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MIPRE.Background.LIDT.Co.SelfImprovement.Theorems.Results.HelperCompleteness.FiberBounds

Helper completeness: fiber operators and Cauchy--Schwarz bounds #

The fiber operator T_[h(u)=a] of the helper-completeness proof, the pointwise operator inequalities and the averaged Cauchy--Schwarz estimates of its two analytic moves: the counterpart of the vendored SelfImprovement/Theorems/Results/HelperCompleteness/FiberBounds.lean (under MIPRE/Background/LIDT/MIPStarRE/LDT/) in the port of planning/c6b-plan.md (milestone M10, section "Port conventions").

A strategy is a SymStrat params 𝔓 K. The fiber operator and its bounds live in the local algebra 𝔓, where their positivity is proved; the joint operators are strategy.state.L, strategy.state.opTensor in K →L[ℂ] K.

The vendored file imports Basic/ParametersFiniteAnswers.lean (for polynomial_sum_fiberwise) and SelfImprovement/Theorems/Thresholds/Final.lean, both classical and without a Co file; so does this one.

Not ported #

Every declaration of the vendored file has a counterpart here.

References #

In LionSR/MIPStarRE at commit 507e8122, not in this repository:

The fiber operator T_[h(u)=a] in the helper-completeness proof.

It is the sum of all SDP-measurement outcomes indexed by polynomials whose value at the point u is a.

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    The helper fiber operator is positive.

    The helper fiber operator is bounded by the identity.

    The fiber operators over all values at a fixed point sum to the total SDP submeasurement operator.

    theorem MIPRE.LIDT.Co.SelfImprovement.helper_second_move_first_factor_operator_le_one {𝔓 : Type u_1} [CStarAlgebra 𝔓] [PartialOrder 𝔓] [StarOrderedRing 𝔓] {K : Type u_2} [NormedAddCommGroup K] [InnerProductSpace ℂ K] [CompleteSpace K] (S : SymModel 𝔓 K) (params : MIPStarRE.LDT.Parameters) [MIPStarRE.LDT.FieldModel params.q] (T : SubMeas (MIPStarRE.LDT.Polynomial params) 𝔓) (u : MIPStarRE.LDT.Point params) :
    (∑ a : MIPStarRE.LDT.Fq params, have Tfiber := helperFiberOperator params T u a; S.L (Tfiber * Tfiber)) ≤ 1

    Pointwise operator form of the identity bound for the first Cauchy--Schwarz factor in the second helper-completeness move.

    At a fixed point u, the fiber operators form a submeasurement after grouping by the value h(u). Thus Σ_a T_[h(u)=a]^2 ≤ Σ_a T_[h(u)=a] = T.total ≤ I.

    theorem MIPRE.LIDT.Co.SelfImprovement.helper_second_move_first_factor_le_one {𝔓 : Type u_1} [CStarAlgebra 𝔓] [PartialOrder 𝔓] [StarOrderedRing 𝔓] {K : Type u_2} [NormedAddCommGroup K] [InnerProductSpace ℂ K] [CompleteSpace K] (params : MIPStarRE.LDT.Parameters) [MIPStarRE.LDT.FieldModel params.q] (strategy : SymStrat params 𝔓 K) (T : SubMeas (MIPStarRE.LDT.Polynomial params) 𝔓) :
    (MIPStarRE.LDT.avgOver (MIPStarRE.LDT.uniformDistribution (MIPStarRE.LDT.Point params)) fun (u : MIPStarRE.LDT.Point params) => ∑ a : MIPStarRE.LDT.Fq params, have Tfiber := helperFiberOperator params T u a; strategy.state.ev (strategy.state.L (Tfiber * Tfiber))) ≤ 1

    The first Cauchy--Schwarz factor in the second helper-completeness move is bounded by one.

    This is the Lean form of the paper's assertion, following eq:mysterious-case-of-the-disappearing-a, that E_u Σ_a ⟨ψ, T_[h(u)=a]^2 ⊗ I ψ⟩ ≤ 1.

    theorem MIPRE.LIDT.Co.SelfImprovement.helper_second_move_second_factor_pointwise_le_qBipartiteSSCDefect {𝔓 : Type u_1} [CStarAlgebra 𝔓] [PartialOrder 𝔓] [StarOrderedRing 𝔓] {K : Type u_2} [NormedAddCommGroup K] [InnerProductSpace ℂ K] [CompleteSpace K] (params : MIPStarRE.LDT.Parameters) [MIPStarRE.LDT.FieldModel params.q] (strategy : SymStrat params 𝔓 K) (u : MIPStarRE.LDT.Point params) :
    (∑ a : MIPStarRE.LDT.Fq params, have Au := (strategy.pointMeasurement u).outcome a; strategy.state.ev (strategy.state.opTensor (Au * Au) ((1 - Au) * (1 - Au)))) ≤ strategy.state.qBipartiteSSCDefect (strategy.pointMeasurement u).toSubMeas

    Pointwise comparison between the projective residual in the second Cauchy--Schwarz move and the bipartite strong self-consistency defect.

    Projectivity gives (A^u_a)^2 = A^u_a and (I - A^u_a)^2 = I - A^u_a. After summing over a, the residual is the one-register total mass minus the diagonal cross-register overlap, and hence is bounded by the max 0 defining qBipartiteSSCDefect.

    theorem MIPRE.LIDT.Co.SelfImprovement.helper_second_move_second_factor_le_delta {𝔓 : Type u_1} [CStarAlgebra 𝔓] [PartialOrder 𝔓] [StarOrderedRing 𝔓] {K : Type u_2} [NormedAddCommGroup K] [InnerProductSpace ℂ K] [CompleteSpace K] (params : MIPStarRE.LDT.Parameters) [MIPStarRE.LDT.FieldModel params.q] (strategy : SymStrat params 𝔓 K) (delta : ℝ) (hssc : strategy.state.BipartiteSSCRel (MIPStarRE.LDT.uniformDistribution (MIPStarRE.LDT.Point params)) strategy.pointMeasurement.toIdxSubMeas delta) :
    (MIPStarRE.LDT.avgOver (MIPStarRE.LDT.uniformDistribution (MIPStarRE.LDT.Point params)) fun (u : MIPStarRE.LDT.Point params) => ∑ a : MIPStarRE.LDT.Fq params, have Au := (strategy.pointMeasurement u).outcome a; strategy.state.ev (strategy.state.opTensor (Au * Au) ((1 - Au) * (1 - Au)))) ≤ delta

    The second Cauchy--Schwarz factor in the second helper-completeness move is bounded by the bipartite strong self-consistency error.

    This is the Lean form of the paper's assertion that E_u Σ_a ⟨ψ, A^u_a ⊗ (I-A^u_a) ψ⟩ ≤ delta.

    theorem MIPRE.LIDT.Co.SelfImprovement.helper_first_move_second_factor_operator_le_one {𝔓 : Type u_1} [CStarAlgebra 𝔓] [PartialOrder 𝔓] [StarOrderedRing 𝔓] {K : Type u_2} [NormedAddCommGroup K] [InnerProductSpace ℂ K] [CompleteSpace K] (params : MIPStarRE.LDT.Parameters) [MIPStarRE.LDT.FieldModel params.q] (strategy : SymStrat params 𝔓 K) (T : SubMeas (MIPStarRE.LDT.Polynomial params) 𝔓) (u : MIPStarRE.LDT.Point params) :
    (∑ a : MIPStarRE.LDT.Fq params, have Au := (strategy.pointMeasurement u).outcome a; have Tfiber := helperFiberOperator params T u a; strategy.state.L (Au * (Tfiber * Tfiber) * Au)) ≤ 1

    Pointwise operator form of the identity bound for the second Cauchy--Schwarz factor in the first helper-completeness move.

    For a fixed point u, each fiber operator satisfies 0 ≤ T_[h(u)=a] ≤ I, hence T_[h(u)=a]^2 ≤ I. Sandwiching by the projection A^u_a gives A^u_a T_[h(u)=a]^2 A^u_a ≤ A^u_a, and the projective measurement A^u sums to the identity.

    theorem MIPRE.LIDT.Co.SelfImprovement.helper_first_move_second_factor_le_one {𝔓 : Type u_1} [CStarAlgebra 𝔓] [PartialOrder 𝔓] [StarOrderedRing 𝔓] {K : Type u_2} [NormedAddCommGroup K] [InnerProductSpace ℂ K] [CompleteSpace K] (params : MIPStarRE.LDT.Parameters) [MIPStarRE.LDT.FieldModel params.q] (strategy : SymStrat params 𝔓 K) (T : SubMeas (MIPStarRE.LDT.Polynomial params) 𝔓) :
    (MIPStarRE.LDT.avgOver (MIPStarRE.LDT.uniformDistribution (MIPStarRE.LDT.Point params)) fun (u : MIPStarRE.LDT.Point params) => ∑ a : MIPStarRE.LDT.Fq params, have Au := (strategy.pointMeasurement u).outcome a; have Tfiber := helperFiberOperator params T u a; strategy.state.ev (strategy.state.L (Au * (Tfiber * Tfiber) * Au))) ≤ 1

    The second Cauchy--Schwarz factor in the first helper-completeness move is bounded by the identity contribution.

    This is the Lean form of the paper's assertion, following eq:yet-another-move-a, that E_u Σ_a ⟨ψ, (A^u_a T_[h(u)=a]^2 A^u_a) ⊗ I ψ⟩ ≤ 1.

    The scalar expression after the first Cauchy--Schwarz move in helper completeness.

    This is E_u Σ_a ⟨ψ, (T_[h(u)=a] A^u_a) ⊗ A^u_a ψ⟩, the right-hand side of eq:yet-another-move-a in the paper. The fiber T_[h(u)=a] is represented by the finite sum over polynomials whose value at u is a.

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      The scalar expression after removing the remaining point-measurement operator in helper completeness.

      This is E_u Σ_h ⟨ψ, (T_h A^u_{h(u)}) ⊗ I ψ⟩. Complementary slackness identifies this quantity with the dual mass ⟨ψ, Z ⊗ I ψ⟩.

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        theorem MIPRE.LIDT.Co.SelfImprovement.helper_linearized_completeness_quantity_eq_fiber_sum {𝔓 : Type u_1} [CStarAlgebra 𝔓] [PartialOrder 𝔓] [StarOrderedRing 𝔓] {K : Type u_2} [NormedAddCommGroup K] [InnerProductSpace ℂ K] [CompleteSpace K] (params : MIPStarRE.LDT.Parameters) [MIPStarRE.LDT.FieldModel params.q] (strategy : SymStrat params 𝔓 K) (T : SubMeas (MIPStarRE.LDT.Polynomial params) 𝔓) :
        helperLinearizedCompletenessQuantity params strategy T = MIPStarRE.LDT.avgOver (MIPStarRE.LDT.uniformDistribution (MIPStarRE.LDT.Point params)) fun (u : MIPStarRE.LDT.Point params) => ∑ a : MIPStarRE.LDT.Fq params, have Au := (strategy.pointMeasurement u).outcome a; have Tfiber := helperFiberOperator params T u a; strategy.state.ev (strategy.state.L (Tfiber * Au))

        Fiberwise form of the linearized helper-completeness quantity.

        The expression E_u Σ_h ⟨ψ, (T_h A^u_{h(u)}) ⊗ I ψ⟩ may equivalently be grouped by the value a = h(u), giving E_u Σ_a ⟨ψ, (T_[h(u)=a] A^u_a) ⊗ I ψ⟩. This is the algebraic rewrite used after eq:mysterious-case-of-the-disappearing-a in the paper.

        theorem MIPRE.LIDT.Co.SelfImprovement.helper_second_move_pointwise_abs_le_sqrt {𝔓 : Type u_1} [CStarAlgebra 𝔓] [PartialOrder 𝔓] [StarOrderedRing 𝔓] {K : Type u_2} [NormedAddCommGroup K] [InnerProductSpace ℂ K] [CompleteSpace K] (params : MIPStarRE.LDT.Parameters) [MIPStarRE.LDT.FieldModel params.q] (strategy : SymStrat params 𝔓 K) (T : SubMeas (MIPStarRE.LDT.Polynomial params) 𝔓) (u : MIPStarRE.LDT.Point params) (a : MIPStarRE.LDT.Fq params) :
        |strategy.state.ev (strategy.state.opTensor (helperFiberOperator params T u a * (strategy.pointMeasurement u).outcome a) (1 - (strategy.pointMeasurement u).outcome a))| ≤ √(strategy.state.ev (strategy.state.L (helperFiberOperator params T u a * helperFiberOperator params T u a))) * √(strategy.state.ev (strategy.state.opTensor ((strategy.pointMeasurement u).outcome a * (strategy.pointMeasurement u).outcome a) ((1 - (strategy.pointMeasurement u).outcome a) * (1 - (strategy.pointMeasurement u).outcome a))))

        Pointwise Cauchy--Schwarz estimate for the second helper-completeness move.

        For fixed u and a, this bounds the residual term ⟨ψ, (T_[h(u)=a] A^u_a) ⊗ (I - A^u_a) ψ⟩ by the product of the two square-root factors appearing after eq:mysterious-case-of-the-disappearing-a.

        The second Cauchy--Schwarz move in the helper-completeness proof.

        Assuming bipartite strong self-consistency of the point measurement with error delta, the first-moved helper-completeness expression E_u Σ_a ⟨ψ, (T_[h(u)=a] A^u_a) ⊗ A^u_a ψ⟩ differs from the linearized expression E_u Σ_a ⟨ψ, (T_[h(u)=a] A^u_a) ⊗ I ψ⟩ by at most sqrt delta. The first factor is bounded by the grouped submeasurement estimate, and the second is exactly the projective residual controlled by self-consistency.