nLab H-star-algebra

Redirected from "H-star algebra".

Context

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

Noncommutative geometry

Contents

Definition

Definition

An H *H^*-algebra is a (not necessarily unital) Banach algebra AA that is simultaneously a Hilbert space (A,, A)(A, \langle \cdot, \cdot \rangle_A) with a compatible star-algebra structure, namely with an anti-linear involution :AA\dagger \colon A \to A such that

ab,c A=b,a c A=a,cb A,for alla,b,cA. \langle a b, c \rangle_A = \langle b, a^{\dagger} c \rangle_A = \langle a , c b^{\dagger} \rangle_A \,, \;\;\; \text{for all}\; a,b,c \in A.

(Ambrose 1945 Def. 1.2)

Definition

An H *H^\ast-algebra AA (Def. ) is called proper if

  • The only element aAa \in A such that a()a \cdot (-) is the zero map AAA \to A is a=0a = 0.

or equivalently

  • The only element aAa \in A such that ()a(-) \cdot a is the zero map AAA \to A is a=0a = 0.

(Ambrose 1945 Def. 2.1)

Properties

Classifying Frobenius Algebras

Frobenius structures in the category of finite-dimensional Hilbert spaces can be classified via H *H^*-algebras.

Theorem

A monoid (A,μ,η)(A, \mu, \eta) internal to FdHilb \mathrm{FdHilb} is a symmetric dagger Frobenius monoid if and only if it is a finite-dimensional proper H *H^*-algebra (Def. ), where the the involution is defined by sending an element aAa \in A to

(cf. Abramsky & Heunen 2012)

References

The original article:

Discussion in relation to Frobenius algebra-structures on finite-dimensional Hilbert spaces:

Last revised on May 3, 2026 at 16:18:18. See the history of this page for a list of all contributions to it.