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Using general but simple covariance arguments, we classify the `quantum' Minkowski spaces for dimensionless deformation parameters. This requires a previous analysis of the associated Lorentz groups, which reproduces a previous…

q-alg · Mathematics 2008-11-26 J. A. de Azcarraga , F. Rodenas

We twist the Hopf algebra of igl(n,R) to obtain the kappa-deformed spacetime coordinates. Coproducts of the twisted Hopf algebras are explicitly given. The kappa-deformed spacetime obtained this way satisfies the same commutation relation…

High Energy Physics - Theory · Physics 2008-11-26 Jong-Geon Bu , Hyeong-Chan Kim , Youngone Lee , Chang Hyon Vac , Jae Hyung Yee

The theory of twistors on foliated manifolds is developed and the twistor space of the normal bundle is constructed. It is demonstrated that the classical constructions of the twistor theory lead to foliated objects and permit to formulate…

Differential Geometry · Mathematics 2022-02-08 Rouzbeh Mohseni , Robert A. Wolak

The algebra of biquaternions possess a manifestly Lorentz invariant form and induces an extended space-time geometry. We consider the links between this complex pre-geometry and real geometry of the Minkowski space-time. Twistor structures…

General Relativity and Quantum Cosmology · Physics 2022-09-05 Vladimir V. Kassandrov , Nina V. Markova

Symmetric ordering and Weyl realizations for non commutative quantum Minkowski spaces are reviewed. Weyl realizations of Lie deformed spaces and corresponding star products, as well as twist corresponding to Weyl realization and coproduct…

Mathematical Physics · Physics 2022-12-21 Stjepan Meljanac , Zoran Škoda , Sasa Kresic-Juric

Massless particle dynamics in $D=10$ Minkowski space is given an $E_7$-covariant formulation, including both space-time and twistor variables. $E_7$ contains the conformal algebra as a subalgebra. Analogous constructions apply to $D=3,4$…

High Energy Physics - Theory · Physics 2009-10-22 Martin Cederwall

A useful concept in the development of physical models on the $\kappa$-Minkowski noncommutative spacetime is that of a curved momentum space. This structure is not unique: several inequivalent momentum space geometries have been identified.…

High Energy Physics - Theory · Physics 2020-08-14 Fedele Lizzi , Flavio Mercati , Mattia Manfredonia

The twistor construction is applied for obtaining examples of generalized complex structures (in the sense of N. Hitchin) that are not induced by a complex or a symplectic structure.

Differential Geometry · Mathematics 2009-11-11 Johann Davidov , Oleg Mushkarov

The role of the quantum universal enveloping algebras of symmetries in constructing non-commutative geometry of the space-time including vector bundles, measure, equations of motion and their solutions is discussed. In the framework of the…

Quantum Algebra · Mathematics 2011-07-26 P. P. Kulish , A. I. Mudrov

Starting from the standard supertwistor realizations for conformally compactified N-extended Minkowski superspaces in three and four space-time dimensions, we elaborate on alternative realizations in terms of graded two-forms on the dual…

High Energy Physics - Theory · Physics 2015-06-05 Sergei M. Kuzenko

A hypercomplex structure on a differentiable manifold consists of three integrable almost complex structures that satisfy quaternionic relations. If, in addition, there exists a metric on the manifold which is Hermitian with respect to the…

Differential Geometry · Mathematics 2019-08-13 Artour Tomberg

We describe a general procedure, based on Gerstenhaber-Schack complexes, for extending to quantized twistor spaces the Donaldson-Friedman gluing of twistor spaces via deformation theory of singular spaces. We consider in particular various…

Mathematical Physics · Physics 2020-12-08 Matilde Marcolli , Roger Penrose

The space-time symmetry of noncommutative quantum field theories with a deformed quantization is described by the twisted Poincar\'e algebra, while that of standard commutative quantum field theories is described by the Poincar\'e algebra.…

High Energy Physics - Theory · Physics 2008-11-26 Yasumi Abe

We show that a two twistor phase space {\`a} priori describing two non localized massless and spinning particles may be decomposed into a product of three independent phase spaces: the (forward) cotangent bundle of the Minkowski space, the…

High Energy Physics - Theory · Physics 2007-05-23 Andreas Bette , Stanislaw Zakrzewski

We introduce a covariant non-commutative deformation of 3+1-dimensional conformal field theory. The deformation depends on a short-distance scale \ell_p, and thus breaks scale invariance, but preserves all space-time isometries. The…

High Energy Physics - Theory · Physics 2015-06-18 Jonathan Heckman , Herman Verlinde

We prove that the Moyal product is covariant under linear affine spacetime transformations. From the covariance law, by introducing an $(x,\Theta)$-space where the spacetime coordinates and the noncommutativity matrix components are on the…

High Energy Physics - Theory · Physics 2014-11-18 J. M. Gracia-Bondia , Fedele Lizzi , F. Ruiz Ruiz , Patrizia Vitale

Consistency conditions for the local existence of massless spin 3/2 fields has been explored that the field equations for massless helicity 3/2 are consistent iff the space-time is Ricci-flat and that in Minkowski space-time the space of…

High Energy Physics - Theory · Physics 2009-11-07 Mitsuo J. Hayashi

Stabilization, by deformation, of the Poincar\'{e}-Heisenberg algebra requires both the introduction of a fundamental lentgh and the noncommutativity of translations which is associated to the gravitational field. The noncommutative…

Mathematical Physics · Physics 2017-11-02 R. Vilela Mendes

We consider noncommutative geometries obtained from a triangular Drinfeld twist. This allows to construct and study a wide class of noncommutative manifolds and their deformed Lie algebras of infinitesimal diffeomorphisms. This way symmetry…

Quantum Algebra · Mathematics 2010-05-13 Paolo Aschieri

A spinless covariant field $\phi$ on Minkowski spacetime $\M^{d+1}$ obeys the relation $U(a,\Lambda)\phi(x)U(a,\Lambda)^{-1}=\phi(\Lambda x+a)$ where $(a,\Lambda)$ is an element of the Poincar\'e group $\Pg$ and $U:(a,\Lambda)\to…

High Energy Physics - Theory · Physics 2011-04-04 A. P. Balachandran , A. Ibort , G. Marmo , M. Martone