Theorem 1 — EQ-MEAS, EQ-LIND, EQ-HS, EQ-KL are equivalent (finite dimension)
ProvedProjectiveMeasurementEquilibration.projective_measurement_equilibrationThroughout, is a finite index type, the Hilbert space is , is a Hermitian complex matrix with spectral decomposition ( ranging over the distinct eigenvalues, the orthogonal projection onto the -eigenspace, and for not an eigenvalue), and a density matrix is a positive semidefinite matrix of trace . Let be any map on matrices (the black-box spectral equilibration process ; only its values on density matrices matter). Then the conditions
- EQ-MEAS: ;
- EQ-LIND: , where , ;
- EQ-HS: ;
- EQ-KL: ,
each required for all density matrices , are pairwise equivalent. This is Theorem 1 of the source specialised to finite-dimensional Hilbert spaces, where Condition [B]FINENT holds automatically.
import Mathlib import Definitions.Def_pme_quantum_basics import Definitions.Def_pme_measurement_conditions open Matrix Filter Topology
namespace ProjectiveMeasurementEquilibration
theorem projective_measurement_equilibration {n : Type} [Fintype n] [DecidableEq n] {X : Matrix n n ℂ}
(hX : X.IsHermitian) (Φ : Matrix n n ℂ → Matrix n n ℂ) :
(EqMeas hX Φ ↔ EqLind X Φ) ∧ (EqMeas hX Φ ↔ EqHS X Φ) ∧ (EqMeas hX Φ ↔ EqKL X Φ) := by sorry
end ProjectiveMeasurementEquilibrationRead-back
What the Lean code literally says, in plain math · Aristotle (Harmonic) - same agent as the drafter; non-blind
Non-blind read-back. This read-back was written by the same agent (Aristotle, by Harmonic) that drafted the Lean statements, at the explicit request of the account owner. It is not blind and not independent testimony: the author knew the intended meaning while writing it. Reviewers should not treat it as an independent audit.
For every finite index type , every Hermitian matrix and every function , the three equivalences hold: , , and , where (all quantifiers over density matrices = positive semidefinite trace-one matrices):
- : for all ( distinct eigenvalues of , eigenprojections);
- : for all , a function with and within for exists, and every such function tends entrywise to as ;
- : for all , is a density matrix commuting with and for every density matrix commuting with ;
- : as but with , the extended-real relative entropy ( unless , otherwise with ).
The statement is only about finite-dimensional matrices; separable infinite-dimensional Hilbert spaces and unbounded observables are not covered. When is empty, all four conditions hold vacuously.
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.