Research article

On the reducibility of a class of almost-periodic linear Hamiltonian systems and its application in Schrödinger equation

  • Received: 27 October 2022 Revised: 26 December 2022 Accepted: 02 January 2023 Published: 16 January 2023
  • MSC : 37K55, 70K40

  • In the present paper, we focus on the reducibility of an almost-periodic linear Hamiltonian system

    $ \frac{dX}{dt} = J[A+\varepsilon Q(t)]X, X\in \mathbb{R}^{2d} , $

    where $ J $ is an anti-symmetric symplectic matrix, $ A $ is a symmetric matrix, $ Q(t) $ is an analytic almost-periodic matrix with respect to $ t $, and $ \varepsilon $ is a parameter which is sufficiently small. Using some non-resonant and non-degeneracy conditions, rapidly convergent methods prove that, for most sufficiently small $ \varepsilon $, the Hamiltonian system is reducible to a constant coefficients Hamiltonian system through an almost-periodic symplectic transformation with similar frequencies as $ Q(t) $. At the end, an application to Schrödinger equation is given.

    Citation: Muhammad Afzal, Tariq Ismaeel, Azhar Iqbal Kashif Butt, Zahid Farooq, Riaz Ahmad, Ilyas Khan. On the reducibility of a class of almost-periodic linear Hamiltonian systems and its application in Schrödinger equation[J]. AIMS Mathematics, 2023, 8(3): 7471-7489. doi: 10.3934/math.2023375

    Related Papers:

  • In the present paper, we focus on the reducibility of an almost-periodic linear Hamiltonian system

    $ \frac{dX}{dt} = J[A+\varepsilon Q(t)]X, X\in \mathbb{R}^{2d} , $

    where $ J $ is an anti-symmetric symplectic matrix, $ A $ is a symmetric matrix, $ Q(t) $ is an analytic almost-periodic matrix with respect to $ t $, and $ \varepsilon $ is a parameter which is sufficiently small. Using some non-resonant and non-degeneracy conditions, rapidly convergent methods prove that, for most sufficiently small $ \varepsilon $, the Hamiltonian system is reducible to a constant coefficients Hamiltonian system through an almost-periodic symplectic transformation with similar frequencies as $ Q(t) $. At the end, an application to Schrödinger equation is given.



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