nLab polar decomposition

Context

Linear algebra

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

Idea

The polar decomposition of bounded operators (on some Hilbert space) generalizes the decomposition of complex numbers zz as products z=re iϕz = r e^{i \phi} with r,r0r \in \mathbb{R}, r \ge 0 being the absolute value of zz and the complex number e iϕe^{i \phi} of norm 11 being the modulus, or the complex sign, of zz.

Definition

Let \mathcal{H} be a Hilbert space and S 1,S 2S_1, S_2 be closed linear subspaces.

Definition

A unitary isomorphism

U:S 1S 2 U \,\colon\, S_1 \longrightarrow S_2

is called a partial isometry with initial space S 1S_1 and final space or range S 2S_2

Let TT be a bounded operator on \mathcal{H}

Definition

The positive operator

|T|(T *T) 12 |T| \,\coloneqq\, \big(T^* T\big)^{\frac{1}{2}}

is called the modulus of T.

Properties

Existence

Proposition

For every bounded operator TT on \mathcal{H} there exists a unique partial isometry UU such that

  1. U has initial space R(|T|)¯\overline{R(|T|)} and range R(T)¯\overline{R(T)}

  2. T=U|T|=U(T *T) 12T = U |T| = U (T^*T)^{\frac{1}{2}}

Remark

Beware that this statement does not generalize from algebras of bounded operators ()\mathcal{B}(\mathcal{H}) to general C * C^\ast -algebras CC, because the partial isometry UU need not be contained in CC.

However, the analog statement is again true for von Neumann algebras.

References

Most textbooks on operator algebra and Hilbert spaces mention the polar decomposition, for example it can be found in the beginning of

See also:

Last revised on June 17, 2024 at 16:01:12. See the history of this page for a list of all contributions to it.