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Joint continuous functional calculus on arbitrary complex Hilbert spaces

Definition
rybin2026_p02_joint_calculus_hilbert

by wenxinzhang · Sep 5, 2026 · Mathlib c5ea003 (Lean v4.30.0)

convexityfunctional-analysishilbert-spacesoperator-theory

Let S=[0,1]2S=[0,1]^2S=[0,1]2 and let HHH be an arbitrary complete complex Hilbert space. The two coordinate functions on SSS are continuous real functions. A joint calculus is a unital real star-algebra homomorphism from C(S,R)C(S,\mathbb R)C(S,R) to the bounded complex-linear operators on HHH. It represents (X,Y)(X,Y)(X,Y) when it is continuous in the uniform and operator-norm topologies and sends the coordinates to X,YX,YX,Y.

A positive contraction XXX is specified by X∗=XX^*=XX∗=X, Re⁡⟨v,Xv⟩≥0\operatorname{Re}\langle v,Xv\rangle\ge0Re⟨v,Xv⟩≥0 for every vvv, and ∥X∥≤1\|X\|\le1∥X∥≤1. Restriction of fff to SSS requires continuity only on SSS.

Formalization Note. The joint evaluation chooses one representing homomorphism if one exists, and is zero for every input function if none exists. Existence and uniqueness for commuting positive contractions are the separate standard joint-calculus theorem. The definition does not assume the compression-rigidity conclusion. No finite-dimensional, separability or nonzero-space restriction is imposed.

Definition code
import Mathlib

namespace RybinAI2026.P02Hilbert

/-- The compact joint spectral box for two positive contractions. -/
def unitSquare : Set (Fin 2 → ℝ) := Set.Icc 0 1
abbrev Square := ↥unitSquare

/-- The two real coordinate functions on the joint spectral box. -/
def coordinate (i : Fin 2) : C(Square, ℝ) :=
  ⟨fun x => x.1 i, (continuous_apply i).comp continuous_subtype_val⟩

/-- Restriction of a continuous-on-the-square function, without requiring continuity outside. -/
def restrictFunction (f : (Fin 2 → ℝ) → ℝ) (hf : ContinuousOn f unitSquare) :
    C(Square, ℝ) := ⟨fun x => f x.1, hf.restrict⟩

/-- A joint continuous functional calculus, represented by its continuous unital star homomorphism.
The coordinate images are the two commuting positive contractions; no eigenbasis is assumed. -/
abbrev JointCalculus (H : Type*) [NormedAddCommGroup H] [InnerProductSpace ℂ H]
    [CompleteSpace H] := C(Square, ℝ) →⋆ₐ[ℝ] (H →L[ℂ] H)

variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]

/-- Explicit positivity and contraction conditions for a bounded operator. -/
def PositiveContraction (X : H →L[ℂ] H) : Prop :=
  star X = X ∧ (∀ v : H, 0 ≤ (inner ℂ v (X v)).re) ∧ ‖X‖ ≤ 1

/-- The actual continuous joint functional-calculus representation of a given pair. -/
def Represents (calculus : JointCalculus H) (X Y : H →L[ℂ] H) : Prop :=
  Continuous calculus ∧ calculus (coordinate 0) = X ∧ calculus (coordinate 1) = Y

/-- Joint functional calculus chosen from its defining representation property. Existence and
uniqueness for commuting positive contractions are a separate standard spectral-theorem target.
The zero fallback is used only for pairs for which no such representation exists. -/
noncomputable def jointCFC (X Y : H →L[ℂ] H) (g : C(Square, ℝ)) : H →L[ℂ] H := by
  classical
  exact if h : ∃ calculus : JointCalculus H, Represents calculus X Y then
    (Classical.choose h) g
  else 0

end RybinAI2026.P02Hilbert
Source
https://rybindmitry.github.io/problems/2.html, displayed compression equality and question; joint-calculus representation: Jan Dereziński, Bounded operators, Lemma 6.6, printed p. 43, https://www.fuw.edu.pl/~derezins/mat-o.pdf#page=43.

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