nLab 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

An H *H^*-algebra is a \mathbb{C} -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 \langle a b, c \rangle_A = \langle b, a^{\dagger} c \rangle_A = \langle a , c b^{\dagger} \rangle_A

for all a,b,cAa,b,c \in A.

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 H *H^*-algebra, where the the involution is defined by sending an element aAa \in A to

References

An exposition of the classification of Frobenius structures in finite-dimensional Hilbert spaces as H *H^*-algebras:

Last revised on December 3, 2025 at 19:00:00. See the history of this page for a list of all contributions to it.