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Statement List for Metamath Proof Explorer - 10001-10100 - Page 101 of 108
TypeLabelDescription
Statement
 
Theoremcnlnadjlem7 10001 Lemma for cnlnadj 10004. Helper lemma to show that F is continuous.
 
Theoremcnlnadjlem8 10002 Lemma for cnlnadj 10004. F is continuous.
 
Theoremcnlnadjlem9 10003 Lemma for cnlnadj 10004. F provides an example showing the existence of a continuous linear adjoint.
 
Theoremcnlnadj 10004 Every continuous linear operator has an adjoint. Theorem 3.10 of [Beran] p. 104.
|- T e. LinOp   &   |- T e. ConOp   =>   |- E.t e. (LinOp i^i ConOp)A.x e. H~ A.y e. H~ ((T` x) .ih y) = (x .ih (t` y))
 
Theoremcnlnadjeu 10005 Every continuous linear operator has a unique adjoint. Theorem 3.10 of [Beran] p. 104.
|- T e. LinOp   &   |- T e. ConOp   =>   |- E!t e. (LinOp i^i ConOp)A.x e. H~ A.y e. H~ ((T` x) .ih y) = (x .ih (t` y))
 
Theoremcnlnadjeut 10006 Every continuous linear operator has a unique adjoint. Theorem 3.10 of [Beran] p. 104.
|- (T e. (LinOp i^i ConOp) -> E!t e. (LinOp i^i ConOp)A.x e. H~ A.y e. H~ ((T` x) .ih y) = (x .ih (t` y)))
 
Theoremcnlnadjt 10007 Every continuous linear operator has an adjoint. Theorem 3.10 of [Beran] p. 104.
|- (T e. (LinOp i^i ConOp) -> E.t e. (LinOp i^i ConOp)A.x e. H~ A.y e. H~ ((T` x) .ih y) = (x .ih (t` y)))
 
Theoremcnlnssadj 10008 Every continuous linear Hilbert space operator has an adjoint.
|- (LinOp i^i ConOp) (_ dom adjh
 
Theorembdopssadj 10009 Every bounded linear Hilbert space operator has an adjoint.
|- BndLinOp (_ dom adjh
 
Theorembdopadjt 10010 Every bounded linear Hilbert space operator has an adjoint.
|- (T e. BndLinOp -> T e. dom adjh)
 
Theoremadjbdlnt 10011 The adjoint of a bounded linear operator is a bounded linear operator.
|- (T e. BndLinOp -> (adjh` T) e. BndLinOp)
 
Theoremadjbdlnb 10012 An operator is bounded and linear iff its adjoint is.
|- (T e. BndLinOp <-> (adjh` T) e. BndLinOp)
 
Theoremadjbd1o 10013 The mapping of adjoints of bounded linear operators is one-to-one onto.
|- (adjh |` BndLinOp):BndLinOp-1-1-onto->BndLinOp
 
Theoremadjlnopt 10014 The adjoint of an operator is linear. Proposition 1 of [AkhiezerGlazman] p. 80.
|- (T e. dom adjh -> (adjh` T) e. LinOp)
 
Theoremadjsslnop 10015 Every operator with an adjoint is linear.
|- dom adjh (_ LinOp
 
Theoremnmopadjle 10016 Property of the norm of an adjoint. Part of proof of Theorem 3.10 of [Beran] p. 104.
|- T e. BndLinOp   =>   |- (A e. H~ -> (normh` ((adjh` T)` A)) <_ ((normop` T) x. (normh` A)))
 
Theoremnmopadjlem 10017 Lemma for nmopadj 10018.
 
Theoremnmopadj 10018 Property of the norm of an adjoint. Theorem 3.11(v) of [Beran] p. 106.
|- T e. BndLinOp   =>   |- (normop` (adjh` T)) = (normop` T)
 
Theoremadjeq0 10019 An operator is zero iff its adjoint is zero. Theorem 3.11(i) of [Beran] p. 106.
|- (T = 0hop <-> (adjh` T) = 0hop)
 
Theoremadjmult 10020 The adjoint of the scalar product of an operator. Theorem 3.11(ii) of [Beran] p. 106.
|- ((A e. CC /\ T e. dom adjh) -> (adjh` (A .op T)) = ((*` A) .op (adjh` T)))
 
Theoremadjaddt 10021 The adjoint of the sum of two operators. Theorem 3.11(iii) of [Beran] p. 106.
|- ((S e. dom adjh /\ T e. dom adjh) -> (adjh` (S +op T)) = ((adjh` S) +op (adjh` T)))
 
Theoremnmoptri 10022 Triangle inequality for the norms of bounded linear operators.
|- S e. BndLinOp   &   |- T e. BndLinOp   =>   |- (normop` (S +op T)) <_ ((normop` S) + (normop` T))
 
Theoremnmopco 10023 Upper bound for the norm of the composition of two bounded linear operators.
|- S e. BndLinOp   &   |- T e. BndLinOp   =>   |- (normop` (S o. T)) <_ ((normop` S) x. (normop` T))
 
Theorembdophs 10024 The sum of two bounded linear operators is a bounded linear operator.
|- S e. BndLinOp   &   |- T e. BndLinOp   =>   |- (S +op T) e. BndLinOp
 
Theorembdophd 10025 The difference between two bounded linear operators is bounded.
|- S e. BndLinOp   &   |- T e. BndLinOp   =>   |- (S -op T) e. BndLinOp
 
Theorembdopco 10026 The composition of two bounded linear operators is bounded.
|- S e. BndLinOp   &   |- T e. BndLinOp   =>   |- (S o. T) e. BndLinOp
 
Theoremnmoptri2 10027 Triangle-type inequality for the norms of bounded linear operators.
|- S e. BndLinOp   &   |- T e. BndLinOp   =>   |- ((normop` S) - (normop` T)) <_ (normop` (S +op T))
 
Theoremadjco 10028 The adjoint of a composition of bounded linear operators. Theorem 3.11(viii) of [Beran] p. 106.
|- S e. BndLinOp   &   |- T e. BndLinOp   =>   |- (adjh` (S o. T)) = ((adjh` T) o. (adjh` S))
 
Theoremnmopcoadj 10029 The norm of an operator composed with its adjoint. Part of Theorem 3.11(vi) of [Beran] p. 106.
|- T e. BndLinOp   =>   |- (normop` ((adjh` T) o. T)) = ((normop` T)^2)
 
Theoremnmopcoadj2 10030 The norm of an operator composed with its adjoint. Part of Theorem 3.11(vi) of [Beran] p. 106.
|- T e. BndLinOp   =>   |- (normop` (T o. (adjh` T))) = ((normop` T)^2)
 
Theoremnmopcoadj0 10031 An operator composed with its adjoint is zero iff the operator is zero. Theorem 3.11(vii) of [Beran] p. 106.
|- T e. BndLinOp   =>   |- ((T o. (adjh` T)) = 0hop <-> T = 0hop)
 
Quantum computation error bound theorem
 
Theoremunierr 10032 If we approximate a chain of unitary transformations (quantum computer gates) F, G by other unitary transformations S, T, the error increases at most additively. Equation 4.73 of [NielsenChuang] p. 195.
|- F e. UniOp   &   |- G e. UniOp   &   |- S e. UniOp   &   |- T e. UniOp   =>   |- (normop` ((F o. G) -op (S o. T))) <_ ((normop` (F -op S)) + (normop` (G -op T)))
 
Dirac bra-ket notation (cont.)
 
Theorembranmfnt 10033 The norm of the bra function.
|- (A e. H~ -> (normfn` (bra` A)) = (normh` A))
 
Theorembrabnt 10034 The bra of a vector is a bounded functional.
|- (A e. H~ -> (normfn` (bra` A)) e. RR)
 
Theoremrnbra 10035 The set of bras equals the set of continuous linear functionals.
|- ran bra = (LinFn i^i ConFn)
 
Theorembra11 10036 The bra function maps vectors one-to-one onto the set of continuous linear functionals.
|- bra:H~-1-1-onto->(LinFn i^i ConFn)
 
Theorembracnlnt 10037 A bra is a continuous linear functional.
|- (A e. H~ -> (bra` A) e. (LinFn i^i ConFn))
 
Theoremcnvbravalt 10038 Value of the converse of the bra function. Based on the Riesz Lemma riesz4t 9992, this very important theorem not only justifies the Dirac bra-ket notation, but allows us to extract a unique vector from any continuous linear functional from which the functional can be recovered; i.e. a single vector can "store" all of the information contained in any entire continuous linear functional (mapping from H~ to CC).
|- (T e. (LinFn i^i ConFn) -> (`'bra` T) = U.{y e. H~ | A.x e. H~ (T` x) = (x .ih y)})
 
Theoremcnvbraclt 10039 Closure of the converse of the bra function.
|- (T e. (LinFn i^i ConFn) -> (`'bra` T) e. H~)
 
Theoremcnvbrabrat 10040 The converse bra of the bra of a vector is the vector itself.
|- (A e. H~ -> (`'bra` (bra` A)) = A)
 
Theorembracnvbrat 10041 The bra of the converse bra of a continuous linear functional.
|- (T e. (LinFn i^i ConFn) -> (bra` (`'bra` T)) = T)
 
Theorembracnlnvalt 10042 The vector that a continuous linear functional is the bra of.
|- (T e. (LinFn i^i ConFn) -> T = (bra` U.{y e. H~ | A.x e. H~ (T` x) = (x .ih y)}))
 
Theoremcnvbramult 10043 Multiplication property of the converse bra function.
|- ((A e. CC /\ T e. (LinFn i^i ConFn)) -> (`'bra` (A .fn T)) = ((*` A) .h (`'bra` T)))
 
Theoremkbass1t 10044 Dirac bra-ket associative law ( | A>. <.B | ) | C>. = | A>.(<.B | C>.) i.e. the juxtaposition of an outer product with a ket equals a bra juxtaposed with an inner product. Since <.B | C>. is a complex number, it is the first argument in the inner product .h that it is mapped to, although in Dirac notation it is placed after the ket.
|- ((A e. H~ /\ B e. H~ /\ C e. H~) -> ((A ketbra B)` C) = (((bra` B)` C) .h A))
 
Theoremkbass2t 10045 Dirac bra-ket associative law (<.A | B>.)<.C | = <.A | ( | B>. <.C | ) i.e. the juxtaposition of an inner product with a bra equals a ket juxtaposed with an outer product.
|- ((A e. H~ /\ B e. H~ /\ C e. H~) -> (((bra` A)` B) .fn (bra` C)) = ((bra` A) o. (B ketbra C)))
 
Theoremkbass3t 10046 Dirac bra-ket associative law <.A | B>. <.C | D>. = (<.A | B>. <.C | ) | D>..
|- (((A e. H~ /\ B e. H~) /\ (C e. H~ /\ D e. H~)) -> (((bra` A)` B) x. ((bra` C)` D)) = ((((bra` A)` B) .fn (bra` C))` D))
 
Theoremkbass4t 10047 Dirac bra-ket associative law <.A | B>. <.C | D>. = <.A | ( | B>. <.C | D>.).
|- (((A e. H~ /\ B e. H~) /\ (C e. H~ /\ D e. H~)) -> (((bra` A)` B) x. ((bra` C)` D)) = ((bra` A)` (((bra` C)` D) .h B)))
 
Theoremkbass5t 10048 Dirac bra-ket associative law ( | A>. <.B | )( | C>. <.D | ) = (( | A>. <.B | ) | C>.)<.D |.
|- (((A e. H~ /\ B e. H~) /\ (C e. H~ /\ D e. H~)) -> ((A ketbra B) o. (C ketbra D)) = (((A ketbra B)` C) ketbra D))
 
Theoremkbass6t 10049 Dirac bra-ket associative law ( | A>. <.B | )( | C>. <.D | ) = | A>. (<.B | ( | C>. <.D | )).
|- (((A e. H~ /\ B e. H~) /\ (C e. H~ /\ D e. H~)) -> ((A ketbra B) o. (C ketbra D)) = (A ketbra (`'bra` ((bra` B) o. (C ketbra D)))))
 
Positive operators (cont.)
 
Theoremleopg 10050 Ordering relation for positive operators. Definition of positive operator ordering in [Kreyszig] p. 470.
|- ((T e. A /\ U e. B) -> (T <_op U <-> ((U -op T) e. HrmOp /\ A.x e. H~ 0 <_ (((U -op T)` x) .ih x))))
 
Theoremleopt 10051 Ordering relation for operators. Definition of positive operator ordering in [Kreyszig] p. 470.
|- ((T e. HrmOp /\ U e. HrmOp) -> (T <_op U <-> A.x e. H~ 0 <_ (((U -op T)` x) .ih x)))
 
Theoremleop2t 10052 Ordering relation for operators. Definition of operator ordering in [Young] p. 141.
|- ((T e. HrmOp /\ U e. HrmOp) -> (T <_op U <-> A.x e. H~ ((T` x) .ih x) <_ ((U` x) .ih x)))
 
Theoremleop3t 10053 Operator ordering in terms of a positive operator. Definition of operator ordering in [Retherford] p. 49.
|- ((T e. HrmOp /\ U e. HrmOp) -> (T <_op U <-> 0hop <_op (U -op T)))