nLab Atkinson's theorem

Context

Operator algebra

algebraic quantum field theory (perturbative, on curved spacetimes, homotopical)

Introduction

Concepts

field theory:

Lagrangian field theory

quantization

quantum mechanical system, quantum probability

free field quantization

gauge theories

interacting field quantization

renormalization

Theorems

States and observables

Operator algebra

Local QFT

Perturbative QFT

Contents

Preliminaries

Definition

A continuous linear operator F:B 1B 2F \colon B_1\to B_2 between Banach spaces is Fredholm if it has finite dimensional kernel and finite dimensional cokernel.

Definition

A parametrix of a bounded linear operator F: 1 2F \colon \mathcal{H}_1 \to \mathcal{H}_2 is a reverse operator P: 2 1P \colon \mathcal{H}_2 \to \mathcal{H}_1 which is an “inverse up to compact operators”, i.e. such that FPid 2F \circ P - id_{\mathcal{H}_2} and PFid 1P \circ F - id_{\mathcal{H}_1} are both compact operators.

Statement

Theorem

(Atkinson 1951)
A bounded linear operator F:B 1B 2 F \colon B_1\to B_2 between Banach spaces is Fredholm, def. precisely it is has a parametrix, def. .

References

The original article:

  • F. V. Atkinson: The normal solubility of linear equations in normed spaces, Sb. Math. 70 (1951) [mathnet:sm5589]

Review:

Created on June 17, 2025 at 19:20:39. See the history of this page for a list of all contributions to it.