Exact source: MathlibAnnex/Analysis/InnerProductSpace/UnitaryCompletion.lean, lines 121β234.
Back to Reconstructing a represented unitary from its shells and residual corner
1import MathlibAnnex.Analysis.InnerProductSpace.ProjectionShell 2 3/-! 4# Exact unitary completion from finite defect relations 5 6A fixed unitary conjugating every finite defect projection conjugates the 7limiting defect projections. If its complementary finite pieces converge 8strongly to `S`, the remaining corner `V = U P` completes `S` exactly. 9-/ 10 11set_option autoImplicit false 12 13open Filter Topology 14open scoped InnerProduct 15 16namespace ContinuousLinearMap 17 18variable {π E F : Type*} 19variable [RCLike π] 20variable [NormedAddCommGroup E] [InnerProductSpace π E] [CompleteSpace E] 21variable [NormedAddCommGroup F] [InnerProductSpace π F] [CompleteSpace F] 22 23/-- Termwise shell relations sum to the corresponding finite relation. -/ 24theorem comp_partialSum_eq_of_comp_eq 25 (e : E βL[π] F) (D : β β E βL[π] E) (W : β β E βL[π] F) 26 (h : β n, e.comp (D n) = W n) (N : β) : 27 e.comp (partialSum D N) = partialSum W N := by 28 ext x 29 simp only [partialSum, map_sum, sum_apply, 30 ContinuousLinearMap.comp_apply] 31 apply Finset.sum_congr rfl 32 intro n hn 33 exact congrArg (fun T : E βL[π] F β¦ T x) (h n) 34 35/-- Termwise shells plus a finite telescoping identity give the finite 36complement relation consumed by `unitaryCompletion_of_finite_relations`. -/ 37theorem comp_complement_eq_partialSum_of_shells 38 (e : E βL[π] F) (D : β β E βL[π] E) (W : β β E βL[π] F) 39 (U : β β Submodule π E) [β N, (U N).HasOrthogonalProjection] 40 (hshell : β n, e.comp (D n) = W n) 41 (htelescope : β N, partialSum D N = 1 - (U N).starProjection) : 42 β N, e.comp (1 - (U N).starProjection) = partialSum W N := by 43 intro N 44 rw [β htelescope] 45 exact comp_partialSum_eq_of_comp_eq e D W hshell N 46 47/-- If a unitary's complementary corner has the prescribed final defect product, 48then it conjugates the remaining projection onto the remaining final projection. -/ 49theorem unitary_conjugacy_of_complement_product 50 (e : E ββα΅’[π] F) (P : E βL[π] E) (Q : F βL[π] F) 51 (A : E βL[π] F) 52 (hPadj : Pβ = P) (hPidem : P.comp P = P) 53 (hA : (e : E βL[π] F).comp (1 - P) = A) 54 (hprod : A.comp (Aβ ) = 1 - Q) : 55 ((e : E βL[π] F).comp P).comp ((e : E βL[π] F)β ) = Q := by 56 have hAadj : Aβ = (1 - P).comp ((e : E βL[π] F)β ) := by 57 have h := congrArg (fun T : E βL[π] F β¦ Tβ ) hA 58 simpa [adjoint_comp, map_sub, hPadj] using h.symm 59 have hPapply : β x, P (P x) = P x := by 60 intro x 61 exact congrArg (fun T : E βL[π] E β¦ T x) hPidem 62 have hcompApply : β x, (1 - P) ((1 - P) x) = (1 - P) x := by 63 intro x 64 simp [hPapply] 65 ext y 66 have hprodApply := congrArg (fun T : F βL[π] F β¦ T y) hprod 67 change A ((Aβ ) y) = y - Q y at hprodApply 68 rw [hAadj] at hprodApply 69 change A ((1 - P) (((e : E βL[π] F)β ) y)) = y - Q y at hprodApply 70 have hAApply : β x, A x = e ((1 - P) x) := by 71 intro x 72 exact (congrArg (fun T : E βL[π] F β¦ T x) hA).symm 73 rw [hAApply, hcompApply] at hprodApply 74 change e (P (((e : E βL[π] F)β ) y)) = Q y 75 have heApply : e (((e : E βL[π] F)β ) y) = y := by 76 rw [e.adjoint_eq_symm] 77 exact e.apply_symm_apply y 78 have hdecomp : e ((1 - P) (((e : E βL[π] F)β ) y)) = 79 e (((e : E βL[π] F)β ) y) - e (P (((e : E βL[π] F)β ) y)) := by 80 simp 81 rw [hdecomp, heApply] at hprodApply 82 exact sub_right_inj.mp hprodApply 83 84/-- The raw termwise unitary shell relation and the two shell support identities 85imply every finite unitary conjugacy relation. -/ 86theorem unitary_starProjection_conjugacy_of_projectionShells 87 (e : E ββα΅’[π] F) (W : β β E βL[π] F) 88 (U : β β Submodule π E) (V : β β Submodule π F) 89 [β n, (U n).HasOrthogonalProjection] 90 [β n, (V n).HasOrthogonalProjection] 91 (hU : Antitone U) (hV : Antitone V) 92 (hU0 : U 0 = β€) (hV0 : V 0 = β€) 93 (hInitial : β n, ((W n)β ).comp (W n) = Submodule.projectionShell U n) 94 (hFinal : β n, (W n).comp ((W n)β ) = Submodule.projectionShell V n) 95 (hUnitary : β n, (e : E βL[π] F).comp (Submodule.projectionShell U n) = W n) : 96 β N, ((e : E βL[π] F).comp (U N).starProjection).comp 97 ((e : E βL[π] F)β ) = (V N).starProjection := by 98 intro N 99 have hi := pairwiseInitialOrthogonal_of_projectionShells W U hU hInitial 100 have hfiniteComplement : (e : E βL[π] F).comp (1 - (U N).starProjection) = 101 partialSum W N := 102 comp_complement_eq_partialSum_of_shells (e : E βL[π] F) 103 (Submodule.projectionShell U) W U hUnitary 104 (Submodule.partialSum_projectionShell U hU0) N 105 have hfiniteProduct : (partialSum W N).comp 106 (partialSum (fun n β¦ (W n)β ) N) = 1 - (V N).starProjection := by 107 rw [partialSum_comp_adjoint_partialSum_eq W (Submodule.projectionShell V) hi hFinal, 108 Submodule.partialSum_projectionShell V hV0] 109 have hpartialAdjoint : (partialSum W N)β = partialSum (fun n β¦ (W n)β ) N := by 110 exact (partialSum_adjoint W N).symm 111 apply unitary_conjugacy_of_complement_product e (U N).starProjection 112 (V N).starProjection (partialSum W N) 113 Β· exact (U N).starProjection_isSymmetric.clm_adjoint_eq 114 Β· exact (U N).isIdempotentElem_starProjection 115 Β· exact hfiniteComplement 116 Β· rwa [hpartialAdjoint] 117 118/-- Exact completion of a strong shell limit by the limiting defect corner. 119The two finite hypotheses are precisely the finite complement and finite 120conjugacy relations; all asserted limiting and corner identities are proved. -/ 121theorem unitaryCompletion_of_finite_relations 122 (e : E ββα΅’[π] F) (A : β β E βL[π] F) (S : E βL[π] F) 123 (U : β β Submodule π E) (V : β β Submodule π F) 124 [β N, (U N).HasOrthogonalProjection] 125 [β N, (V N).HasOrthogonalProjection] 126 [(β¨ N, U N).HasOrthogonalProjection] 127 [(β¨ N, V N).HasOrthogonalProjection] 128 (hU : Antitone U) (hV : Antitone V) 129 (hA : StronglyConverges A atTop S) 130 (hfiniteComplement : β N, 131 (e : E βL[π] F).comp (1 - (U N).starProjection) = A N) 132 (hfiniteConjugacy : β N, 133 ((e : E βL[π] F).comp (U N).starProjection).comp 134 ((e : E βL[π] F)β ) = (V N).starProjection) : 135 let P := (β¨ N, U N).starProjection 136 let Q := (β¨ N, V N).starProjection 137 let R := (e : E βL[π] F).comp P 138 (e : E βL[π] F) = S + R β§ 139 R = (e : E βL[π] F).comp P β§ 140 (Rβ ).comp R = P β§ R.comp (Rβ ) = Q β§ 141 R = (Q.comp R).comp P β§ 142 (β x, x β β¨ N, U N β e x β β¨ N, V N) := by 143 dsimp only 144 let P : E βL[π] E := (β¨ N, U N).starProjection 145 let Q : F βL[π] F := (β¨ N, V N).starProjection 146 let R : E βL[π] F := (e : E βL[π] F).comp P 147 have hPlim := Submodule.stronglyConverges_starProjection_iInf U hU 148 have hQlim := Submodule.stronglyConverges_starProjection_iInf V hV 149 have hcompLimit : (e : E βL[π] F).comp (1 - P) = S := by 150 apply ext 151 intro x 152 apply tendsto_nhds_unique (l := (atTop : Filter β)) 153 Β· exact ((StronglyConverges.const (ΞΉ := β) (l := atTop) 154 (1 : E βL[π] E)).sub hPlim |>.comp_left (e : E βL[π] F)) x 155 Β· simpa [hfiniteComplement] using hA x 156 have hconjLimit : 157 ((e : E βL[π] F).comp P).comp ((e : E βL[π] F)β ) = Q := by 158 apply ext 159 intro y 160 apply tendsto_nhds_unique (l := (atTop : Filter β)) 161 Β· exact (hPlim.comp_left (e : E βL[π] F) |>.comp_right 162 ((e : E βL[π] F)β )) y 163 Β· apply Filter.Tendsto.congr' 164 (h := by simpa [Q] using hQlim y) 165 filter_upwards [] with N 166 exact (congrArg (fun T : F βL[π] F β¦ T y) 167 (hfiniteConjugacy N)).symm 168 have hPadj : Pβ = P := by 169 exact (β¨ N, U N).starProjection_isSymmetric.clm_adjoint_eq 170 have hQadj : Qβ = Q := by 171 exact (β¨ N, V N).starProjection_isSymmetric.clm_adjoint_eq 172 have hPidem : P.comp P = P := (β¨ N, U N).isIdempotentElem_starProjection 173 have hQidem : Q.comp Q = Q := (β¨ N, V N).isIdempotentElem_starProjection 174 have hleft : (e : E βL[π] F) = S + R := by 175 apply ext 176 intro x 177 have hx := congrArg (fun T : E βL[π] F β¦ T x) hcompLimit 178 change e ((1 - P) x) = S x at hx 179 calc 180 e x = e ((1 - P) x + P x) := by simp 181 _ = e ((1 - P) x) + e (P x) := map_add e _ _ 182 _ = S x + R x := by rw [hx]; rfl 183 _ = (S + R) x := rfl 184 have hPapply : β x, P (P x) = P x := by 185 intro x 186 exact congrArg (fun T : E βL[π] E β¦ T x) hPidem 187 have hRadj : Rβ = P.comp ((e : E βL[π] F)β ) := by 188 simp [R, adjoint_comp, hPadj] 189 have hinitial : (Rβ ).comp R = P := by 190 ext x 191 rw [hRadj] 192 change P (((e : E βL[π] F)β ) (e (P x))) = P x 193 rw [LinearIsometryEquiv.adjoint_eq_symm] 194 have he : (e.symm : F βL[π] E) (e (P x)) = P x := by 195 exact e.symm_apply_apply (P x) 196 rw [he] 197 exact hPapply x 198 have hfinal : R.comp (Rβ ) = Q := by 199 ext y 200 have hc := congrArg (fun T : F βL[π] F β¦ T y) hconjLimit 201 change e (P (((e : E βL[π] F)β ) y)) = Q y at hc 202 rw [hRadj] 203 change e (P (P (((e : E βL[π] F)β ) y))) = Q y 204 rw [hPapply] 205 exact hc 206 have hsupport : R = (Q.comp R).comp P := by 207 have hi : β x, (Rβ ) (R x) = P x := by 208 intro x 209 exact congrArg (fun T : E βL[π] E β¦ T x) hinitial 210 have hf : β y, R ((Rβ ) y) = Q y := by 211 intro y 212 exact congrArg (fun T : F βL[π] F β¦ T y) hfinal 213 ext x 214 calc 215 R x = R (P x) := by 216 dsimp [R] 217 rw [hPapply] 218 _ = R ((Rβ ) (R (P x))) := by rw [hi, hPapply] 219 _ = Q (R (P x)) := hf _ 220 _ = ((Q.comp R).comp P) x := rfl 221 have hmem : β x, x β β¨ N, U N β e x β β¨ N, V N := by 222 intro x 223 rw [β Submodule.starProjection_eq_self_iff, β Submodule.starProjection_eq_self_iff] 224 change P x = x β Q (e x) = e x 225 constructor 226 Β· intro hx 227 have hc := congrArg (fun T : F βL[π] F β¦ T (e x)) hconjLimit 228 simpa [P, Q, ContinuousLinearMap.comp_apply, hx] using hc.symm 229 Β· intro hx 230 have hc := congrArg (fun T : F βL[π] F β¦ T (e x)) hconjLimit 231 have : e (P x) = e x := by 232 simpa [P, Q, ContinuousLinearMap.comp_apply, hx] using hc 233 exact e.injective this 234 exact β¨hleft, rfl, hinitial, hfinal, hsupport, hmemβ© 235 236/-- Complete raw-shell entry theorem. Decreasing normalized projection families, 237the two termwise support products, and the termwise unitary relation suffice to 238construct the strong shell sum and its adjoint and to identify the complementary 239unitary corner. Finite products, finite conjugacy, and strong convergence are all 240conclusions or internal derived facts, not hypotheses. -/ 241theorem exists_strongSums_unitaryCompletion_of_projectionShells 242 (e : E ββα΅’[π] F) (W : β β E βL[π] F) 243 (U : β β Submodule π E) (V : β β Submodule π F) 244 [β n, (U n).HasOrthogonalProjection] 245 [β n, (V n).HasOrthogonalProjection] 246 [(β¨ n, U n).HasOrthogonalProjection] 247 [(β¨ n, V n).HasOrthogonalProjection] 248 (hU : Antitone U) (hV : Antitone V) 249 (hU0 : U 0 = β€) (hV0 : V 0 = β€) 250 (hInitial : β n, ((W n)β ).comp (W n) = Submodule.projectionShell U n) 251 (hFinal : β n, (W n).comp ((W n)β ) = Submodule.projectionShell V n) 252 (hUnitary : β n, (e : E βL[π] F).comp (Submodule.projectionShell U n) = W n) : 253 β S : E βL[π] F, β T : F βL[π] E, 254 StronglyConverges (partialSum W) atTop S β§ 255 StronglyConverges (partialSum fun n β¦ (W n)β ) atTop T β§ 256 βSβ β€ 1 β§ βTβ β€ 1 β§ T = Sβ β§ 257 (Sβ ).comp S = 1 - (β¨ n, U n).starProjection β§ 258 S.comp (Sβ ) = 1 - (β¨ n, V n).starProjection β§ 259 (let P := (β¨ n, U n).starProjection 260 let Q := (β¨ n, V n).starProjection 261 let R := (e : E βL[π] F).comp P 262 (e : E βL[π] F) = S + R β§ 263 R = (e : E βL[π] F).comp P β§ 264 (Rβ ).comp R = P β§ R.comp (Rβ ) = Q β§ 265 R = (Q.comp R).comp P β§ 266 (β x, x β β¨ n, U n β e x β β¨ n, V n)) := by 267 obtain β¨S, T, hS, hT, hSnorm, hTnorm, hAdj, hProdU, hProdVβ© := 268 exists_strongSums_of_projectionShells W U V hU hV hU0 hV0 hInitial hFinal 269 have hfiniteComplement : β N, 270 (e : E βL[π] F).comp (1 - (U N).starProjection) = partialSum W N := 271 comp_complement_eq_partialSum_of_shells (e : E βL[π] F) 272 (Submodule.projectionShell U) W U hUnitary 273 (Submodule.partialSum_projectionShell U hU0) 274 have hfiniteConjugacy : β N, 275 ((e : E βL[π] F).comp (U N).starProjection).comp 276 ((e : E βL[π] F)β ) = (V N).starProjection := 277 unitary_starProjection_conjugacy_of_projectionShells e W U V hU hV hU0 hV0 278 hInitial hFinal hUnitary 279 have hcompletion := unitaryCompletion_of_finite_relations e (partialSum W) S U V 280 hU hV hS hfiniteComplement hfiniteConjugacy 281 exact β¨S, T, hS, hT, hSnorm, hTnorm, hAdj, hProdU, hProdV, hcompletionβ© 282 283end ContinuousLinearMap