Pairs in the block space H ⊕ H #
The pair (v, v') in H².
Equations
- CommutingRepetition.GraphMod.pair M v v' = (CommutingRepetition.Block.embed M (Fin 2) 0) v + (CommutingRepetition.Block.embed M (Fin 2) 1) v'
Instances For
A block operator on a pair, through its four entries.
The graph of left multiplication by x #
The generator (ι a, x·a) of the graph.
Equations
- CommutingRepetition.GraphMod.gen M x a = CommutingRepetition.GraphMod.pair M (M.ι a) ((M.Rop a) x)
Instances For
The closed graph Γₓ.
Equations
Instances For
The orthogonal projection onto the graph.
Equations
Instances For
Closability #
The vectors (−(Jx)·b, ι b) are orthogonal to the graph.
Equations
- CommutingRepetition.GraphMod.orthGen M x b = CommutingRepetition.GraphMod.pair M (-(M.Rop b) (M.J x)) (M.ι b)
Instances For
Closability: the graph closure is a graph.
An operator leaving a closed subspace and its orthogonal complement invariant commutes with the orthogonal projection.
E = P₁₁ = TT*(1+TT*)⁻¹.
Equations
Instances For
C = P₀₁ = T*(1+TT*)⁻¹.
Equations
Instances For
The graph relations #
Injectivity of 1 − E.
The spectrum of E lies in [0, 1].
The Borel calculus of E #
t ↦ max 0 (min 1 t): a bounded continuous function equal to the identity on [0, 1].
Equations
- CommutingRepetition.GraphMod.clamp t = max 0 (min 1 t)
Instances For
E = clamp(E).
The spectral projection at {1} vanishes (1 − E is injective).
The key formula: C g(E) Ω = J ((1 − t) g)(E) x for bounded Borel g.
x has no mass at {0} (it lies in the closure of the range of T).