1988
DOI: 10.1016/0550-3213(88)90379-3
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The background field method and the non-linear σ-model

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Cited by 123 publications
(141 citation statements)
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“…(14) it is clear that these translations correspond to multiplying the SU (2) element, G, by a constant, diagonal SU (2) matrix from the left (respectively from the right). Since in the dual variables there is always a translational symmetry and the duality transformation amounts to a canonical transformation (classically) the 'ψ dual' is expected to show the full remaining SU (2) × U (1) symmetry of the original model (15), while for the φ dual only a U (1) × U (1) symmetry is expected.…”
Section: The Deformed Su(2) Principal σ-Model and Some Of Its Dualsmentioning
confidence: 99%
See 1 more Smart Citation
“…(14) it is clear that these translations correspond to multiplying the SU (2) element, G, by a constant, diagonal SU (2) matrix from the left (respectively from the right). Since in the dual variables there is always a translational symmetry and the duality transformation amounts to a canonical transformation (classically) the 'ψ dual' is expected to show the full remaining SU (2) × U (1) symmetry of the original model (15), while for the φ dual only a U (1) × U (1) symmetry is expected.…”
Section: The Deformed Su(2) Principal σ-Model and Some Of Its Dualsmentioning
confidence: 99%
“…The Lagrangian of the deformed σ-model given by Eq. (15) exhibits two obvious Abelian isometries that can be used to construct two different (Abelian) duals: namely the translations in the φ and ψ fields; we call the models obtained this way the 'φ dual' and the 'ψ dual' of the deformed σ model (15). From Eq.…”
Section: The Deformed Su(2) Principal σ-Model and Some Of Its Dualsmentioning
confidence: 99%
“…To examine the anomalies for (2,0)-supersymmetric sigma models with Nijenhuis symmetries, we quantise the theory in the background field method. As in the case of (2,0)-supersymmetric sigma models with target spaces complex manifolds, the model can be quantised in such a way that the background/quantum field split symmetry [14], (1,0) supersymmetry and sigma model manifold reparameterisations are manifestly preserved quantum mechanically. The arguments for this are similar to those of ref.…”
Section: Anomaliesmentioning
confidence: 99%
“…The currents of the theory are 14) where the components of the G 0 += , G 0 −= are the energy momentum tensor and the (1,0) and (0,1) supersymmetry currents, the components of G 1 ++ and G 1 −− are the (2,0) and (0,2) supersymmetry currents and two U(1) currents, and the components of P += and P −= are the currents corresponding to Nijenhuis symmetries. All the above currents are conserved, i.e.…”
Section: The Poisson Bracket Algebra Of Chargesmentioning
confidence: 99%
“…Therefore it is surprising that the counterterms of the sigma model with affine-metric manifold differ from counter terms of the sigma model with Riemannian manifold [6]. This difference can not be reduced to the metric redefenition caused by infinitesimal coordinate transformation [2] or to the nonlinear renormalization of the quantum fields [8]. In the paper [6], the counter terms are calculated for conventional sigma model without assuming a metric connection for the geodesic line equation in covariant background field method.…”
Section: Introductionmentioning
confidence: 99%