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The Bullough-Dodd model is an integrable model in 1+1-dimensional quantum field theory. Its Lagrangian density is

\( \mathcal{L}=\frac{1}{2}(\partial_\mu\phi)^2-\frac{m_0^2}{6g^2}(2e^{g\phi} +e^{-2g\phi}) \)

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

References

R.K. Dodd, R.K. Bullough, Proc.Roy.Soc.Lond. A352, 481, 1977
A. Fring, G. Mussardo, P. Simonetti, Phys.Lett. B307, 83-90, 1993, arXiv: hep-th/9303108

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