and using (V5): (1F)v=(1Fv)=v(-1_F)v = -(1_F v) = -v, which is claim 4.

step 4.1L1
6.1

Claim 1 is step 2.1, claim 2 is step 2.2, claim 3 is steps 4.1 and 5.1, and claim 4 is step 5.2; for claim 5, if λv=0V\lambda v = 0_V then either λ=0F\lambda = 0_F, or λ0F\lambda \ne 0_F and step 3.3 gives v=0Vv = 0_V.

step 2.1step 2.2step 3.3step 4.1step 5.1step 5.2

Remarks

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