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G M Chechin

Publications and source records attributed to G M Chechin.

3 recordsLinked to original sources

Quasibreathers as a generalization of the concept of discrete breathers.

The majority of dynamical objects, which demonstrate energy localization in nonlinear lattices, represent quasibreathers rather than strictly time-periodic discrete breathers since, as a rule, there exist certain deviations in vibrational frequencies of the individual particles exceeding the possible numerical errors. We illustrate this idea with the James breathers in the K2-K3-K4 chain and with quasibreathers in the K4 chain. For the latter case, a rigorous investigation of existence and stability of the breathers and quasibreathers is presented. In particular, it is proved that they are stable up to a certain strength of the intersite part of the potential with respect to its on-site part. We conjecture that quasibreathers play a fundamental role in the problem of energy localization in more realistic nonlinear lattices, as well. The difference between breathers and quasibreathers can be characterized by the mean square deviation of the frequencies of individual particles.

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Stability analysis of dynamical regimes in nonlinear systems with discrete symmetries.

We present a theorem that allows one to simplify the linear stability analysis of periodic and quasiperiodic nonlinear regimes in N-particle mechanical systems with different kinds of discrete symmetry. This theorem suggests a decomposition of the linearized system arising in the standard stability analysis into a number of subsystems whose dimensions can be considerably less than the dimension of the full system. As an example of such a simplification, we discuss the stability of bushes of modes (invariant manifolds) for the Fermi-Pasta-Ulam chains and prove another theorem about the maximal dimension of the above-mentioned subsystems.

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Three-dimensional chaotic flows with discrete symmetries.

There are a number of well-known three-dimensional flows with quadratic nonlinearities, which demonstrate a chaotic behavior. The most popular among them are Lorenz and Rössler systems. Using an exhaustive computer search, J. Sprott found 19 examples of chaotic flows with either five terms and two quadratic nonlinearities or six terms and one nonlinearity [Phys. Rev. E 50, R647 (1994)]. In contrast to this approach, we use symmetry-related considerations to construct types of chaotic flows with an arbitrary dimension. The discussion is based on our previous work devoted to nonlinear dynamics of the physical systems with discrete symmetries [see Physica D 117, 43 (1998), etc.]. Here, we present all possible chaotic flows with quadratic nonlinearities which are invariant under the action of 32 point groups of crystallographic symmetry. These systems demonstrate a typical chaotic behavior as well as general dynamical properties of nonlinear systems with discrete symmetries. In particular, we found a dynamical system with the point symmetry group D2 which seems to be more simple and more elegant than those by Lorenz and Rössler.

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