TeV scale implications of non commutative space time in laboratory frame with polarized beams
From MaRDI portal
Publication:467329
DOI10.1007/JHEP07(2011)024zbMath1298.81460arXiv1105.5203MaRDI QIDQ467329
Publication date: 3 November 2014
Published in: Journal of High Energy Physics (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/1105.5203
Unified quantum theories (81V22) String and superstring theories; other extended objects (e.g., branes) in quantum field theory (81T30) Noncommutative geometry methods in quantum field theory (81T75) Inelastic and multichannel quantum scattering (81U35)
Related Items (2)
Probing space–time noncommutativity in the top quark pair production at e+e- collider ⋮ Minimal NCSM direct photon production in proton-antiproton collisions
Uses Software
Cites Work
- Renormalisability of the matter determinants in noncommutative gauge theory in the enveloping-algebra formalism
- Constraining noncommutative field theories with holography
- The standard model on non-commutative space-time: electroweak currents and the Higgs sector
- The standard model on non-commutative space-time: strong interactions included
- Some phenomenological consequences of the time-ordered perturbation theory of QED on non-commutative spacetime
- General properties of non-commutative field theories
- Enveloping algebra-valued gauge transformations for non-abelian gauge groups on non-commutative spaces
- String theory and noncommutative geometry
- The gauge anomaly and the Seiberg-Witten map
- Renormalizability and phenomenology of θ‐expanded noncommutative gauge field theory
- Quantized Space-Time
- Noncommutative perturbative dynamics
- The IR/UV connection in non-commutative gauge theories
- Construction of non-Abelian gauge theories on noncommutative spaces
- The standard model on non-commutative space-time
This page was built for publication: TeV scale implications of non commutative space time in laboratory frame with polarized beams
