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Statement List for Metamath Proof Explorer - 9501-9600 - Page 96 of 123
TypeLabelDescription
Statement
 
Theorempjthlem7 9501 Lemma for pjthi 9509.
 
Theorempjthlem8 9502 Lemma for pjthi 9509.
 
Theorempjthlem9 9503 Lemma for pjthi 9509.
 
Theorempjthlem10 9504 Lemma for pjthi 9509.
 
Theorempjthlem11 9505 Lemma for pjthi 9509.
 
Theorempjthlem12 9506 Lemma for pjthi 9509.
 
Theorempjthlem13 9507 Lemma for pjthi 9509.
 
Theorempjthlem14 9508 Lemma for pjthi 9509.
 
Theorempjthi 9509 Projection Theorem: Any Hilbert space vector A can be decomposed into a member x of a closed subspace H and a member y of the complement of the subspace. Theorem 3.7(i) of [Beran] p. 102 (existence part).
|- A e. H~   &   |- H e. CH   =>   |- E.x e. H E.y e. (_|_` H)A = (x +h y)
 
Theorempjth 9510 Projection Theorem: Any Hilbert space vector A can be decomposed into a member x of a closed subspace H and a member y of the complement of the subspace. Theorem 3.7(i) of [Beran] p. 102 (existence part).
|- ((H e. CH /\ A e. H~) -> E.x e. H E.y e. (_|_` H)A = (x +h y))
 
Theorempjtheui 9511 Uniqueness of x for the projection theorem. See pjtheu2i 9526 for the uniqueness of y.
|- H e. CH   =>   |- (A e. H~ -> E!x e. H E.y e. (_|_` H)A = (x +h y))
 
Theorempjtheu 9512 Uniqueness of x for the projection theorem.
|- ((H e. CH /\ A e. H~) -> E!x e. H E.y e. (_|_` H)A = (x +h y))
 
Projectors
 
Definitiondf-pj 9513 Define the projection function on a Hilbert space, as a mapping from the Hilbert lattice to a function on Hilbert space. Every closed subspace is associated with a unique projection function. Remark in [Kalmbach] p. 66, adopted as a definition. (proj` H)` A is the projection of vector A onto closed subspace H. Note that the range of proj is the set of all projection operators, so T e. ran proj means that T is a projection operator.
|- proj = {<.h, f>. | (h e. CH /\ f = {<.x, y>. | (x e. H~ /\ y = U.{z e. h | E.w e. (_|_` h)x = (z +h w)})})}
 
Theorempjmval 9514 The value of the projection map.
|- (H e. CH -> (proj` H) = {<.x, y>. | (x e. H~ /\ y = U.{z e. H | E.w e. (_|_` H)x = (z +h w)})})
 
Theorempjval 9515 Value of a projection.
|- ((H e. CH /\ A e. H~) -> ((proj` H)` A) = U.{x e. H | E.y e. (_|_` H)A = (x +h y)})
 
Theoremaxpjcl 9516 Closure of a projection in its subspace. If we consider this together with axpjpj 9532 to be axioms, the need for the ax-hcompl 9347 can often be avoided for the kinds of theorems we are interested in here. An interesting project is to see how far we can go by using them in place of it. In particular, we can prove the orthomodular law pjomli 9544.)
|- ((H e. CH /\ A e. H~) -> ((proj` H)` A) e. H)
 
Theorempjeq2 9517 Equality with a projection.
|- ((H e. CH /\ A e. H~ /\ B e. H) -> (((proj` H)` A) = B <-> E.x e. (_|_` H)A = (B +h x)))
 
Theorempjeq 9518 Equality with a projection.
|- ((H e. CH /\ A e. H~) -> (((proj` H)` A) = B <-> (B e. H /\ E.x e. (_|_` H)A = (B +h x))))
 
Theorempjhcl 9519 Closure of a projection in Hilbert space.
|- ((H e. CH /\ A e. H~) -> ((proj` H)` A) e. H~)
 
Orthomodular law
 
Theoremomlsilem 9520 Lemma for orthomodular law in the Hilbert lattice.
 
Theoremomlsii 9521 Subspace inference form of orthomodular law in the Hilbert lattice.
|- A e. CH   &   |- B e. SH   &   |- A (_ B   &   |- (B i^i (_|_` A)) = 0H   =>   |- A = B
 
Theoremomlsi 9522 Subspace form of orthomodular law in the Hilbert lattice. Compare the orthomodular law in Theorem 2(ii) of [Kalmbach] p. 22.
|- A e. CH   &   |- B e. SH   =>   |- ((A (_ B /\ (B i^i (_|_` A)) = 0H) -> A = B)
 
Theoremococi 9523 Complement of complement of a closed subspace of Hilbert space. Theorem 3.7(ii) of [Beran] p. 102.
|- A e. CH   =>   |- (_|_` (_|_` A)) = A
 
Theoremococ 9524 Complement of complement of a closed subspace of Hilbert space. Theorem 3.7(ii) of [Beran] p. 102.
|- (A e. CH -> (_|_` (_|_`
 A)) = A)
 
Theoremdfch2 9525 Alternate definition of the Hilbert lattice.
|- CH = {x | (x (_ H~ /\ (_|_` (_|_`
 x)) = x)}
 
Projectors (cont.)
 
Theorempjtheu2i 9526 Uniqueness of y for the projection theorem.
|- H e. CH   =>   |- (A e. H~ -> E!y e. (_|_` H)E.x e. H A = (x +h y))
 
Theorempjcli 9527 Closure of a projection in its subspace.
|- H e. CH   =>   |- (A e. H~ -> ((proj` H)` A) e. H)
 
Theorempjhcli 9528 Closure of a projection in Hilbert space.
|- H e. CH   =>   |- (A e. H~ -> ((proj` H)` A) e. H~)
 
Theorempjclii 9529 Closure of a projection in its subspace.
|- H e. CH   &   |- A e. H~   =>   |- ((proj` H)` A) e. H
 
Theorempjhclii 9530 Closure of a projection in Hilbert space.
|- H e. CH   &   |- A e. H~   =>   |- ((proj` H)` A) e. H~
 
Theorempjpj0i 9531 Decomposition of a vector into projections.
|- H e. CH   &   |- A e. H~   =>   |- A = (((proj` H)` A) +h ((proj` (_|_` H))` A))
 
Theoremaxpjpj 9532 Decomposition of a vector into projections. See comment in axpjcl 9516.
|- ((H e. CH /\ A e. H~) -> A = (((proj` H)` A) +h ((proj` (_|_` H))` A)))
 
Theorempjpji 9533 Decomposition of a vector into projections.
|- H e. CH   &   |- A e. H~   =>   |- A = (((proj` H)` A) +h ((proj` (_|_` H))` A))
 
Theorempjpjth 9534 Projection Theorem: Any Hilbert space vector A can be decomposed into a member x of a closed subspace H and a member y of the complement of the subspace. Theorem 3.7(i) of [Beran] p. 102 (existence part).
|- ((H e. CH /\ A e. H~) -> E.x e. H E.y e. (_|_` H)A = (x +h y))
 
Theorempjpjthi 9535 Projection Theorem: Any Hilbert space vector A can be decomposed into a member x of a closed subspace H and a member y of the complement of the subspace. Theorem 3.7(i) of [Beran] p. 102 (existence part).
|- A e. H~   &   |- H e. CH   =>   |- E.x e. H E.y e. (_|_` H)A = (x +h y)
 
Theorempjop 9536 Orthocomplement projection in terms of projection.
|- ((H e. CH /\ A e. H~) -> ((proj` (_|_` H))` A) = (A -h ((proj` H)` A)))
 
Theorempjpo 9537 Projection in terms of orthocomplement projection.
|- ((H e. CH /\ A e. H~) -> ((proj` H)` A) = (A -h ((proj` (_|_` H))` A)))
 
Theorempjopi 9538 Orthocomplement projection in terms of projection.
|- H e. CH   &   |- A e. H~   =>   |- ((proj` (_|_` H))` A) = (A -h ((proj` H)` A))
 
Theorempjpoi 9539 Projection in terms of orthocomplement projection.
|- H e. CH   &   |- A e. H~   =>   |- ((proj` H)` A) = (A -h ((proj` (_|_` H))` A))
 
Theorempjoc1i 9540 Projection of a vector in the orthocomplement of the projection subspace.
|- H e. CH   &   |- A e. H~   =>   |- (A e. H <-> ((proj` (_|_` H))` A) = 0h)
 
Theorempjchi 9541 Projection of a vector in the projection subspace. Lemma 4.4(ii) of [Beran] p. 111.
|- H e. CH   &   |- A e. H~   =>   |- (A e. H <-> ((proj` H)` A) = A)
 
Theorempjoccl 9542 The part of a vector that belongs to the orthocomplemented space.
|- ((H e. CH /\ A e. H~) -> (A -h ((proj` H)` A)) e. (_|_` H))
 
Theorempjoc1 9543 Projection of a vector in the orthocomplement of the projection subspace.
|- ((H e. CH /\ A e. H~) -> (A e. H <-> ((proj` (_|_` H))` A) = 0h))
 
Theorempjomli 9544 Subspace form of orthomodular law in the Hilbert lattice. Compare the orthomodular law in Theorem 2(ii) of [Kalmbach] p. 22. Derived using projections; compare omlsi 9522.
|- A e. CH   &   |- B e. SH   =>   |- ((A (_ B /\ (B i^i (_|_` A)) = 0H) -> A = B)
 
Theorempjoml 9545 Subspace form of orthomodular law in the Hilbert lattice. Compare the orthomodular law in Theorem 2(ii) of [Kalmbach] p. 22. Derived using projections; compare omlsi 9522.
|- (((A e. CH /\ B e. SH) /\ (A (_ B /\ (B i^i (_|_` A)) = 0H)) -> A = B)
 
Theorempjococi 9546 Proof of orthocomplement theorem using projections. Compare ococ 9524.
|- H e. CH   =>   |- (_|_` (_|_` H)) = H
 
Theorempjoc2i 9547 Projection of a vector in the orthocomplement of the projection subspace. Lemma 4.4(iii) of [Beran] p. 111.
|- H e. CH   &   |- A e. H~   =>   |- (A e. (_|_` H) <-> ((proj` H)` A) = 0h)
 
Theorempjoc2 9548 Projection of a vector in the orthocomplement of the projection subspace. Lemma 4.4(iii) of [Beran] p. 111.
|- ((H e. CH /\ A e. H~) -> (A e. (_|_` H) <-> ((proj` H)` A) = 0h))
 
Subspace sum, span, lattice join, lattice supremum
 
Definitiondf-shsum 9549 Define subspace sum in SH. See shsumval 9553, shsumval2i 9636, and shsumval3i 9637 for its value.
|- +H = {<.<.x, y>., z>. | ((x e. SH /\ y e. SH) /\ z = {w e. H~ | E.v e. x E.u e. y w = (v +h u)})}
 
Definitiondf-span 9550 Define the linear span of a subset of Hilbert space. Definition of span in [Schechter] p. 276. See spanval 9575 for its value.
|- span = {<.x, y>. | (x (_ H~ /\ y = |^|{z e. SH | x (_ z})}
 
Definitiondf-chj 9551 Define Hilbert lattice join. See chjval 9598 for its value and chjcl 9605 for its closure law. Note that we define it over all Hilbert space subsets to allow proving more general theorems. Even for general subsets the join belongs to CH; see sshjcl 9603. For an alternate definition see dfchj2 9600.
|- vH = {<.<.x, y>., z>. | ((x (_ H~ /\ y (_ H~) /\ z = (_|_` (_|_` (x u. y))))}
 
Definitiondf-chsup 9552 Define the supremum of a set of Hilbert lattice elements. See chsupval2 9578 for its value and dfchsup2 9574 for an alternate definition. We actually define the supremum for an arbitrary collection of Hilbert space subsets, not just elements of the Hilbert lattice CH, to allow more general theorems. Even for general subsets the supremum still a Hilbert lattice element; see hsupcl 9583.
|- \/H = {<.x, y>. | (x (_ P~H~ /\ y = (_|_` (_|_` U.x)))}
 
Theoremshsumval 9553 Value of subspace sum of two Hilbert space subspaces. Definition of subspace sum in [Kalmbach] p. 65.
|- ((A e. SH /\ B e. SH) -> (A +H B) = {x e. H~ | E.y e. A E.z e. B x = (y +h z)})
 
Theoremshsel 9554 Membership in the subspace sum of two Hilbert subspaces.
|- ((A e. SH /\ B e. SH) -> (C e. (A +H B) <-> E.x e. A E.y e. B C = (x +h y)))
 
Theoremshsel3 9555 Membership in the subspace sum of two Hilbert subspaces, using vector subtraction.
|- ((A e. SH /\ B e. SH) -> (C e. (A +H B) <-> E.x e. A E.y e. B C = (x -h y)))
 
Theoremshseli 9556 Membership in subspace sum.
|- A e. SH   &   |- B e. SH   =>   |- (C e. (A +H B) <-> E.x e. A E.y e. B C = (x +h y))
 
Theoremshscli 9557 Closure of subspace sum.
|- A e. SH   &   |- B e. SH   =>   |- (A +H B) e. SH
 
Theoremshscl 9558 Closure of subspace sum.
|- ((A e. SH /\ B e. SH) -> (A +H B) e. SH)
 
Theoremshscom 9559 Commutative law for subspace sum.
|- ((A e. SH /\ B e. SH) -> (A +H B) = (B +H A))
 
Theoremshsva 9560 Vector sum belongs to subspace sum.
|- ((A e. SH /\ B e. SH) -> ((C e. A /\ D e. B) -> (C +h D) e. (A +H B)))
 
Theoremshsel1 9561 A subspace sum contains a member of one of its subspaces.
|- ((A e. SH /\ B e. SH) -> (C e. A -> C e. (A +H B)))
 
Theoremshsel2 9562 A subspace sum contains a member of one of its subspaces.
|- ((A e. SH /\ B e. SH) -> (C e. B -> C e. (A +H B)))
 
Theoremshsvs 9563 Vector subtraction belongs to subspace sum.
|- ((A e. SH /\ B e. SH) -> ((C e. A /\ D e. B) -> (C -h D) e. (A +H B)))
 
Theoremshsub1 9564 Subspace sum is an upper bound of its arguments.
|- ((A e. SH /\ B e. SH) -> A (_ (A +H B))
 
Theoremshsub2 9565 Subspace sum is an upper bound of its arguments.
|- ((A e. SH /\ B e. SH) -> A (_ (B +H A))
 
Theoremchoc0 9566 The orthocomplement of the zero subspace is the unit subspace.
|- (_|_` 0H) = H~
 
Theoremchoc1 9567 The orthocomplement of the unit subspace is the zero subspace. Does not require Axiom of Choice.
|- (_|_` H~) = 0H
 
Theoremchocnul 9568 Orthogonal complement of the empty set.
|- (_|_` (/)) = H~
 
Theoremshintcli 9569 Closure of intersection of a non-empty subset of SH.
|- (A (_ SH /\ A =/= (/))   =>   |- |^|A e. SH
 
Theoremshintcl 9570 The intersection of a non-empty set of subspaces is a subspace.
|- ((A (_ SH /\ A =/= (/)) -> |^|A e. SH)
 
Theoremchintcli 9571 The intersection of a non-empty set of closed subspaces is a closed subspace.
|- (A (_ CH /\ A =/= (/))   =>   |- |^|A e. CH
 
Theoremchintcl 9572 The intersection (infimum) of a non-empty subset of CH belongs to CH. Part of Theorem 3.13 of [Beran] p. 108. Also part of Definition 3.4-1 in [MegillPavicic] p. 2345 (PDF p. 8).
|- ((A (_ CH /\ A =/= (/)) -> |^|A e. CH)
 
Theoremococin 9573 The double complement is the smallest closed subspace containing a subset of Hilbert space. Remark 3.12(B) of [Beran] p. 107.
|- (A (_ H~ -> (_|_` (_|_` A)) = |^|{x e. CH | A (_ x})
 
Theoremdfchsup2 9574 Alternate definition of supremum of a subset of the Hilbert lattice. Definition in Proposition 1 of [Kalmbach] p. 65. We actually define it on any collection of Hilbert space subsets, not just the Hilbert lattice CH, to allow more general theorems.
|- \/H = {<.x, y>. | (x (_ P~H~ /\ y = |^|{z e. CH | U.x (_ z})}
 
Theoremspanval 9575 Value of the linear span of a subset of Hilbert space. The span is the intersection of all subspaces constraining the subset. Definition of span in [Schechter] p. 276.
|- (A (_ H~ -> (span` A) = |^|{x e. SH | A (_ x})
 
Theoremhsupval2 9576 Value of supremum of set of subsets of Hilbert space. Definition of supremum in Proposition 1 of [Kalmbach] p. 65.
|- (A (_ P~H~ -> ( \/H ` A) = |^|{x e. CH | U.A (_ x})
 
Theoremhsupval 9577 Value of supremum of set of subsets of Hilbert space. For an alternate version of the value, see hsupval2 9576.
|- (A (_ P~H~ -> ( \/H ` A) = (_|_` (_|_` U.A)))
 
Theoremchsupval2 9578 The value of the supremum of a set of closed subspaces of Hilbert space. Definition of supremum in Proposition 1 of [Kalmbach] p. 65.
|- (A (_ CH -> ( \/H ` A) = |^|{x e. CH | U.A (_ x})
 
Theoremchsupval 9579 The value of the supremum of a set of closed subspaces of Hilbert space. For an alternate version of the value, see chsupval2 9578.
|- (A (_ CH -> ( \/H ` A) = (_|_` (_|_`
 U.A)))
 
Theoremspancl 9580 The span of a subset of Hilbert space is a subspace.
|- (A (_ H~ -> (span` A) e. SH)
 
Theoremelspancl 9581 A member of a span is a vector.
|- ((A (_ H~ /\ B e. (span` A)) -> B e. H~)
 
Theoremshsupcl 9582 Closure of the subspace supremum of set of subsets of Hilbert space.
|- (A (_ P~H~ -> (span` U.A) e. SH)
 
Theoremhsupcl 9583 Closure of supremum of set of subsets of Hilbert space. Note that the supremum belongs to CH even if the subsets do not.
|- (A (_ P~H~ -> ( \/H ` A) e. CH)
 
Theoremchsupcl 9584 Closure of supremum of subset of CH. Definition of supremum in Proposition 1 of [Kalmbach] p. 65. Shows that CH is a complete lattice. Also part of Definition 3.4-1 in [MegillPavicic] p. 2345 (PDF p. 8).
|- (A (_ CH -> ( \/H ` A) e. CH)
 
Theoremhsupss 9585 Subset relation for supremum of Hilbert space subsets.
|- ((A (_ P~H~ /\ B (_ P~H~) -> (A (_ B -> ( \/H ` A) (_ ( \/H ` B)))
 
Theoremchsupss 9586 Subset relation for supremum of subset of CH.
|- ((A (_ CH /\ B (_ CH) -> (A (_ B -> ( \/H ` A) (_ ( \/H ` B)))
 
Theoremchsupid 9587 A subspace is the supremum of all smaller subspaces.
|- (A e. CH -> ( \/H ` {x e. CH | x (_ A}) = A)
 
Theoremchsupsn 9588 Value of supremum of subset of CH on a singleton.
|- (A e. CH -> ( \/H ` {A}) = A)
 
Theoremhsupunss 9589 The union of a set of Hilbert space subsets is smaller than its supremum.
|- (A (_ P~H~ -> U.A (_ ( \/H ` A))
 
Theoremspanss2 9590 A subset of Hilbert space is included in its span.
|- (A (_ H~ -> A (_ (span` A))
 
Theoremshsupunss 9591 The union of a set of subspaces is smaller than its supremum.
|- (A (_ SH -> U.A (_ (span` U.A))
 
Theoremchsupunss 9592 The union of a set of closed subspaces is smaller than its supremum.
|- (A (_ CH -> U.A (_ ( \/H ` A))
 
Theoremspanid 9593 A subspace of Hilbert space is its own span.
|- (A e. SH -> (span` A) = A)
 
Theoremspanss 9594 Ordering relationship for the spans of subsets of Hilbert space.
|- ((B (_ H~ /\ A (_ B) -> (span` A) (_ (span` B))
 
Theoremspanssoc 9595 The span of a subset of Hilbert space is less than or equal to its closure (double orthogonal complement).
|- (A (_ H~ -> (span` A) (_ (_|_` (_|_`
 A)))
 
Theoremsshjval 9596 Value of join for subsets of Hilbert space.
|- ((A (_ H~ /\ B (_ H~) -> (A vH B) = (_|_` (_|_` (A u. B))))
 
Theoremshjval 9597 Value of join in SH.
|- ((A e. SH /\ B e. SH) -> (A vH B) = (_|_` (_|_`
 (A u. B))))
 
Theoremchjval 9598 Value of join in CH.
|- ((A e. CH /\ B e. CH) -> (A vH B) = (_|_` (_|_`
 (A u. B))))
 
Theoremchjvali 9599 Value of join in CH.
|- A e. CH   &   |- B e. CH   =>   |- (A vH B) = (_|_` (_|_` (A u. B)))
 
Theoremdfchj2 9600 Alternate definition of join in the set of closed subspaces of Hilbert space CH.
|- vH = {<.<.x, y>., z>. | ((x (_ H~ /\ y (_ H~) /\ z = |^|{w e. CH | (x u. y) (_ w})}

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