*-Wars Episode I: The Phantom Anomaly
arXiv:hep-th/0107199 · doi:10.1016/S0550-3213(01)00555-7
Abstract
As pointed out, chiral non-commutative theories exist, and examples can be constructed via string theory. Gauge anomalies require the matter content of individual gauge group factors, including U(1) factors, to be non-chiral. All ``bad'' mixed gauge anomalies, and also all ``good'' (e.g. for ) ABJ type flavor anomalies, automatically vanish in non-commutative gauge theories. We interpret this as being analogous to string theory, and an example of UV/IR mixing: non-commutative gauge theories automatically contain ``closed string,'' Green-Schwarz fields, which cancel these anomalies.
20 pages. Added references and minor typos corrected
References in corpus (1)
Cited by in corpus (18)
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- Noncommutative Standard Modelling
- Lattice Perturbation Theory in Noncommutative Geometry and Parity Anomaly in 3D Noncommutative QED
- Anomalies in noncommutative gauge theories, Seiberg-Witten transformation and Ramond-Ramond couplings
- Axial anomaly of QED in a strong magnetic field and noncommutative anomaly
- Noncommutativity and Model Building
- Translational-invariant noncommutative gauge theory
- UV/IR Mixing and Anomalies in Noncommutative Gauge Theories
- Effective actions, Wilson lines and the IR/UV mixing in noncommutative supersymmetric gauge theories
- The U(1)A anomaly in noncommutative SU(N) theories
- Consistent Anomalies in Translation-Invariant Noncommutative Gauge Theories
- On the Anomalies and Schwinger Terms in Noncommutative Gauge Theories
- Conformal Anomalies in Noncommutative Gauge Theories
- Planar and Nonplanar Konishi Anomalies and Effective Superpotential for Noncommutative N=1 Supersymmetric U(1)
- High-Energy Scattering in Non-Commutative Field Theory