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Bullough–Dodd model : ウィキペディア英語版
Bullough–Dodd model
The Bullough–Dodd model is an integrable model in 1+1-dimensional quantum field theory introduced by Robin Bullough and Roger Dodd. Its
Lagrangian density is
:\mathcal=\frac(\partial_\mu\phi)^2-\frac(2e^
+e^)

where m_0\, is a mass parameter, g\, is the coupling constant and \phi\, is a real scalar field.
The Bullough–Dodd model belongs to the class of Affine Toda Field Theories.
The spectrum of the model consists of a single massive particle.
==See also==

*List of integrable models

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