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Statement List for Metamath Proof Explorer - 10101-10200 - Page 102 of 108
TypeLabelDescription
Statement
 
Theorempjocco 10101 Composition of projections of a subspace and its orthocomplement.
|- H e. CH   =>   |- ((proj` H) o. (proj` (_|_` H))) = 0hop
 
Theorempjtot 10102 Subspace sum of projection and projection of orthocomplement.
|- H e. CH   =>   |- ((proj` H) +op (proj` (_|_` H))) = (proj` H~)
 
Theorempjoc 10103 Projection of orthocomplement. First part of Theorem 27.3 of [Halmos] p. 45.
|- H e. CH   =>   |- ((proj` H~) -op (proj` H)) = (proj` (_|_` H))
 
Theorempjidmcot 10104 A projection operator is idempotent. Property (ii) of [Beran] p. 109.
|- (H e. CH -> ((proj` H) o. (proj` H)) = (proj` H))
 
Theorempjhmopidm 10105 Two ways to express the set of all projection operators.
|- ran proj = (HrmOp i^i {t | (t o. t) = t})
 
Theoremdfpjopt 10106 Definition of projection operator in [Hughes] p. 47, except that we do not need linearity to be explicit by virtue of hmoplint 9861.
|- (T e. ran proj <-> (T e. HrmOp /\ (T o. T) = T))
 
Theoremelpjidmt 10107 A projection operator is idempotent. Part of Theorem 26.1 of [Halmos] p. 43.
|- (T e. ran proj -> (T o. T) = T)
 
Theoremelpjhmopt 10108 A projection operator is Hermitian. Part of Theorem 26.1 of [Halmos] p. 43.
|- (T e. ran proj -> T e. HrmOp)
 
Theorempjadj2t 10109 A projector is self-adjoint. Property (i) of [Beran] p. 109.
|- (T e. ran proj -> (adjh` T) = T)
 
Theorempjadj3t 10110 A projector is self-adjoint. Property (i) of [Beran] p. 109.
|- (H e. CH -> (adjh` (proj` H)) = (proj` H))
 
Theoremelpjcht 10111 Reconstruction of the subspace of a projection operator. Part of Theorem 26.2 of [Halmos] p. 44.
|- (T e. ran proj -> ({x e. H~ | (T` x) = x} e. CH /\ T = (proj` {x e. H~ | (T` x) = x})))
 
Theoremelpjrnt 10112 Reconstruction of the subspace of a projection operator.
|- (T e. ran proj -> ran T = {x e. H~ | (T` x) = x})
 
Theoremelpjrncht 10113 Reconstruction of the subspace of a projection operator.
|- (T e. ran proj -> (ran T e. CH /\ T = (proj` ran T)))
 
Theorempjinvar 10114 A closed subspace H with projection T is invariant under an operator S iff ST = TST. Theorem 27.1 of [Halmos] p. 45.
|- S:H~-->H~   &   |- H e. CH   &   |- T = (proj` H)   =>   |- ((S o. T):H~-->H <-> (S o. T) = (T o. (S o. T)))
 
Theorempjin1 10115 Lemma for Theorem 1.22 of Mittelstaedt, p. 20.
 
Theorempjin2 10116 Lemma for Theorem 1.22 of Mittelstaedt, p. 20.
 
Theorempjin3 10117 Lemma for Theorem 1.22 of Mittelstaedt, p. 20.
 
Theorempjclem1 10118 Lemma for projection commutation theorem.
 
Theorempjclem2 10119 Lemma for projection commutation theorem.
 
Theorempjclem3 10120 Lemma for projection commutation theorem.
 
Theorempjclem4a 10121 Lemma for projection commutation theorem.
 
Theorempjclem4 10122 Lemma for projection commutation theorem.
 
Theorempjc 10123 Two subspaces commute iff their projections commute. Lemma 4 of [Kalmbach] p. 67.
|- G e. CH   &   |- H e. CH   =>   |- (G C_H H <-> ((proj` G) o. (proj` H)) = ((proj` H) o. (proj` G)))
 
Theorempjcmmul1 10124 A necessary and sufficient condition for the product of two projectors to be a projector is that the projectors commute. Part 1 of Theorem 1 of [AkhiezerGlazman] p. 65.
|- G e. CH   &   |- H e. CH   =>   |- (((proj` G) o. (proj` H)) = ((proj` H) o. (proj` G)) <-> ((proj` G) o. (proj` H)) e. ran proj)
 
Theorempjcmmul2 10125 The projection subspace of the difference between two projectors. Part 2 of Theorem 1 of [AkhiezerGlazman] p. 65.
|- G e. CH   &   |- H e. CH   =>   |- (((proj` G) o. (proj` H)) = ((proj` H) o. (proj` G)) <-> ((proj` G) o. (proj` H)) = (proj` (G i^i H)))
 
Theorempjcohocl 10126 Closure of composition of projection and Hilbert space operator.
|- H e. CH   &   |- T:H~-->H~   =>   |- (A e. H~ -> (((proj` H) o. T)` A) e. H)
 
Theorempjadj2co 10127 Adjoint of double composition of projections. Generalization of special case of Theorem 3.11(viii) of [Beran] p. 106.
|- F e. CH   &   |- G e. CH   &   |- H e. CH   =>   |- ((A e. H~ /\ B e. H~) -> (((((proj` F) o. (proj` G)) o. (proj` H))` A) .ih B) = (A .ih ((((proj` H) o. (proj` G)) o. (proj` F))` B)))
 
Theorempj2cocl 10128 Closure of double composition of projections.
|- F e. CH   &   |- G e. CH   &   |- H e. CH   =>   |- (A e. H~ -> ((((proj` F) o. (proj` G)) o. (proj` H))` A) e. F)
 
Theorempj3lem1 10129 Lemma for projection triplet theorem.
 
Theorempj3s 10130 Stronger projection triplet theorem.
|- F e. CH   &   |- G e. CH   &   |- H e. CH   =>   |- (((((proj` F) o. (proj` G)) o. (proj` H)) = (((proj` H) o. (proj` G)) o. (proj` F)) /\ ran (((proj` F) o. (proj` G)) o. (proj` H)) (_ G) -> (((proj` F) o. (proj` G)) o. (proj` H)) = (proj` ((F i^i G) i^i H)))
 
Theorempj3 10131 Projection triplet theorem.
|- F e. CH   &   |- G e. CH   &   |- H e. CH   =>   |- (((((proj` F) o. (proj` G)) o. (proj` H)) = (((proj` H) o. (proj` G)) o. (proj` F)) /\ (((proj` F) o. (proj` G)) o. (proj` H)) = (((proj` G) o. (proj` F)) o. (proj` H))) -> (((proj` F) o. (proj` G)) o. (proj` H)) = (proj` ((F i^i G) i^i H)))
 
Theorempj3cor1 10132 Projection triplet corollary.
|- F e. CH   &   |- G e. CH   &   |- H e. CH   =>   |- (((((proj` F) o. (proj` G)) o. (proj` H)) = (((proj` H) o. (proj` G)) o. (proj` F)) /\ (((proj` F) o. (proj` G)) o. (proj` H)) = (((proj` G) o. (proj` F)) o. (proj` H))) -> (((proj` F) o. (proj` G)) o. (proj` H)) = (((proj` H) o. (proj` F)) o. (proj` G)))
 
Theorempjs14 10133 Theorem S-14 of Watanabe, p. 486.
|- G e. CH   &   |- H e. CH   =>   |- (A e. H~ -> (normh` (((proj` H) o. (proj` G))` A)) <_ (normh` ((proj` G)` A)))
 
States on a Hilbert lattice
 
Definitiondf-st 10134 Define the set of states on a Hilbert lattice. Definition of [Kalmbach] p. 266.
|- States = {f | ((f:CH-->RR /\ A.x e. CH (0 <_ (f` x) /\ (f` x) <_ 1)) /\ ((f` H~) = 1 /\ A.x e. CH A.y e. CH (x (_ (_|_` y) -> (f` (x vH y)) = ((f` x) + (f` y)))))}
 
Definitiondf-hst 10135 Define the set of complex Hilbert-space-valued states on a Hilbert lattice. Definition of CH-states in [Mayet3] p. 9.
|- CHStates = {f | (f:CH-->H~ /\ (normh` (f` H~)) = 1 /\ A.x e. CH A.y e. CH (x (_ (_|_` y) -> (((f` x) .ih (f` y)) = 0 /\ (f` (x vH y)) = ((f` x) +h (f` y)))))}
 
Theoremstelt 10136 Property of a state.
|- (S e. States <-> ((S:CH-->RR /\ A.x e. CH (0 <_ (S` x) /\ (S` x) <_ 1)) /\ ((S` H~) = 1 /\ A.x e. CH A.y e. CH (x (_ (_|_` y) -> (S` (x vH y)) = ((S` x) + (S` y))))))
 
Theoremhstelt 10137 Property of a complex Hilbert-space-valued state. Definition of CH-states in [Mayet3] p. 9.
|- (S e. CHStates <-> (S:CH-->H~ /\ (normh` (S` H~)) = 1 /\ A.x e. CH A.y e. CH (x (_ (_|_` y) -> (((S` x) .ih (S` y)) = 0 /\ (S` (x vH y)) = ((S` x) +h (S` y))))))
 
Theoremstclt 10138 Real closure of the value of a state.
|- (S e. States -> (A e. CH -> (S` A) e. RR))
 
Theoremhstclt 10139 Closure of the value of a Hilbert-space-valued state.
|- ((S e. CHStates /\ A e. CH) -> (S` A) e. H~)
 
Theoremhst1t 10140 Unit value of a Hilbert-space-valued state.
|- (S e. CHStates -> (normh` (S` H~)) = 1)
 
Theoremhstel2t 10141 Properties of a Hilbert-space-valued state.
|- (((S e. CHStates /\ A e. CH) /\ (B e. CH /\ A (_ (_|_` B))) -> (((S` A) .ih (S` B)) = 0 /\ (S` (A vH B)) = ((S` A) +h (S` B))))
 
Theoremhstortht 10142 Orthogonality property of a Hilbert-space-valued state. This is a key feature distinguishing it from a real-valued state.
|- (((S e. CHStates /\ A e. CH) /\ (B e. CH /\ A (_ (_|_` B))) -> ((S` A) .ih (S` B)) = 0)
 
Theoremhstosumt 10143 Orthogonal sum property of a Hilbert-space-valued state.
|- (((S e. CHStates /\ A e. CH) /\ (B e. CH /\ A (_ (_|_` B))) -> (S` (A vH B)) = ((S` A) +h (S` B)))