##
**Algebraic implications of composability of physical systems.**
*(English)*
Zbl 0358.17005

From the examples provided by classical and quantum mechanics, the authors abstract the concept of a two-product algebra, i.e., of an ordered triple \(\{\mathcal H, \tau, \alpha\}\) where \(\mathcal H\) is a vector space over a (commutative) field \(\mathcal F\), \(\tau\) is a multiplication on \(\mathcal H\) and \(\alpha\) is a Lie multiplication on \(\mathcal H\) which is derivative with respect to \(\tau\).

From the manner in which physical system compose in classical and quantum mechanics, they abstract then the concept of a composition class, i.e., of a set \(\mathcal J\) of two-product algebras equipped with a multiplication making it into a monoid with the neutral element \(\{\mathcal F, \tau, 0\}\), where \(\tau\) is the multiplication on \(\mathcal F\). They show that all composition classes are obtainable from a family \(\{\mathcal J_a\}\), labelled by an index \(a \in \mathcal J\) defined modulo the set of all squares in \(\mathcal F\), such that the multiplication \(\tau\) is symmetric on every element of \(\mathcal J_a\) for all \(a\). The composition class \(\mathcal J_0\) is said to be classical and, for \(a \neq 0\), \(\mathcal J_a\) is said to be quantal because the case of quantum mechanics is obtained with \(\mathcal F = \mathcal R\) and \(a = (n/2)^2\).

From the manner in which physical system compose in classical and quantum mechanics, they abstract then the concept of a composition class, i.e., of a set \(\mathcal J\) of two-product algebras equipped with a multiplication making it into a monoid with the neutral element \(\{\mathcal F, \tau, 0\}\), where \(\tau\) is the multiplication on \(\mathcal F\). They show that all composition classes are obtainable from a family \(\{\mathcal J_a\}\), labelled by an index \(a \in \mathcal J\) defined modulo the set of all squares in \(\mathcal F\), such that the multiplication \(\tau\) is symmetric on every element of \(\mathcal J_a\) for all \(a\). The composition class \(\mathcal J_0\) is said to be classical and, for \(a \neq 0\), \(\mathcal J_a\) is said to be quantal because the case of quantum mechanics is obtained with \(\mathcal F = \mathcal R\) and \(a = (n/2)^2\).

Reviewer: Uberto Cattaneo (Maggia)

### MSC:

17B40 | Automorphisms, derivations, other operators for Lie algebras and super algebras |

22E70 | Applications of Lie groups to the sciences; explicit representations |

81R05 | Finite-dimensional groups and algebras motivated by physics and their representations |

PDFBibTeX
XMLCite

\textit{E. Grgin} and \textit{A. Petersen}, Commun. Math. Phys. 50, 177--188 (1976; Zbl 0358.17005)

Full Text:
DOI

### References:

[1] | An investigation of two-product algebras, based on the duality between observables and generators in classical and quantum mechanics, is presented in E. Grgin and A. Petersen. J. Math. Phys.15, 764–769 (1974) · Zbl 0287.17003 |

[2] | Mehta, C. L.: J. Math. Phys.5, 677–686 (1964) · Zbl 0152.23502 |

[3] | See, e.g. Schafer, R. D.: An introduction to nonassociative algebras. Ch. V, section 3. New York: Academic Press 1966 |

This reference list is based on information provided by the publisher or from digital mathematics libraries. Its items are heuristically matched to zbMATH identifiers and may contain data conversion errors. In some cases that data have been complemented/enhanced by data from zbMATH Open. This attempts to reflect the references listed in the original paper as accurately as possible without claiming completeness or a perfect matching.