TY - JOUR
T1 - Quantum orthogonal planes
T2 - ISOq,r(N) and SOq,r(N) - Bicovariant calculi and differential geometry on quantum Minkowski space
AU - Aschieri, P.
AU - Castellani, L.
AU - Scarfone, A. M.
PY - 1999
Y1 - 1999
N2 - We construct differential calculi on multiparametric quantum orthogonal planes in any dimension N. These calculi are bicovariant under the action of the full inhomogeneous (multiparametric) quantum group ISOq,r(N), and do contain dilatations. If we require bicovariance only under the quantum orthogonal group SOq,r(N), the calculus on the q-plane can be expressed in terms of its coordinates cursive Greek chia, differentials dcursive Greek chia and partial derivatives ∂a without the need of dilatations, thus generalizing known results to the multiparametric case. Using real forms that lead to the signature (n + 1, m) with m=n - 1, n, n + 1, we find ISOq,r(n + 1, m) and SOq,r(n + 1, m) bicovariant calculi on the multiparametric quantum spaces. The particular case of the quantum Minkowski space ISOq,r(3, 1)/SOq,r(3, 1) is treated in detail. The conjugated partial derivatives ∂*a can be expressed as linear combinations of the ∂a. This allows a deformation of the phase-space where no additional operators (besides cursive Greek chia and pa) are needed.
AB - We construct differential calculi on multiparametric quantum orthogonal planes in any dimension N. These calculi are bicovariant under the action of the full inhomogeneous (multiparametric) quantum group ISOq,r(N), and do contain dilatations. If we require bicovariance only under the quantum orthogonal group SOq,r(N), the calculus on the q-plane can be expressed in terms of its coordinates cursive Greek chia, differentials dcursive Greek chia and partial derivatives ∂a without the need of dilatations, thus generalizing known results to the multiparametric case. Using real forms that lead to the signature (n + 1, m) with m=n - 1, n, n + 1, we find ISOq,r(n + 1, m) and SOq,r(n + 1, m) bicovariant calculi on the multiparametric quantum spaces. The particular case of the quantum Minkowski space ISOq,r(3, 1)/SOq,r(3, 1) is treated in detail. The conjugated partial derivatives ∂*a can be expressed as linear combinations of the ∂a. This allows a deformation of the phase-space where no additional operators (besides cursive Greek chia and pa) are needed.
UR - http://www.scopus.com/inward/record.url?scp=0000273180&partnerID=8YFLogxK
U2 - 10.1007/s100529800968
DO - 10.1007/s100529800968
M3 - Article
SN - 1434-6044
VL - 7
SP - 159
EP - 175
JO - European Physical Journal C
JF - European Physical Journal C
IS - 1
ER -