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Statement List for Metamath Proof Explorer - 5501-5600 - Page 56 of 58
TypeLabelDescription
Statement
 
Theoremcmcm 5501 Commutation is symmetric. Theorem 2(v) of [Kalmbach] p. 22.
|- A e. CH   &   |- B e. CH   =>   |- (A Com B <-> B Com A)
 
Theoremcmcm2 5502 Commutation with orthocomplement. Theorem 2.3(i) of [Beran] p. 39.
|- A e. CH   &   |- B e. CH   =>   |- (A Com B <-> A Com (_|_` B))
 
Theoremcmcm3 5503 Commutation with orthocomplement. Remark in [Kalmbach] p. 23.
|- A e. CH   &   |- B e. CH   =>   |- (A Com B <-> (_|_`
 A) Com B)
 
Theoremcmcm4 5504 Commutation with orthocomplement. Remark in [Kalmbach] p. 23.
|- A e. CH   &   |- B e. CH   =>   |- (A Com B <-> (_|_`
 A) Com (_|_` B))
 
Theoremcmbr2 5505 Alternate definition of the commutes relation. Remark in [Kalmbach] p. 23.
|- A e. CH   &   |- B e. CH   =>   |- (A Com B <-> A = ((A vH B) i^i (A vH (_|_` B))))
 
Theoremcmcmi 5506 Commutation is symmetric. Theorem 2(v) of [Kalmbach] p. 22.
|- A e. CH   &   |- B e. CH   &   |- A Com B   =>   |- B Com A
 
Theoremcmcm2i 5507 Commutation with orthocomplement. Theorem 2.3(i) of [Beran] p. 39.
|- A e. CH   &   |- B e. CH   &   |- A Com B   =>   |- A Com (_|_`
 B)
 
Theoremcmcm3i 5508 Commutation with orthocomplement. Remark of [Kalmbach] p. 23.
|- A e. CH   &   |- B e. CH   &   |- A Com B   =>   |- (_|_` A) Com B
 
Theoremcmbr3 5509 Alternate definition for the commutes relation. Lemma 3 of [Kalmbach] p. 23.
|- A e. CH   &   |- B e. CH   =>   |- (A Com B <-> (A i^i ((_|_`
 A) vH B)) = (A i^i B))
 
Theoremcmbr4 5510 Alternate definition for the commutes relation.
|- A e. CH   &   |- B e. CH   =>   |- (A Com B <-> (A i^i ((_|_`
 A) vH B)) (_ B)
 
Theoremcmle 5511 Comparable Hilbert lattice elements commute. Theorem 2.3(iii) of [Beran] p. 40.
|- A e. CH   &   |- B e. CH   &   |- A (_ B   =>   |- A Com B
 
Theoremcmj1 5512 A Hilbert lattice element commutes with its join.
|- A e. CH   &   |- B e. CH   =>   |- A Com (A vH B)
 
Theoremcmj2 5513 A Hilbert lattice element commutes with its join.
|- A e. CH   &   |- B e. CH   =>   |- B Com (A vH B)
 
Theoremcmm1 5514 A Hilbert lattice element commutes with its meet.
|- A e. CH   &   |- B e. CH   =>   |- A Com (A i^i B)
 
Theoremcmm2 5515 A Hilbert lattice element commutes with its meet.
|- A e. CH   &   |- B e. CH   =>   |- B Com (A i^i B)
 
Theoremcmid 5516 The commutes relation is reflexive.
|- A e. CH   =>   |- A Com A
 
Theorempjoml3t 5517 Variation of orthomodular law.
|- ((A e. CH /\ B e. CH) -> (B (_ A -> (A i^i ((_|_`
 A) vH B)) = B))
 
Theoremfh1 5518 Foulis-Holland Theorem. If any 2 pairs in a triple of orthomodular lattice elements commute, the triple is distributive. First of two parts. Theorem 5 of [Kalmbach] p. 25.
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- A Com B   &   |- A Com C   =>   |- (A i^i (B vH C)) = ((A i^i B) vH (A i^i C))
 
Theoremfh2 5519 Foulis-Holland Theorem. If any 2 pairs in a triple of orthomodular lattice elements commute, the triple is distributive. Second of two parts. Theorem 5 of [Kalmbach] p. 25.
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- A Com B   &   |- A Com C   =>   |- (B i^i (A vH C)) = ((B i^i A) vH (B i^i C))
 
Theoremqlax1 5520 One of the equations showing CH is an ortholattice. (This corresponds to axiom "ax-1" in the Quantum Logic Explorer.)
|- A e. CH   =>   |- A = (_|_`
 (_|_` A))
 
Theoremqlax2 5521 One of the equations showing CH is an ortholattice. (This corresponds to axiom "ax-2" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   =>   |- (A vH B) = (B vH A)
 
Theoremqlax3 5522 One of the equations showing CH is an ortholattice. (This corresponds to axiom "ax-3" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   &   |- C e. CH   =>   |- ((A vH B) vH C) = (A vH (B vH C))
 
Theoremqlax4 5523 One of the equations showing CH is an ortholattice. (This corresponds to axiom "ax-4" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   =>   |- (A vH (B vH (_|_` B))) = (B vH (_|_` B))
 
Theoremqlax5 5524 One of the equations showing CH is an ortholattice. (This corresponds to axiom "ax-5" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   =>   |- (A vH (_|_` ((_|_` A) vH B))) = A
 
Theoremqlaxr1 5525 One of the conditions showing CH is an ortholattice. (This corresponds to axiom "ax-r1" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   &   |- A = B   =>   |- B = A
 
Theoremqlaxr2 5526 One of the conditions showing CH is an ortholattice. (This corresponds to axiom "ax-r2" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- A = B   &   |- B = C   =>   |- A = C
 
Theoremqlaxr4 5527 One of the conditions showing CH is an ortholattice. (This corresponds to axiom "ax-r4" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   &   |- A = B   =>   |- (_|_` A) = (_|_` B)
 
Theoremqlaxr5 5528 One of the conditions showing CH is an ortholattice. (This corresponds to axiom "ax-r5" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- A = B   =>   |- (A vH C) = (B vH C)
 
Theoremqlaxr3 5529 A variation of the orthomodular law, showing CH is an orthomodular lattice. (This corresponds to axiom "ax-r3" in the Quantum Logic Explorer.)
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- (C vH (_|_` C)) = ((_|_` ((_|_` A) vH (_|_` B))) vH (_|_` (A vH B)))   =>   |- A = B
 
Theoremosumlem1 5530 Lemma for osum 5538.
|- A e. CH   &   |- B e. CH   &   |- B (_ (_|_` A)   &   |- (ph <-> (((C e. A /\ D e. B) /\ R = (C +v D)) /\ ((x e. A /\ y e. (_|_` A)) /\ z = (x +v y))))   =>   |- (ph -> (((C e. H~ /\ D e. H~) /\ R e. H~) /\ ((x e. H~ /\ y e. H~) /\ z e. H~)))
 
Theoremosumlem2 5531 Lemma for osum 5538.
|- A e. CH   &   |- B e. CH   &   |- B (_ (_|_` A)   &   |- (ph <-> (((C e. A /\ D e. B) /\ R = (C +v D)) /\ ((x e. A /\ y e. (_|_` A)) /\ z = (x +v y))))   =>   |- (ph -> (((norm` (C -v x))^2) + ((norm` (D -v y))^2)) = ((norm` (R -v z))^2))
 
Theoremosumlem3 5532 Lemma for osum 5538.
|- A e. CH   &   |- B e. CH   &   |- B (_ (_|_` A)   &   |- (ph <-> (((C e. A /\ D e. B) /\ R = (C +v D)) /\ ((x e. A /\ y e. (_|_` A)) /\ z = (x +v y))))   =>   |- (ph -> (norm` (D -v y)) <_ (norm` (R -v z)))
 
Theoremosumlem4 5533 Lemma for osum 5538.
|- A e. CH   &   |- B e. CH   &   |- B (_ (_|_` A)   &   |- G e. V   &   |- H e. V   =>   |- ((((F:NN-->A /\ G:NN-->B) /\ A.w e. NN (H` w) = ((F` w) +v (G` w))) /\ ((x e. A /\ y e. (_|_` A)) /\ z = (x +v y))) -> (H ~~>v z -> G ~~>v y))
 
Theoremosumlem5 5534 Lemma for osum 5538.
|- A e. CH   &   |- B e. CH   =>   |- (H:NN-->(A +H B) -> E.fE.g((f:NN-->A /\ g:NN-->B) /\ A.w e. NN (H` w) = ((f` w) +v (g` w))))
 
Theoremosumlem6 5535 Lemma for osum 5538.
|- A e. CH   &   |- B e. CH   &   |- B (_ (_|_` A)   &   |- H e. V   =>   |- (((H:NN-->(A +H B) /\ H ~~>v z) /\ ((x e. A /\ y e. (_|_` A)) /\ z = (x +v y))) -> y e. B)
 
Theoremosumlem7 5536 Lemma for osum 5538.
|- A e. CH   &   |- B e. CH   &   |- B (_ (_|_` A)   =>   |- (A +H B) e. CH
 
Theoremosumlem8 5537 Lemma for osum 5538.
|- A e. CH   &   |- B e. CH   =>   |- (B (_ (_|_` A) -> (A +H B) e. CH)
 
Theoremosum 5538 If two closed subspaces of a Hilbert space are orthogonal, their subspace sum equals their subspace join. Lemma 3 of [Kalmbach] p. 67. Note that the Axiom of Choice is used for this proof (in osumlem5 5534 and via pjpjtht 5262 in osumlem7 5536).
|- A e. CH   &   |- B e. CH   =>   |- (A (_ (_|_` B) -> (A +H B) = (A vH B))
 
Theoremspansnj 5539 The subspace sum of a closed subspace and a one-dimensional subspace equals their join. (Proof suggested by Eric Schechter 1-Jun-04.)
|- A e. CH   &   |- B e. H~   =>   |- (A +H (span` {B})) = (A vH (span` {B}))
 
Theoremspansnjt 5540 The subspace sum of a closed subspace and a one-dimensional subspace equals their join.
|- ((A e. CH /\ B e. H~) -> (A +H (span` {B})) = (A vH (span` {B})))
 
Theoremspansnsclt 5541 The subspace sum of a closed subspace and a one-dimensional subspace is closed.
|- ((A e. CH /\ B e. H~) -> (A +H (span` {B})) e. CH)
 
Theoremspansncv 5542 Hilbert space has the covering property (using spans of singletons to represent atoms). Exercise 5 of [Kalmbach] p. 153.
|- A e. CH   &   |- B e. CH   &   |- C e. H~   =>   |- ((A (. B /\ B (_ (A vH (span` {C}))) -> B = (A vH (span` {C})))
 
Theoremspansncvt 5543 Hilbert space has the covering property (using spans of singletons to represent atoms). Exercise 5 of [Kalmbach] p. 153.
|- ((A e. CH /\ B e. CH /\ C e. H~) -> ((A (. B /\ B (_ (A vH (span` {C}))) -> B = (A vH (span` {C})))