Abstract:We study a necessary condition for the integrability of the polynomials fields in the plane by means of the differential Galois theory. More concretely, by means of the variational equations around a particular solution it is obtained a necessary condition for the existence of a rational first integral. The method is systematic starting with the first order variational equation. We illustrate this result with several families of examples. A key point is to check wether a suitable primitive is elementary or not… Show more
“…Using this expression, we write the kth-order VE of (3.2) along the periodic orbit (x, ε) = (x(t), 0) as 1) , y (2) ) + 2 f (1,1) (y (1) , χ (2) ) + 2 f (1,1) (y (1) , χ (2) ) + 2 f (0,2) (χ (1) , χ (2) )…”
Section: Proof Of Theorem 12mentioning
confidence: 99%
“…where such terms as (y(1)) 0 and (χ (1) ) 0 = 1 have been eliminated and the summation in the last equation has been taken over all integers j, l, r, s, i 1 , . .…”
Section: Proof Of Theorem 12mentioning
confidence: 99%
“…with y = y (k) and χ = k! (χ (1) ) k . We regard (3.5) as a linear differential equation on a Riemann surface, again.…”
We consider perturbations of integrable systems which may be non-Hamiltonian and give a weak sufficient condition for them to be not meromorphically integrable near resonant tori such that the first integrals and commutative vector fields also depend meromorphically on the small parameter. Moreover, we discuss a relationship of our theory with the subharmonic Melnikov method for time-periodic perturbations of single-degree-of-freedom Hamiltonian systems. We illustrate the theory for three examples: the periodically forced Duffing oscillator, the second-order Kuramoto model and a simple pendulum with a small constant torque. In a companion paper, the theory is applied to prove the nonintegrability of the restricted three-body problem.
“…Using this expression, we write the kth-order VE of (3.2) along the periodic orbit (x, ε) = (x(t), 0) as 1) , y (2) ) + 2 f (1,1) (y (1) , χ (2) ) + 2 f (1,1) (y (1) , χ (2) ) + 2 f (0,2) (χ (1) , χ (2) )…”
Section: Proof Of Theorem 12mentioning
confidence: 99%
“…where such terms as (y(1)) 0 and (χ (1) ) 0 = 1 have been eliminated and the summation in the last equation has been taken over all integers j, l, r, s, i 1 , . .…”
Section: Proof Of Theorem 12mentioning
confidence: 99%
“…with y = y (k) and χ = k! (χ (1) ) k . We regard (3.5) as a linear differential equation on a Riemann surface, again.…”
We consider perturbations of integrable systems which may be non-Hamiltonian and give a weak sufficient condition for them to be not meromorphically integrable near resonant tori such that the first integrals and commutative vector fields also depend meromorphically on the small parameter. Moreover, we discuss a relationship of our theory with the subharmonic Melnikov method for time-periodic perturbations of single-degree-of-freedom Hamiltonian systems. We illustrate the theory for three examples: the periodically forced Duffing oscillator, the second-order Kuramoto model and a simple pendulum with a small constant torque. In a companion paper, the theory is applied to prove the nonintegrability of the restricted three-body problem.
“…In Section 2 we give the key result to reduce the problems of (1.1) and (1.2) to those of (1.6) and (1.7), respectively. In Section 3 we review a necessary part of Acosta-Humánez et al [2] for nonintegrability of planar polynomial vector fields and extend their discussion to give the other key result to analyze (1.6) and (1.7). The proof of Theorem 1.3 is provided in Section 4, and the proofs of Theorems 1.4 and 1.5 are provided in Section 5. whereD ⊂ C × C m is a region containing the m-dimensional y-plane {(0, y) ∈ C × C m | θ ∈ C, y ∈ C m }, and R :D → C,g :D → C m and Θ :D → R are analytic.…”
Section: )mentioning
confidence: 99%
“…Moreover, if deg(κ 1d ) ≤ deg(κ 1n ), then the VE 1 and consequently the LVE k have an irregular singularity at infinity for k ≥ 2. Rational nonintegrability of (3.1) in this situation was extensively discussed in [2].…”
Section: Nonintegrability Of Planar Polynomial Vector Fieldsmentioning
Codimension-two bifurcations are fundamental and interesting phenomena in dynamical systems. Fold-Hopf and double-Hopf bifurcations are the most important among them. We study the unfoldings of these two codimension-two bifurcations, and obtain sufficient conditions for their nonintegrability in the meaning of Bogoyavlenskij. We reduce the problems of the unfoldings to those of planar polynomial vector fields and analyze the nonintegrability of the planar vector fields, based on Ayoul and Zung's version of the Morales-Ramis theory. New useful criteria for nonintegrability of planar polynomial vector fields are also given. The approaches used here are applicable to many problems including circular symmetric systems.
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