1971
DOI: 10.1016/0370-2693(71)90582-x
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Consequences of anomalous ward identities

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Cited by 2,782 publications
(2,590 citation statements)
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“…The first and second terms are the normal Skyrme Lagrangians and the third term is the contribution of the chiral anomaly called the Wess-Zumino term [4][5][6]. The last term in Eq.…”
Section: Methodsmentioning
confidence: 99%
“…The first and second terms are the normal Skyrme Lagrangians and the third term is the contribution of the chiral anomaly called the Wess-Zumino term [4][5][6]. The last term in Eq.…”
Section: Methodsmentioning
confidence: 99%
“…In addition to the non-resonant S -wave, the resonant π-π S -wave with a pole at (512± 15)− i(188±12) MeV, interpreted as the broad σ meson, plays an essential role in the η → πππ decays. Due to the large interference between non-resonant and resonant S -waves, only the sum is used to describe the S -wave contribution, and the branching fractions Theoretically the non-resonant part of coupling in η → γπ + π − is accounted for by the higher term of Wess-Zumino-Witten (WZW) ChPT Lagrangian [26](also known as the box anomaly). However the decay dynamics of η → γπ + π − has been explored with very limited statistics only and new measurements are needed to clarify the scenario.…”
Section: Light Meson Decaysmentioning
confidence: 99%
“…[6] it was argued that this picture is not complete, but that a Wess-Zumino-Witten (WZW) term [7] should be added to the Lagrangian of the model. WZW terms typically occur if the symmetry breaking at the scale Λ is facilitated by some strong dynamics.…”
Section: The Little Higgs and T-paritymentioning
confidence: 99%