OAI/MathematicalPhysics/ContinuumCoulomb/ManyBody/MediatorSector.lean
21 declarations, 0 contain sorry, 0 declared as axioms
The singlet and excited mediator coordinates form the full spin space.
- theorem
OAI.ContinuumCoulomb.mediatorLowInclusion_applyline 13 - theorem
OAI.ContinuumCoulomb.mediatorHighInclusion_applyline 26 - theorem
OAI.ContinuumCoulomb.mediatorHighInclusion_vacuumline 32 - theorem
OAI.ContinuumCoulomb.mediatorLowRestriction_applyline 38 - theorem
OAI.ContinuumCoulomb.mediatorHighRestriction_applyline 42 - theorem
OAI.ContinuumCoulomb.mediatorLowRestriction_inclusionline 47 - theorem
OAI.ContinuumCoulomb.mediatorHighRestriction_inclusionline 51 - theorem
OAI.ContinuumCoulomb.mediatorLowRestriction_highline 55 - theorem
OAI.ContinuumCoulomb.mediatorHighRestriction_lowline 60 - theorem
OAI.ContinuumCoulomb.mediator_full_decompositionline 67Source documentation
Every full spin state decomposes into its singlet and triplet sectors.
theorem mediator_full_decomposition (n r : ℕ) (x : MediatorFullSpace n r) : mediatorLowInclusion n r (mediatorLowRestriction n r x) + mediatorHighInclusion n r (mediatorHighRestriction n r x) = x := by …Mentions: OAI.ContinuumCoulomb.MediatorFullSpace, OAI.ContinuumCoulomb.mediatorLowInclusion, OAI.ContinuumCoulomb.mediatorLowRestriction, OAI.ContinuumCoulomb.mediatorHighInclusion, OAI.ContinuumCoulomb.mediatorHighRestriction
- theorem
OAI.ContinuumCoulomb.mediatorLow_real_innerline 80 - theorem
OAI.ContinuumCoulomb.mediatorHigh_real_innerline 84 - theorem
OAI.ContinuumCoulomb.mediatorLowInclusion_norm_mapline 88 - theorem
OAI.ContinuumCoulomb.mediatorHighInclusion_norm_mapline 92 - def
OAI.ContinuumCoulomb.assembleMediatorline 96 - theorem
OAI.ContinuumCoulomb.assembleMediator_norm_sqline 99 - theorem
OAI.ContinuumCoulomb.mediatorLow_operator_compressionline 107Source documentation
The matrix vacuum compression agrees with the actual Hilbert-space block.
theorem mediatorLow_operator_compression (n r : ℕ) (M : Matrix (MediatedSpinBasis n r) (MediatedSpinBasis n r) ℂ) : (mediatorLowRestriction n r).comp ((spinMatrixOperator M).comp (mediatorLowInclusion n r)) = spinMatrixOperator (mediatorCompression n r M) := by …Mentions: OAI.ContinuumCoulomb.MediatedSpinBasis, OAI.ContinuumCoulomb.mediatorLowRestriction, OAI.ContinuumCoulomb.spinMatrixOperator, OAI.ContinuumCoulomb.mediatorLowInclusion, OAI.ContinuumCoulomb.mediatorCompression
- theorem
OAI.ContinuumCoulomb.spinMatrixOperator_diagonalline 120 - theorem
OAI.ContinuumCoulomb.liftedMediatorInverse_diagonalline 125 - theorem
OAI.ContinuumCoulomb.mediatorInverse_highInclusionline 134Source documentation
The full inverse matrix is the actual diagonal high-sector inverse, extended by zero on the singlet sector.
theorem mediatorInverse_highInclusion (n r : ℕ) (Delta : ℝ) (q : MediatorHighSpace n r) : spinMatrixOperator (liftedMediatorInverse n r Delta) (mediatorHighInclusion n r q) = mediatorHighInclusion n r (diagonalPenalty (fun s => (actualMediatorWeight n r Delta s)⁻¹) q) := by …Mentions: OAI.ContinuumCoulomb.MediatorHighSpace, OAI.ContinuumCoulomb.spinMatrixOperator, OAI.ContinuumCoulomb.liftedMediatorInverse, OAI.ContinuumCoulomb.mediatorHighInclusion, OAI.ContinuumCoulomb.diagonalPenalty, OAI.ContinuumCoulomb.actualMediatorWeight
- theorem
OAI.ContinuumCoulomb.liftedSource_lowInclusionline 152Source documentation
The original Hamiltonian acts only on the original-spin coordinates.
theorem liftedSource_lowInclusion (n r : ℕ) (C : Matrix (SourceSpinBasis n) (SourceSpinBasis n) ℂ) (p : MediatorLowSpace n) : spinMatrixOperator (C ⊗ₖ (1 : Matrix (MediatorBasis r) (MediatorBasis r) ℂ)) (mediatorLowInclusion n r p) = mediatorLowInclusion n r (spinMatrixOperator C p) := by …Mentions: OAI.ContinuumCoulomb.SourceSpinBasis, OAI.ContinuumCoulomb.MediatorLowSpace, OAI.ContinuumCoulomb.spinMatrixOperator, OAI.ContinuumCoulomb.MediatorBasis, OAI.ContinuumCoulomb.mediatorLowInclusion