Abstract

Usually, the physical interest of the Lorenz system is restricted to the region where its three parameters are positive. However, this famous system appears, when $$\sigma <0$$ , in the study of a thermosolutal convection model and in the analysis of traveling-wave solutions of the Maxwell–Bloch equations. In this context, a Takens–Bogdanov bifurcation of heteroclinic type becomes an important organizing center. It has been very recently shown that the periodic orbit born in the Hopf bifurcation of the origin undergoes a torus bifurcation. In this paper we perform a detailed numerical study of the resonances of periodic orbits in the three-parameter Lorenz system, $$ \dot{x} = \sigma (y-x), \ \dot{y} = \rho x - y - xz, \ \dot{z} = -bz + xy, $$ when $$\sigma <0$$ and $$\rho , b >0$$ . The combination of numerical continuation methods and Poincare sections of the flow provides important information of how the resonances appear and evolve giving rise to a very rich dynamical and bifurcation scenario.

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