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Statement List for Metamath Proof Explorer - 11201-11300 - Page 113 of 175
TypeLabelDescription
Statement
 
Theoremcm2ji 11201 A lattice element that commutes with two others also commutes with their join. Theorem 4.2 of [Beran] p. 49.
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- A C_H B   &   |- A C_H C   =>   |- A C_H (B vH C)
 
Theoremcm2mi 11202 A lattice element that commutes with two others also commutes with their meet. Theorem 4.2 of [Beran] p. 49.
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- A C_H B   &   |- A C_H C   =>   |- A C_H (B i^i C)
 
Quantum Logic Explorer axioms
 
Theoremqlax1i 11203 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))
 
Theoremqlax2i 11204 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)
 
Theoremqlax3i 11205 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))
 
Theoremqlax4i 11206 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))
 
Theoremqlax5i 11207 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
 
Theoremqlaxr1i 11208 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
 
Theoremqlaxr2i 11209 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
 
Theoremqlaxr4i 11210 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)
 
Theoremqlaxr5i 11211 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)
 
Theoremqlaxr3i 11212 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
 
Orthogonal subspaces
 
Theoremosumlem1 11213 Lemma for osumi 11221.
 
Theoremosumlem2 11214 Lemma for osumi 11221.
 
Theoremosumlem3 11215 Lemma for osumi 11221.
 
Theoremosumlem4 11216 Lemma for osumi 11221.
 
Theoremosumlem5 11217 Lemma for osumi 11221.
 
Theoremosumlem6 11218 Lemma for osumi 11221.
 
Theoremosumlem7 11219 Lemma for osumi 11221.
 
Theoremosumlem8 11220 Lemma for osumi 11221.
 
Theoremosumi 11221 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 11217 and via pjpjth 10891 in osumlem7 11219).
|- A e. CH   &   |- B e. CH   =>   |- (A C_ (_|_` B) -> (A +H B) = (A vH B))
 
Theoremosumcori 11222 Corollary of osumi 11221.
|- A e. CH   &   |- B e. CH   =>   |- ((A i^i B) +H (A i^i (_|_` B))) = ((A i^i B) vH (A i^i (_|_` B)))
 
Theoremosum 11223 If two closed subspaces of a Hilbert space are orthogonal, their subspace sum equals their subspace join. Lemma 3 of [Kalmbach] p. 67.
|- ((A e. CH /\ B e. CH /\ A C_ (_|_`
 B)) -> (A +H B) = (A vH B))
 
Theoremchso 11224 The subspace sum of a closed subspace and its complement is all of Hilbert space.
|- (A e. CH -> (A +H (_|_` A)) = ~H)
 
Theoremosumcor2i 11225 Corollary of osumi 11221, showing it holds under the weaker hypothesis that A and B commute.
|- A e. CH   &   |- B e. CH   =>   |- (A C_H B -> (A +H B) = (A vH B))
 
Theoremspansnji 11226 The subspace sum of a closed subspace and a one-dimensional subspace equals their join. (Proof suggested by Eric Schechter 1-Jun-2004.)
|- A e. CH   &   |- B e. ~H   =>   |- (A +H (span` {B})) = (A vH (span` {B}))
 
Theoremspansnj 11227 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})))
 
Theoremspansnscl 11228 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)
 
Theoremsumspansn 11229 The sum of two vectors belong to the span of one of them iff the other vector also belongs.
|- ((A e. ~H /\ B e. ~H) -> ((A +h B) e. (span` {A}) <-> B e. (span` {A})))
 
Theoremspansnm0i 11230 The meet of different one-dimensional subspaces is the zero subspace.
|- A e. ~H   &   |- B e. ~H   =>   |- (-. A e. (span` {B}) -> ((span` {A}) i^i (span` {B})) = 0H)
 
Theoremnonbooli 11231 A Hilbert lattice with two or more dimensions fails the distributive law and therefore cannot be a Boolean algebra. This counterexample demonstrates a condition where ((H i^i F) vH (H i^i G)) = 0H but (H i^i (F vH G)) =/= 0H. The antecedent specifies that the vectors A and B are nonzero and non-colinear. The last three hypotheses assign one-dimensional subspaces to F, G, and H.
|- A e. ~H   &   |- B e. ~H   &   |- F = (span` {A})   &   |- G = (span` {B})   &   |- H = (span` {(A +h B)})   =>   |- (-. (A e. G \/ B e. F) -> (H i^i (F vH G)) =/= ((H i^i F) vH (H i^i G)))
 
Theoremspansncvi 11232 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 C. B /\ B C_ (A vH (span` {C}))) -> B = (A vH (span` {C})))
 
Theoremspansncv 11233 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 C. B /\ B C_ (A vH (span` {C}))) -> B = (A vH (span` {C}))))
 
Orthoarguesian laws 5OA and 3OA
 
Theorem5oalem1 11234 Lemma for orthoarguesian law 5OA.
 
Theorem5oalem2 11235 Lemma for orthoarguesian law 5OA.
 
Theorem5oalem3 11236 Lemma for orthoarguesian law 5OA.
 
Theorem5oalem4 11237 Lemma for orthoarguesian law 5OA.
 
Theorem5oalem5 11238 Lemma for orthoarguesian law 5OA.
 
Theorem5oalem6 11239 Lemma for orthoarguesian law 5OA.
 
Theorem5oalem7 11240 Lemma for orthoarguesian law 5OA.
 
Theorem5oai 11241 Orthoarguesian law 5OA. This 8-variable inference is called 5OA because it can be converted to a 5-variable equation (see Quantum Logic Explorer).
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- D e. CH   &   |- F e. CH   &   |- G e. CH   &   |- R e. CH   &   |- S e. CH   &   |- A C_ (_|_` B)   &   |- C C_ (_|_`
 D)   &   |- F C_ (_|_` G)   &   |- R C_ (_|_`
 S)   =>   |- (((A vH B) i^i (C vH D)) i^i ((F vH G) i^i (R vH S))) C_ (B vH (A i^i (C vH ((((A vH C) i^i (B vH D)) i^i (((A vH R) i^i (B vH S)) vH ((C vH R) i^i (D vH S)))) i^i ((((A vH F) i^i (B vH G)) i^i (((A vH R) i^i (B vH S)) vH ((F vH R) i^i (G vH S)))) vH (((C vH F) i^i (D vH G)) i^i (((C vH R) i^i (D vH S)) vH ((F vH R) i^i (G vH S)))))))))
 
Theorem3oalem1 11242 Lemma for 3OA (weak) orthoarguesian law.
 
Theorem3oalem2 11243 Lemma for 3OA (weak) orthoarguesian law.
 
Theorem3oalem3 11244 Lemma for 3OA (weak) orthoarguesian law.
 
Theorem3oalem4 11245 Lemma for 3OA (weak) orthoarguesian law.
 
Theorem3oalem5 11246 Lemma for 3OA (weak) orthoarguesian law.
 
Theorem3oalem6 11247 Lemma for 3OA (weak) orthoarguesian law.
 
Theorem3oai 11248 3OA (weak) orthoarguesian law. Equation IV of [GodowskiGreechie] p. 249.
|- A e. CH   &   |- B e. CH   &   |- C e. CH   &   |- R = ((_|_` B) i^i (B vH A))   &   |- S = ((_|_`
 C) i^i (C vH A))   =>   |- ((B vH R) i^i (C vH S)) C_ (B vH (R i^i (S vH ((B vH C) i^i (R vH S)))))
 
Projectors (cont.)
 
Theorempjorthi 11249 Projection components on orthocomplemented subspaces are orthogonal.
|- A e. ~H   &   |- B e. ~H   =>   |- (H e. CH -> (((proj` H)` A) .ih ((proj` (_|_` H))` B)) = 0)
 
Theorempjch1 11250 Property of identity projection. Remark in [Beran] p. 111.
|- (A e. ~H -> ((proj` ~H)` A) = A)
 
Theorempjo 11251 The orthogonal projection. Lemma 4.4(i) of [Beran] p. 111.
|- ((H e. CH /\ A e. ~H) -> ((proj` (_|_` H))` A) = (((proj` ~H)` A) -h ((proj` H)` A)))
 
Theorempjidmi 11252 A projection is idempotent. Property (ii) of [Beran] p. 109.
|- H e. CH   &   |- A e. ~H   =>   |- ((proj` H)` ((proj` H)` A)) = ((proj` H)` A)
 
Theorempjadjii 11253 A projection is self-adjoint. Property (i) of [Beran] p. 109.
|- H e. CH   &   |- A e. ~H   &   |- B e. ~H   =>   |- (((proj` H)` A) .ih B) = (A .ih ((proj` H)` B))
 
Theorempjcompi 11254 Component of a projection.
|- H e. CH   &   |- A e. ~H   &   |- B e. ~H   =>   |- ((A e. H /\ B e. (_|_` H)) -> ((proj` H)` (A +h B)) = A)
 
Theorempjaddii 11255 Projection of vector sum is sum of projections.
|- H e. CH   &   |- A e. ~H   &   |- B e. ~H   =>   |- ((proj` H)` (A +h B)) = (((proj` H)` A) +h ((proj` H)` B))
 
Theorempjinormii 11256 The inner product of a projection and its argument is the square of the norm of the projection. Remark in [Halmos] p. 44.
|- H e. CH   &   |- A e. ~H   =>   |- (((proj` H)` A) .ih A) = ((normh` ((proj` H)` A))^2)
 
Theorempjmulii 11257 Projection of (scalar) product is product of projection.
|- H e. CH   &   |- A e. ~H   &   |- C e. CC   =>   |- ((proj` H)` (C .h A)) = (C .h ((proj` H)` A))
 
Theorempjsubii 11258 Projection of vector difference is difference of projections.
|- H e. CH   &   |- A e. ~H   &   |- B e. ~H   =>   |- ((proj` H)` (A -h B)) = (((proj` H)` A) -h ((proj` H)` B))
 
Theorempjsslem 11259 Lemma for subset relationships of projections.
 
Theorempjss2i 11260 Subset relationship for projections. Theorem 4.5(i)->(ii) of [Beran] p. 112.
|- H e. CH   &   |- A e. ~H   &   |- G e. CH   =>   |- (H C_ G -> ((proj` H)` ((proj` G)` A)) = ((proj` H)` A))
 
Theorempjssmii 11261 Projection meet property. Remark in [Kalmbach] p. 66. Also Theorem 4.5(i)->(iv) of [Beran] p. 112.
|- H e. CH   &   |- A e. ~H   &   |- G e. CH   =>   |- (H C_ G -> (((proj` G)` A) -h ((proj` H)` A)) = ((proj` (G i^i (_|_` H)))` A))
 
Theorempjssge0ii 11262 Theorem 4.5(iv)->(v) of [Beran] p. 112.
|- H e. CH   &   |- A e. ~H   &   |- G e. CH   =>   |- ((((proj` G)` A) -h ((proj` H)` A)) = ((proj` (G i^i (_|_` H)))` A) -> 0 <_ ((((proj` G)` A) -h ((proj` H)` A)) .ih A))
 
Theorempjdifnormii 11263 Theorem 4.5(v)<->(vi) of [Beran] p. 112.
|- H e. CH   &   |- A e. ~H   &   |- G e. CH   =>   |- (0 <_ ((((proj` G)` A) -h ((proj` H)` A)) .ih A) <-> (normh` ((proj` H)` A)) <_ (normh` ((proj` G)` A)))
 
Theorempjcji 11264 The projection on a subspace join is the sum of the projections.
|- H e. CH   &   |- A e. ~H   &   |- G e. CH   =>   |- (H C_ (_|_` G) -> ((proj` (H vH G))` A) = (((proj` H)` A) +h ((proj` G)` A)))
 
Theorempjadji 11265 A projection is self-adjoint. Property (i) of [Beran] p. 109.
|- H e. CH   =>   |- ((A e. ~H /\ B e. ~H) -> (((proj` H)` A) .ih B) = (A .ih ((proj` H)` B)))
 
Theorempjaddi 11266 Projection of vector sum is sum of projections.
|- H e. CH   =>   |- ((A e. ~H /\ B e. ~H) -> ((proj` H)` (A +h B)) = (((proj` H)` A) +h ((proj` H)` B)))
 
Theorempjinormi 11267 The inner product of a projection and its argument is the square of the norm of the projection. Remark in [Halmos] p. 44.
|- H e. CH   =>   |- (A e. ~H -> (((proj` H)` A) .ih A) = ((normh` ((proj` H)` A))^2))
 
Theorempjsubi 11268 Projection of vector difference is difference of projections.
|- H e. CH   =>   |- ((A e. ~H /\ B e. ~H) -> ((proj` H)` (A -h B)) = (((proj` H)` A) -h ((proj` H)` B)))
 
Theorempjmuli 11269 Projection of scalar product is scalar product of projection.
|- H e. CH   =>   |- ((A e. CC /\ B e. ~H) -> ((proj` H)` (A .h B)) = (A .h ((proj` H)` B)))
 
Theorempjige0i 11270 The inner product of a projection and its argument is nonnegative.
|- H e. CH   =>   |- (A e. ~H -> 0 <_ (((proj` H)` A) .ih A))
 
Theorempjige0 11271 The inner product of a projection and its argument is nonnegative.
|- ((H e. CH /\ A e. ~H) -> 0 <_ (((proj` H)` A) .ih A))
 
Theorempjcjt2 11272 The projection on a subspace join is the sum of the projections.
|- ((H e. CH /\ G e. CH /\ A e. ~H) -> (H C_ (_|_` G) -> ((proj` (H vH G))` A) = (((proj` H)` A) +h ((proj` G)` A))))
 
Theorempj0i 11273 The projection of the zero vector.
|- H e. CH   =>   |- ((proj` H)` 0h) = 0h
 
Theorempjch 11274 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))
 
Theorempjid 11275 The projection of a vector in the projection subspace is itself.
|- ((H e. CH /\ A e. H) -> ((proj` H)` A) = A)
 
Theorempjvec 11276 The set of vectors belonging to the subspace of a projection. Part of Theorem 26.2 of [Halmos] p. 44.
|- (H e. CH -> H = {x e. ~H | ((proj` H)` x) = x})
 
Theorempjocvec 11277 The set of vectors belonging to the orthocomplemented subspace of a projection. Second part of Theorem 27.3 of [Halmos] p. 45.
|- (H e. CH -> (_|_` H) = {x e. ~H | ((proj` H)` x) = 0h})
 
Theorempjocini 11278 Membership of projection in orthocomplement of intersection.
|- G e. CH   &   |- H e. CH   =>   |- (A e. (_|_` (G i^i H)) -> ((proj` G)` A) e. (_|_` (G i^i H)))
 
Theorempjini 11279 Membership of projection in an intersection.
|- G e. CH   &   |- H e. CH   =>   |- (A e. (G i^i H) -> ((proj` G)` A) e. (G i^i H))
 
Theorempjjsi 11280 A sufficient condition for subspace join to be equal to subspace sum.
|- G e. CH   &   |- H e. SH   =>   |- (A.x e. (G vH H)((proj` (_|_` G))` x) e. H -> (G vH H) = (G +H H))
 
Theorempjfni 11281 Functionality of a projection.
|- H e. CH   =>   |- (proj` H) Fn ~H
 
Theorempjrni 11282 The range of a projection. Part of Theorem 26.2 of [Halmos] p. 44.
|- H e. CH   =>   |- ran (proj` H) = H
 
Theorempjfoi 11283 A projection maps onto its subspace.
|- H e. CH   =>   |- (proj` H):~H-onto->H
 
Theorempjfi 11284 The mapping of a projection.
|- H e. CH   =>   |- (proj` H):~H-->~H
 
Theorempjvi 11285 The value of a projection in terms of components.
|- H e. CH   =>   |- ((A e. H /\ B e. (_|_` H)) -> ((proj` H)` (A +h B)) = A)
 
Theorempjfo 11286 A projection maps onto its subspace.
|- (H e. CH -> (proj` H):~H-onto->H)
 
Theorempjrn 11287 The range of a projection. Part of Theorem 26.2 of [Halmos] p. 44.
|- (H e. CH -> ran (proj` H) = H)
 
Theorempjf 11288 The mapping of a projection.
|- (H e. CH -> (proj` H):~H-->~H)
 
Theorempjfn 11289 Functionality of a projection.
|- (H e. CH -> (proj` H) Fn ~H)
 
Theorempjsumi 11290 The projection on a subspace sum is the sum of the projections.
|- G e. CH   &   |- H e. CH   =>   |- (A e. ~H -> (G C_ (_|_`
 H) -> ((proj` (G +H H))` A) = (((proj` G)` A) +h ((proj` H)` A))))
 
Theorempj11i 11291 One-to-one correspondence of projection and subspace.
|- G e. CH   &   |- H e. CH   =>   |- ((proj` G) = (proj` H) <-> G = H)
 
Theorempjdsi 11292 Vector decomposition into sum of projections on orthogonal subspaces.
|- G e. CH   &   |- H e. CH   =>   |- ((A e. (G vH H) /\ G C_ (_|_`
 H)) -> A = (((proj` G)` A) +h ((proj` H)` A)))
 
Theorempjds3i 11293 Vector decomposition into sum of projections on orthogonal subspaces.
|- F e. CH   &   |- G e. CH   &   |- H e. CH   =>   |- (((A e. ((F vH G) vH H) /\ F C_ (_|_` G)) /\ (F C_ (_|_` H) /\ G C_ (_|_` H))) -> A = ((((proj` F)` A) +h ((proj` G)` A)) +h ((proj` H)` A)))
 
Theorempj11 11294 One-to-one correspondence of projection and subspace.
|- ((G e. CH /\ H e. CH) -> ((proj` G) = (proj` H) <-> G = H))
 
Theorempjmfn 11295 Functionality of the projection function.
|- proj Fn CH
 
Theorempjmf1 11296 The projector function maps one-to-one into the set of Hilbert space operators.
|- proj:CH-1-1->(~H ^m ~H)
 
Theorempjoi0 11297 The inner product of projections on orthogonal subspaces vanishes.
|- (((G e. CH /\ H e. CH /\ A e. ~H) /\ G C_ (_|_` H)) -> (((proj` G)` A) .ih ((proj` H)` A)) = 0)
 
Theorempjoi0i 11298 The inner product of projections on orthogonal subspaces vanishes.
|- G e. CH   &   |- H e. CH   &   |- A e. ~H   =>   |- (G C_ (_|_` H) -> (((proj` G)` A) .ih ((proj` H)` A)) = 0)
 
Theorempjopythi 11299 Pythagorean theorem for projections on orthogonal subspaces.
|- G e. CH   &   |- H e. CH   &   |- A e. ~H   =>   |- (G C_ (_|_` H) -> ((normh` (((proj` G)` A) +h ((proj` H)` A)))^2) = (((normh` ((proj` G)` A))^2) + ((normh` ((proj` H)` A))^2)))
 
Theorempjopyth 11300 Pythagorean theorem for projections on orthogonal subspaces.
|- ((H e. CH /\ G e. CH /\ A e. ~H) -> (H C_ (_|_` G) -> ((normh` (((proj` H)` A) +h ((proj` G)` A)))^2) = (((normh` ((proj` H)` A))^2) + ((normh` ((proj` G)` A))^2))))

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