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Kazuyuki Yagasaki

Publications and source records attributed to Kazuyuki Yagasaki.

At least 19 recordsLinked to original sources

Smooth integrability of diffeomorphisms

Motivated by the notion of integrability introduced by Bogoyavlenskij for vector fields, we propose a definition of smooth integrability for general diffeomorphisms. In brief, we say that a diffeomorphism is integrable if it commutes with the flows of {\color{black}commutative} vector fields and shares their first integrals. We establish a Liouville-Arnold type theorem and prove that on connected invariant level sets of the first integrals, a smoothly integrable diffeomorphism is conjugate to a skew translation on a toroidal cylinder, and in particular, when the level sets are compact, the induced dynamics is quasiperiodic, as in the classical Hamiltonian case. We further show that linear diffeomorphisms on real or complex Euclidean spaces are integrable in our sense, as is the case for linear vector fields in the sense of Bogoyavlenskij, and symplectic diffeomorphisms that are integrable in their standard Liouville-type definition are integrable in our framework. We also modify the cotangent lift construction, which is useful in the treatment of integrability of vector fields, for diffeomorphisms, and show that integrability is preserved under this correspondence. Several examples are provided to illustrate the scope of the theory.

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Feedback control of the Kuramoto model defined on uniform graphs I: Deterministic natural frequencies

We study feedback control of the Kuramoto model with uniformly spaced natural frequencies defined on uniform graphs which may be complete, random dense or random sparse. The control objective is to drive all nodes to the same constant rotational motion. For the case of node number $n\ge 3$, we establish the existence of exactly $2^n$ synchronized solutions in the controlled Kuramoto model (CKM) and their saddle-node and pitchfork bifurcations, and determine their stability. In particular, we show that only a solution converging to the desired motion in the limit of infinite feedback gain is stable and the others are unstable. Based on the previous results, it is shown that (i) the solution to which the stable synchronized solution in the CKM converge as $n\to\infty$ is always asymptotically stable in the continuous limit (CL) if it exists, and (ii) the asymptotically stable solution of the CL captures the asymptotic behavior of the CKM when the node number is sufficiently large, even if the graphs are random dense or sparse. We demonstrate the theoretical results by numerical simulations for the CKM on complete simple, and uniform random dense and sparse graphs.

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Feedback control of twisted states in the Kuramoto model on nearest neighbor and complete simple graphs

We study feedback control of twisted states in the Kuramoto model (KM) of identical oscillators defined on deterministic nearest neighbor graphs containing complete simple ones when it may have phase-lag. Bifurcations of such twisted solutions in the continuum limit (CL) for the uncontrolled KM defined on nearest neighbor graphs that may be deterministic dense, random dense or random sparse were discussed very recently by using the center manifold reduction, which is a standard technique in dynamical systems theory. In this paper we analyze the stability and bifurcations of twisted solutions in the CL for the KM subjected to feedback control. In particular, it is shown that the twisted solutions exist and can be stabilized not only for nearest neighbor graphs but also for complete simple graphs. Moreover, the CL is shown to suffer bifurcations at which the twisted solution becomes unstable and a stable one-parameter family of modulated or oscillating twisted solutions is born, depending on whether the phase-lag is zero or not. We demonstrate the theoretical results by numerical simulations for the feedback controlled KM on deterministic nearest neighbor and complete simple graphs.

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Bifurcations of twisted solutions in a continuum limit for the Kuramoto model on nearest neighbor graphs

We study bifurcations of twisted solutions in a continuum limit (CL) for the Kuramoto model (KM) of identical oscillators defined on nearest neighbor graphs, which may be deterministic dense, random dense or random sparse, when it may have phase-lag. We use the center manifold reduction, which is a standard technique in dynamical systems theory, and prove that the CL suffers bifurcations at which the one-parameter family of twisted solutions becomes unstable and a stable or unstable two-parameter family of modulated twisted solutions that oscillate or not depending on whether the phase-lag exists or not is born. We demonstrate the theoretical results by numerical simulations for the KM on deterministic dense, random dense and random sparse graphs.

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Bifurcations of synchronized solutions in a continuum limit of the Kuramoto model with two-mode interaction depending on two graphs

We study bifurcations of the completely synchronized state in a continuum limit (CL) for the Kuramoto model (KM) of identical oscillators with two-mode interaction depending on two graphs. Here one of the graphs is uniform but may be deterministic dense, random dense or random sparse, and the other is a deterministic finite nearest neighbor. We use the center manifold reduction technique, which is a standard one in dynamical systems, and prove that the CL suffers bifurcations at which the one-parameter family of completely synchronized state becomes unstable and a stable two-parameter family of $\ell$-humped sinusoidal shape stationary solutions ($\ell\ge 2$) appears. This contrasts the author's recent result on the classical KM for which bifurcation behavior in its CL is very different from ones in the KM and difficult to explain by standard techniques in dynamical systems such as the center manifold reduction. Moreover, similar bifurcation behavior is shown to occur in the KM, based on the previous fundamental results. The occurrence of such bifurcations were suggested by numerical simulations for the deterministic graphs in a previous study. We also demonstrate our theoretical results by numerical simulations for the KM with the zero natural frequency.

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Bifurcations and stability of synchronized solutions in the Kuramoto model with uniformly spaced natural frequencies

We consider the classical Kuramoto model (KM) with natural frequencies and its continuum limit (CL), and discuss the existence of synchronized solutions and their bifurcations and stability. We specifically assume that the frequency function is symmetric and linear in the CL, so that the natural frequencies are evenly spaced in the KM. We show that in the KM, $O(2^n)$ one-parameter families of synchronized solutions are born and $O(2^n)$ saddle-node and pitchfork bifurcations occur at least, when the node number $n$ is odd and tends to infinity. Moreover, we prove that the family of synchronized solutions obtained in the previous work suffers a saddle-node bifurcation at which its stability changes from asymptotically stable to unstable and the other families of synchronized solutions are unstable in the KM. For the CL, we show that a one-parameter family of continuous synchronized solutions obtained in the previous work is asymptotically stable and that there exist uncountably many one-parameter families of discontinuous synchronized solutions and they are unstable along with another one-parameter family of continuous synchronized solutions.

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Continuum limit of the Kuramoto model with random natural frequencies on uniform graphs

We study the Kuramoto model (KM) having random natural frequencies and defined on uniform graphs that may be complete, random dense or random sparse. The natural frequencies are assumed to be independent and identically distributed on a bounded interval. In the previous work, the corresponding continuum limit (CL) was proven to approximate stable motions in the KM well when the natural frequencies are deterministic, even if the graph is not uniform, although it may not do so for unstable motions and bifurcations. We show that the method of CLs is still valid even when the natural frequencies are random, especially uniformly distributed. In particular, an asymptotically stable family of solutions to the CL is proven to behave in the $L^2$ sense as if it is an asymptotically stable one in the KM, under an appropriate uniform random permutation. We demonstrate the theoretical results by numerical simulations for the KM with uniformly distributed random natural frequencies.

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Solvability of the Zakharov-Shabat systems with meromorphic potentials by quadrature

We study the solvability of the general two-dimensional Zakharov-Shabat (ZS) systems with meromorphic potentials by quadrature. These systems appear in application of the inverse scattering transform (IST) to an important class of nonlinear partial differential equations (PDEs) called integrable systems. Their solvability by quadrature is a key to obtain analytical expressions for solutions to the initial value problems of the integrable PDEs by using the IST. We prove that the ZS systems are always integrable in the sense of differential Galois theory, i.e., solvable by quadrature, if and only if the meromporphic potentials are reflectionless, under the condition that the potentials are absolutely integrable on $\mathbb{R}\setminus(-R_0,R_0)$ for some $R_0>0$. Similar statements were previously proved to be true by the author for a limited class of potentials and the linear Schrödinger equations.

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Solvability of the Korteweg-de Vries equation under meromorphic initial conditions by quadrature

We study the solvability of the Korteweg-de Vries equation under meromorphic initial conditions by quadrature when the inverse scattering transform (IST) is applied. It is a key to solve the Schrödinger equation appearing in the Lax pair in application of the IST. We show that the Schrödinger equation is always integrable in the sense of differential Galois theory, i.e., solvable by quadrature, if and only if the meromporphic potential is reflectionless, under the condition that the potential is absolutely integrable on $\mathbb{R}\setminus(-R_0,R_0)$ for some $R_0>0$.This statement was previously proved to be true by the author for a limited class of potentials. We also show that the Schrödinger equation is not integrable in this sense for rational potentials that decay at infinity but do not satisfy the weak condition.

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Nonintegrability of time-periodic perturbations of analytically integrable systems near homo- and heteroclinic orbits

We consider time-periodic perturbations of analytically integrable systems in the sense of Bogoyavlenskij and study their \emph{real-meromorphic} nonintegrability, using a generalized version due to Ayoul and Zung of the Morales-Ramis theory. The perturbation terms are assumed to have finite Fourier series in time, and the perturbed systems are rewritten as higher-dimensional autonomous systems having the small parameter as a state variable. We show that if the Melnikov functions are not constant, then the autonomous systems are not \emph{real-meromorphically} integrable near homo- and heteroclinic orbits. We illustrate the theory for rotational motions of a periodically forced rigid body, which provides a mathematical model of a quadrotor helicopter.

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Nonintegrability of time-periodic perturbations of single-degree-of-freedom Hamiltonian systems near homo- and heteroclinic orbits

We consider time-periodic perturbations of single-degree-of-freedom Hamiltonian systems and study their real-meromorphic nonintegrability in the Bogoyavlenskij sense using a generalized version due to Ayoul and Zung of the Morales-Ramis theory. The perturbation terms are assumed to have finite Fourier series in time, and the perturbed systems are rewritten as higher-dimensional autonomous systems having the small parameter as a state variable.We show that if the Melnikov functions are not constant, then the autonomous systems are not real-meromorphically integrable near homo- and heteroclinic orbits. Our result is not just an extension of previous results for homocliic orbits to heteroclinic orbits and provides a stronger conclusion than them for the case of homoclinic orbits. We illustrate the theory for two periodically forced Duffing oscillators and a periodically forced two-dimensional system.

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Nonintegrability of the restricted three-body problem

The problem of nonintegrability of the circular restricted three-body problem is very classical and important in the theory of dynamical systems. It was partially solved by Poincare in the nineteenth century: He showed that there exists no real-analytic first integral which depends analytically on the mass ratio of the second body to the total and is functionally independent of the Hamiltonian. When the mass of the second body becomes zero, the restricted three-body problem reduces to the two-body Kepler problem. We prove the nonintegrability of the restricted three-body problem both in the planar and spatial cases for any nonzero mass of the second body. Our basic tool of the proofs is a technique developed here for determining whether perturbations of integrable systems which may be non-Hamiltonian are not meromorphically integrable near resonant periodic orbits such that the first integrals and commutative vector fields also depend meromorphically on the perturbation parameter. The technique is based on generalized versions due to Ayoul and Zung of the Morales-Ramis and Morales-Ramis-Simo theories.

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Continuum limits of coupled oscillator networks depending on multiple sparse graphs

The continuum limit provides a useful tool for analyzing coupled oscillator networks. Recently, Medvedev (Comm. Math. Sci., 17 (2019), no. 4, pp. 883-898) gave a mathematical foundation for such an approach when the networks are defined on single graphs which may be dense or sparse, directed or undirected, and deterministic or random. In this paper, we consider coupled oscillator networks depending on multiple graphs, and extend his results to show that the continuum limit is also valid in this situation. Specifically, we prove that the initial value problem (IVP) of the corresponding continuum limit has a unique solution under general conditions and that the solution becomes the limit of those to the IVP of the networks in some adequate meaning. Moreover, we show that if solutions to the networks are stable or asymptotically stable when the node number is sufficiently large, then so are the corresponding solutions to the continuum limit, and that if solutions to the continuum limit are asymptotically stable, then so are the corresponding solutions to the networks in some weak meaning as the node number tends to infinity. These results can also be applied to coupled oscillator networks with multiple frequencies by regarding the frequencies as a weight matrix of another graph. We illustrate the theory for three variants of the Kuramoto model along with numerical simulations.

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Nonintegrability of truncated Poincare-Dulac normal forms of resonance degree two

We give sufficient conditions for three- or four-dimensional truncated Poincare-Dulac normal forms of resonance degree two to be meromorphically nonintegrable when the Jacobian matrices have a zero and pair of purely imaginary eigenvalues or two incommensurate pairs of purely imaginary eigenvalues at the equilibria. For this purpose, we reduce their integrability to that of simple planar systems, and use an approach for proving the meromorphic nonintegrability of planar systems, which is similar to but more sophisticated than the previously developed one. Our result also implies that general three- or four-dimensional systems are analytically nonintegrable if they are formally transformed into one of the truncated normal forms satisfying the sufficient conditions.

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Periodic perturbations of codimension-two bifurcations with a double zero eigenvalue in dynamical systems with symmetry

We study bifurcation behavior in periodic perturbations of two-dimensional symmetric systems exhibiting codimension-two bifurcations with a double eigenvalue when the frequencies of the perturbation terms are small. We transform the periodically perturbed system to a simpler one which is a periodic perturbation of the normal form for codimension-two bifurcations with a double zero eigenvalue and symmetry, and apply the subharmonic and homoclinic Melnikov methods to analyze bifurcations occurring in the system. In particular, we show that there exist transverse homoclinic or heteroclinic orbits, which yield chaotic dynamics, in wide parameter regions. These results can be applied to three or higher-dimensional systems and even to infinite-dimensional systems with the assistance of center manifold reduction and the invariant manifold theory. We illustrate our theory for a pendulum subjected to position and velocity feedback control when the desired position is periodic in time. We also give numerical computations by the computer tool AUTO to demonstrate the theoretical results.

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Nonintegrability of dynamical systems near degenerate equilibria

We prove that general three- or four-dimensional systems %of differential equations are real-analytically nonintegrable near degenerate equilibria in the Bogoyavlenskij sense under additional weak conditions when the Jacobian matrices have a zero and pair of purely imaginary eigenvalues or two incommensurate pairs of purely imaginary eigenvalues at the equilibria. For this purpose, we reduce their integrability to that of the corresponding Poincare-Dulac normal forms and further to that of simple planar systems, and use a novel approach for proving the analytic nonintegrability of planar systems. Our result also implies that general three- and four-dimensional systems exhibiting fold-Hopf and double-Hopf codimension-two bifurcations, respectively, are real-analytically nonintegrable under the weak conditions. To demonstrate these results, we give two examples for the Rossler system and coupled van der Pol oscillators.

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Nonintegrability of the SEIR epidemic model

We prove the nonintegrability of the susceptible-exposed-infected-removed (SEIR) epidemic model in the Bogoyavlenskij sense. This property of the SEIR model is different from the more fundamental susceptible-infected-removed (SIR) model, which is Bogoyavlenskij-nonintegrable. Our basic tool for the proof is an extension of the Morales-Ramis theory due to Ayoul and Zung. Moreover, we extend the system to a six-dimensional system to treat transcendental first integrals and commutative vector fields. We also use the fact that the incomplete gamma function $Γ(α,x)$ is not elementary for $α\not\in\mathbb{N}$, of which a proof is included.

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A new proof of Poincaré's result on the restricted three-body problem

The problem of nonintegrability of the circular restricted three-body problem is very classical and important in dynamical systems. In the first volume of his masterpieces, Henri Poincaré showed the nonexistence of a real-analytic first integral which is functionally independent of the Hamiltonian and real-analytic in a small parameter representing the mass ratio as well as in the state variables, in both the planar and spatial cases. However, his proof was very complicated and unclear. In this paper, we give a new and simple proof of a very similar result for both the planar and spatial cases, using an approach which the author developed recently for nearly integrable systems.

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