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

International Journal of Theoretical Physics

An extended Galilei group and its application

O. Holmaas

Published May 1, 1971• 0 citations
Publisher
DOI
10.1007/bf00673800

Related papers

Representations of the Galilei Group

Erdal İnönü, E. P. Wigner

Springer eBooks•Jan 1, 1993•0 citations

Representations of the Galilei group

Erdal İnönü, Eugene Paul Wigner

Il Nuovo Cimento•Aug 1, 1952•180 citations

The exotic Galilei group and the “Peierls substitution”

Christian Duval, P. A. Horváthy

arXiv:hep-th/0002233•Physics Letters B•Apr 1, 2000•294 citations

Galilei group and Liouville equation

A. Loinger

Annals of Physics•Oct 1, 1962•24 citations

Galilei covariance and quasi-free representations of Fermi fields

K. Kraus, H -G Stark

Some quasi-free irreducible representations of the CAR algebra of a non-relativistic free Fermi field are constructed, which are covariant under certain subgroups of the extended Galilei group. The construction of fully covariant (but reducible) representations as direct integrals of partially covariant ones is described. This method is also applicable to arbitrary C*-algebras and other covariance groups.

Journal of Physics A Mathematical and General•Jul 1, 1982•2 citations

Time dependent quantum generators for the Galilei group

G. Filippelli

In 1995, Doebner and Mann introduced an approach to the ray representations of the Galilei group in (1 + 1)-dimensions, giving rise to quantum generators with an explicit dependence on time. Recently (2004), Wawrzycki proposed a generalization of Bargmann's theory: in his paper, he introduce phase exponents that are explicitely dependent by 4-space point. In order to find applications of such generalization, we extend the approach of Doebner and Mann to higher dimensions: as a result, we determine the generators of the ray representation in (2 + 1) and (3 + 1) dimensions. The differences of the outcoming formal apparatus with respect to the smaller dimension case are established.

arXiv:1411.6048•Journal of Mathematical Physics•Aug 1, 2011•2 citations
In 1995, Doebner and Mann introduced an approach to the ray representations of the Galilei group in (1 + 1)-dimensions, giving rise to quantum generators with an explicit dependence on time. Recently (2004), Wawrzycki proposed a generalization of Bargmann's theory: in his paper, he introduce phase exponents that are explicitely dependent by 4-space point. In order to find applications of such generalization, we extend the approach of Doebner and Mann to higher dimensions: as a result, we determine the generators of the ray representation in (2 + 1) and (3 + 1) dimensions. The differences of the outcoming formal apparatus with respect to the smaller dimension case are established.