Metamath Proof Explorer


Theorem dib0

Description: The value of partial isomorphism B at the lattice zero is the singleton of the zero vector i.e. the zero subspace. (Contributed by NM, 27-Mar-2014)

Ref Expression
Hypotheses dib0.z ⊢ 0 ˙ = 0. ⁡ K
dib0.h ⊢ H = LHyp ⁡ K
dib0.i ⊢ I = DIsoB ⁡ K ⁡ W
dib0.u ⊢ U = DVecH ⁡ K ⁡ W
dib0.o ⊢ O = 0 U
Assertion dib0 ⊢ K ∈ HL ∧ W ∈ H → I ⁡ 0 ˙ = O

Proof

Step Hyp Ref Expression
1 dib0.z ⊢ 0 ˙ = 0. ⁡ K
2 dib0.h ⊢ H = LHyp ⁡ K
3 dib0.i ⊢ I = DIsoB ⁡ K ⁡ W
4 dib0.u ⊢ U = DVecH ⁡ K ⁡ W
5 dib0.o ⊢ O = 0 U
6 fvex ⊢ Base K ∈ V
7 resiexg ⊢ Base K ∈ V → I ↾ Base K ∈ V
8 6 7 ax-mp ⊢ I ↾ Base K ∈ V
9 fvex ⊢ LTrn ⁡ K ⁡ W ∈ V
10 9 mptex ⊢ f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K ∈ V
11 8 10 xpsn ⊢ I ↾ Base K × f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K = I ↾ Base K f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K
12 id ⊢ K ∈ HL ∧ W ∈ H → K ∈ HL ∧ W ∈ H
13 hlop ⊢ K ∈ HL → K ∈ OP
14 13 adantr ⊢ K ∈ HL ∧ W ∈ H → K ∈ OP
15 eqid ⊢ Base K = Base K
16 15 1 op0cl ⊢ K ∈ OP → 0 ˙ ∈ Base K
17 14 16 syl ⊢ K ∈ HL ∧ W ∈ H → 0 ˙ ∈ Base K
18 15 2 lhpbase ⊢ W ∈ H → W ∈ Base K
19 eqid ⊢ ≤ K = ≤ K
20 15 19 1 op0le ⊢ K ∈ OP ∧ W ∈ Base K → 0 ˙ ≤ K W
21 13 18 20 syl2an ⊢ K ∈ HL ∧ W ∈ H → 0 ˙ ≤ K W
22 eqid ⊢ LTrn ⁡ K ⁡ W = LTrn ⁡ K ⁡ W
23 eqid ⊢ f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K = f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K
24 eqid ⊢ DIsoA ⁡ K ⁡ W = DIsoA ⁡ K ⁡ W
25 15 19 2 22 23 24 3 dibval2 ⊢ K ∈ HL ∧ W ∈ H ∧ 0 ˙ ∈ Base K ∧ 0 ˙ ≤ K W → I ⁡ 0 ˙ = DIsoA ⁡ K ⁡ W ⁡ 0 ˙ × f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K
26 12 17 21 25 syl12anc ⊢ K ∈ HL ∧ W ∈ H → I ⁡ 0 ˙ = DIsoA ⁡ K ⁡ W ⁡ 0 ˙ × f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K
27 15 1 2 24 dia0 ⊢ K ∈ HL ∧ W ∈ H → DIsoA ⁡ K ⁡ W ⁡ 0 ˙ = I ↾ Base K
28 27 xpeq1d ⊢ K ∈ HL ∧ W ∈ H → DIsoA ⁡ K ⁡ W ⁡ 0 ˙ × f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K = I ↾ Base K × f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K
29 26 28 eqtrd ⊢ K ∈ HL ∧ W ∈ H → I ⁡ 0 ˙ = I ↾ Base K × f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K
30 15 2 22 4 5 23 dvh0g ⊢ K ∈ HL ∧ W ∈ H → O = I ↾ Base K f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K
31 30 sneqd ⊢ K ∈ HL ∧ W ∈ H → O = I ↾ Base K f ∈ LTrn ⁡ K ⁡ W ⟼ I ↾ Base K
32 11 29 31 3eqtr4a ⊢ K ∈ HL ∧ W ∈ H → I ⁡ 0 ˙ = O