Abstract
Gas detonation is a complex multidimensional process. In nature, the multidimensionality of detona� tion manifests itself in the cellular structure and in the spin. The cellular and spin detonations are formed due to instability of the burning zone behind the head shock wave, due to which small perturbations increase, and periodic spatial flows arise with trans� verse waves in the flow behind the head shock and with breaks of its front [1–4]. Previously, various authors investigated mainly numerically the formation of the 2D cellular detonation in the channels. In this case, the triple points in the spots of breaks of the 2D deto�
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