Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:hep-th/9702066 · Physics Letters B

Algebra of observables for identical particles in one dimension

Serguei B. Isakov, Jon Magne Leinaas, Jan Myrheim, Alexios P. Polychronakos, Raimund Varnhagen

Published Jun 1, 1998• 6 citations
arXivHTMLPDF
DOI
10.1016/s0370-2693(98)00502-4

Related papers

Exchange of identical particles in two dimensions

P. Ramadevi

Resonance•Feb 1, 2001•2 citations

Algebra of physical observables

Susumo Okubo

Cambridge University Press eBooks•Aug 3, 1995•0 citations

Generalized statistics and the algebra of observables

Jon Magne Leinaas

A short review is given of how to apply the algebraic Heisenberg quantization scheme to a system of identical particles. For two particles in one dimension the approach leads to a generalization of the Bose and Fermi description which can be expressed in the form of a 1/x^2 statistics interaction between the particles. For an N-particle system it is shown how a particular infinite-dimensional algebra arises as a generalization of the su(1,1) algebra which is present for the two-particle system.

arXiv:hep-th/9611167•Nov 21, 1996•6 citations

The principle of the indistinguishability of identical particles and the Lie algebraic approach to the field quantisation

A. B. Govorkov

The density matrix, rather than the wavefunction describing the system of a fixed number of non-relativistic identical particles, is subject to the second quantisation. Here the bilinear operators which move a particle from a given state to another appear and satisfy the Lie algebraic relations of the unitary group SU(p) when the dimension p to infinity . The drawing into consideration of the system with a variable number of particles implies the extension of this algebra into one of the simple Lie algebras of classical (orthogonal, symplectic or unitary) groups in the even-dimensional spaces. These Lie algebras correspond to the para-Fermi-, para-Bose- and para-uniquantisation of fields, respectively.

Journal of Physics A Mathematical and General•May 1, 1980•18 citations

Quantum Observables and Effect Algebras

Anatolij Dvurečenskij

arXiv:1609.06691•International Journal of Theoretical Physics•Nov 11, 2017•12 citations

Algebra of Observables and State Space

Nikolay N. Bogolubov, Анатолий Алексеевич Логунов, A. I. Oksak +2 more

Springer eBooks•Jan 1, 1990•0 citations
The density matrix, rather than the wavefunction describing the system of a fixed number of non-relativistic identical particles, is subject to the second quantisation. Here the bilinear operators which move a particle from a given state to another appear and satisfy the Lie algebraic relations of the unitary group SU(p) when the dimension p to infinity . The drawing into consideration of the system with a variable number of particles implies the extension of this algebra into one of the simple Lie algebras of classical (orthogonal, symplectic or unitary) groups in the even-dimensional spaces. These Lie algebras correspond to the para-Fermi-, para-Bose- and para-uniquantisation of fields, respectively.