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The algebra of observables of planar electrons subject to a constant background magnetic field B is given by A_theta(R^2) x A_theta(R^2) the product of two mutually commuting Moyal algebras.
Z. F. Ezawa, Quantum Hall Effects
2000
Earlier work this paper cites.
R. Oeckl, Untwisting noncommutative R d R^{d} and the equivalence of quantum field theories,
2000
Earlier work this paper cites.
M. Chaichian, P. P. Kulish, K. Nishijima, and A. Tureanu, ”On a Lorentz-invariant interpretation of noncommutative space-time and its implications on noncommutative QFT”, Phys. Lett. B 604
2004
Cited alongside, same era.
P. Aschieri, C. Blohmann, M. Dimitrijevic, F. Meyer, P. Schupp, and J. Wess, A gravity theory on noncommutative spaces,
2005
Cited alongside, same era.
A. P. Balachandran, A. Pinzul, B. A. Qureshi, S. Vaidya “Poincare invariant gauge and gravity theories on the Groenewold-Moyal plane,” arXiv:hep-th/0608138
Cited in the paper.
J. Wess, ”Deformed coordinate spaces: Derivatives”, hep-th/0408080
Cited in the paper.
A. P. Balachandran, G. Mangano, A. Pinzul, and S. Vaidya, Spin and statistics on the Groenwald-Moyal plane: Pauli-forbidden levels and transitions,
2006
Later among the works it cites.
A. P. Balachandran, T. R. Govindarajan, G. Mangano, A. Pinzul, B. A. Qureshi and S. Vaidya, “Statistics and UV-IR mixing with twisted Poincare invariance,” Phys. Rev. D 75
2007
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