FeigenbaumSharkovskiiMagnitskii (FSM) theory
In all complex nonlinear systems of differential equations describing numerous natural physical, chemical, biological, ecological, and also both economic and social processes and phenomena of a macrocosm, including dissipative and conservative, autonomous and nonautonomous systems, systems of ordinary and partial differential equations and differential equations with delay argument, it is carried out uniform universal bifurcation scenario of complication of dynamics of solutions through the Feigenbaum double period cascade of bifurcations of stable cycles or tori, then through the Sharkovskii subharmonic cascade of bifurcations of births of stable cycles or tori of any period up to the period three according to the Sharkovskii order
and then through the Magnitskii homoclinic or heteroclinic cascade of bifurcations of stable cycles or tori, converging to corresponding homoclinic or heteroclinic separatrix contours or surfaces.Example of the universal scenario of transition to dynamical chaos in twodimensional nonautonomous systems with periodic coefficients through the subharmonic cascade of bifurcations of stable cycles  generalized Mathieu equation (Fig.1):
Fig.1. Singular cycle, cycle of period 2, Feigenbaum attractor, cycle of period 3, singular cyclic chaotic attractor in the generalized Mathieu system
Example of the universal scenario of transition to dynamical chaos in autonomous systems through the subharmonic cascade of bifurcations of stable cycles – system of Rossler equations (Fig.2):
Fig.2. Singular cycle, cycle of period 4, Feigenbaum attractor, cycle of period 3, singular cyclic chaotic attractor in the Rossler system
Example of the universal scenario of transition to dynamical chaos in nonlinear partial differential equations through the subharmonic cascade of bifurcations of stable twodimensional tori – KuramotoTsuzuki (GinzburgLandau) equation (Fig.3):
Fig.3. Projections of sections of singular twodimensional torus of period 2, toroidal Feigenbaum attractor, twodimensional torus of period 3, singular chaotic toroidal attractor in the KT (GL) equation.
Example of the universal scenario of transition to turbulence in NavierStokes nonlinear partial differential equations through the subharmonic cascade of bifurcations of stable cycles and stable twodimensional tori – RayleighBenard convection(Fig.4):
Fig.4. Projections of the cycle of period 3 and real turbulent regime corresponding to him, twodimensional torus of period 2 and projection of its section
Publications.
Universal Theory of Dynamic and SpaceTime Chaos in Complex Systems.
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Теория динамического хаоса

 Nikola Tesla
 FeigenbaumSharkovskiiMagnitskii (FSM) theory
 Theory EDCW (electrodynamics of curvilinear waves) of A.Kyriakos
 Electrodynamics of physical vacuum
 Theory of elementary particles
 Gravitation and gravitational waves
 Author: Magnitskii N.A.