In the theory of dynamical systems (or turbulent flow), the Pomeau–Manneville scenario is the transition to chaos (turbulence) due to intermittency.[1][2] Named after Yves Pomeau and Paul Manneville.

References

  1. ↑ Pomeau, Yves; Manneville, Paul (1980). "Intermittent Transition to Turbulence in Dissipative Dynamical Systems". Commun. Math. Phys. 74 (2): 189–197. Bibcode:1980CMaPh..74..189P. doi:10.1007/BF01197757. S2CID 56371194.
  2. ↑ Eckmann, J.-P. (1981). "Roads to turbulence in dissipative dynamical systems". Rev. Mod. Phys. 53 (4): 643–654. Bibcode:1981RvMP...53..643E. doi:10.1103/RevModPhys.53.643.


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