Quantitative bounds for the bounded resolvent realization #
This is the abstract Banach-algebra part of blueprint node I-l2op. It
turns the norm-small event for K = G M into explicit Neumann inverse,
tail, and recentered-resolvent bounds. No random-kernel estimate enters
here; those estimates only have to prove that the event occurs with high
probability.
theorem
Anderson4D.norm_neumannInverse_le
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[CompleteSpace H]
[Nontrivial H]
(K : H →L[ℂ] H)
(hK : ‖K‖ < 1)
:
The geometric-series bound for the canonical Neumann inverse.
theorem
Anderson4D.norm_neumannInverse_le_two
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[CompleteSpace H]
[Nontrivial H]
(K : H →L[ℂ] H)
(hKhalf : ‖K‖ ≤ 1 / 2)
:
On the paper's convenient half-ball, the inverse has norm at most two.
theorem
Anderson4D.neumannInverse_sub_partialSum
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[CompleteSpace H]
(K : H →L[ℂ] H)
(hK : ‖K‖ < 1)
(n : ℕ)
:
Exact algebraic remainder after truncating the Neumann series at order
n - 1.
theorem
Anderson4D.norm_neumannInverse_sub_partialSum_le
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[CompleteSpace H]
[Nontrivial H]
(K : H →L[ℂ] H)
(hK : ‖K‖ < 1)
(n : ℕ)
:
Quantitative geometric tail bound.
theorem
Anderson4D.norm_inverseGreen_sub_G_le
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[CompleteSpace H]
[Nontrivial H]
(G M : H →L[ℂ] H)
(hK : ‖Kop G M‖ < 1)
:
Abstract recentered-resolvent bound on the norm-small event.
theorem
Anderson4D.norm_inverseGreen_sub_G_le_two
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[CompleteSpace H]
[Nontrivial H]
(G M : H →L[ℂ] H)
(hKhalf : ‖Kop G M‖ ≤ 1 / 2)
:
Half-ball specialization used by good-event estimates.