OAI/MathematicalPhysics/ContinuumCoulomb/ManyBody/MediatorBlocks.lean
26 declarations, 0 contain sorry, 0 declared as axioms
Concrete low and high blocks for simultaneous singlet mediators. The nonzero original-spin block is retained throughout.
- abbrev
OAI.ContinuumCoulomb.MediatorLowSpaceline 14 - abbrev
OAI.ContinuumCoulomb.MediatorHighSpaceline 15 - abbrev
OAI.ContinuumCoulomb.MediatorFullSpaceline 16 - def
OAI.ContinuumCoulomb.mediatorLowIndexline 18 - def
OAI.ContinuumCoulomb.mediatorHighIndexline 21 - theorem
OAI.ContinuumCoulomb.mediatorLowIndex_injectiveline 24 - theorem
OAI.ContinuumCoulomb.mediatorHighIndex_injectiveline 28 - def
OAI.ContinuumCoulomb.mediatorLowInclusionline 35 - def
OAI.ContinuumCoulomb.mediatorLowRestrictionline 38 - def
OAI.ContinuumCoulomb.mediatorHighInclusionline 41 - def
OAI.ContinuumCoulomb.mediatorHighRestrictionline 44 - theorem
OAI.ContinuumCoulomb.mediatorLowInclusion_normline 47 - theorem
OAI.ContinuumCoulomb.mediatorHighInclusion_normline 50 - theorem
OAI.ContinuumCoulomb.mediatorLowRestriction_normline 53 - theorem
OAI.ContinuumCoulomb.mediatorHighRestriction_normline 56 - def
OAI.ContinuumCoulomb.actualMediatorWeightline 59 - theorem
OAI.ContinuumCoulomb.actualMediator_inverse_dataline 62 - def
OAI.ContinuumCoulomb.actualMediatorLowBlockline 77 - def
OAI.ContinuumCoulomb.actualMediatorCouplingline 83 - def
OAI.ContinuumCoulomb.actualMediatorHighBlockline 90 - theorem
OAI.ContinuumCoulomb.actualMediatorLowBlock_normline 98 - theorem
OAI.ContinuumCoulomb.actualMediatorCoupling_normline 106 - theorem
OAI.ContinuumCoulomb.spinMatrixOperator_add_norm_boundline 115 - theorem
OAI.ContinuumCoulomb.liftedMediatorPerturbation_normline 124 - theorem
OAI.ContinuumCoulomb.actualMediatorHighBlock_normline 133 - theorem
OAI.ContinuumCoulomb.actualMediator_second_orderline 146Source documentation
A supporting block estimate for the actual simultaneous mediator construction, retaining the unreplaced low Hamiltonian C.
theorem actualMediator_second_order (n r : ℕ) {Delta : ℝ} (hDelta : 0 < Delta) (C : Matrix (SourceSpinBasis n) (SourceSpinBasis n) ℂ) (left right : Fin r → Fin n) (member : Fin r → Fin 2) (amplitude : Fin r → ℝ) {epsilon : ℝ} (hepsilon : 0 ≤ epsilon) (hsmall : epsilon ≤ 1 / 4) (hbound : ‖spinMatrixOperator (C ⊗ₖ (1 : Matrix (MediatorBasis r) (MediatorBasis r) ℂ))‖ + 6 * ∑ e, |amplitude e| ≤ epsilon * (4 * Delta)) : |Perturbation.lowBlockBottom (actualMediatorLowBlock n r C) (diagonalPenalty (actualMediatorWeight n r Delta)) (actualMediatorHighBlock n r C left right member amplitude) (actualMediatorCoupling n r left right member amplitude) - Perturbation.effectiveBottom (actualMediatorLowBlock n r C) (diagonalPenalty (fun s => (actualMediatorWeight n r Delta s)⁻¹)) …Mentions: OAI.ContinuumCoulomb.SourceSpinBasis, OAI.ContinuumCoulomb.spinMatrixOperator, OAI.ContinuumCoulomb.MediatorBasis, OAI.ContinuumCoulomb.Perturbation.lowBlockBottom, OAI.ContinuumCoulomb.actualMediatorLowBlock, OAI.ContinuumCoulomb.diagonalPenalty, OAI.ContinuumCoulomb.actualMediatorWeight, OAI.ContinuumCoulomb.actualMediatorHighBlock, OAI.ContinuumCoulomb.actualMediatorCoupling, OAI.ContinuumCoulomb.Perturbation.effectiveBottom