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Almost conservation of the harmonic actions for fully discretized nonlinear Klein--Gordon equations at low regularity

Charbella Abou Khalil, Joackim Bernier

TL;DR

This work treats the nonlinear Klein–Gordon equation on the circle as a nearly integrable Hamiltonian system and proves that, under a CFL-compatible fully discretized scheme with a mollified impulse time integrator, the low harmonic actions remain almost conserved for long times when the initial data are small in the energy space. The authors develop a backward error analysis to construct a modified Hamiltonian $H_h$ that closely tracks the numerical flow and then put $H_h$ into a partial Birkhoff normal form, facilitated by a strong non-resonance property of the discretized frequencies. From this, they derive almost invariance of the modified harmonic actions and, via a priori energy control, almost preservation of the low actions for times $nh\le\varepsilon^{-r}$. The approach extends prior high-regularity results to low regularity, aligns with numerical observations, and offers a robust framework potentially applicable to other dispersive PDE discretizations.

Abstract

Close to the origin, the nonlinear Klein--Gordon equations on the circle are nearly integrable Hamiltonian systems which have infinitely many almost conserved quantities called harmonic actions or super-actions. We prove that, at low regularity and with a CFL number of size 1, this property is preserved if we discretize the nonlinear Klein--Gordon equations with the symplectic mollified impulse methods. This extends previous results of D. Cohen, E. Hairer and C. Lubich to non-smooth solutions.

Almost conservation of the harmonic actions for fully discretized nonlinear Klein--Gordon equations at low regularity

TL;DR

This work treats the nonlinear Klein–Gordon equation on the circle as a nearly integrable Hamiltonian system and proves that, under a CFL-compatible fully discretized scheme with a mollified impulse time integrator, the low harmonic actions remain almost conserved for long times when the initial data are small in the energy space. The authors develop a backward error analysis to construct a modified Hamiltonian that closely tracks the numerical flow and then put into a partial Birkhoff normal form, facilitated by a strong non-resonance property of the discretized frequencies. From this, they derive almost invariance of the modified harmonic actions and, via a priori energy control, almost preservation of the low actions for times . The approach extends prior high-regularity results to low regularity, aligns with numerical observations, and offers a robust framework potentially applicable to other dispersive PDE discretizations.

Abstract

Close to the origin, the nonlinear Klein--Gordon equations on the circle are nearly integrable Hamiltonian systems which have infinitely many almost conserved quantities called harmonic actions or super-actions. We prove that, at low regularity and with a CFL number of size 1, this property is preserved if we discretize the nonlinear Klein--Gordon equations with the symplectic mollified impulse methods. This extends previous results of D. Cohen, E. Hairer and C. Lubich to non-smooth solutions.
Paper Structure (24 sections, 25 theorems, 252 equations, 1 figure)

This paper contains 24 sections, 25 theorems, 252 equations, 1 figure.

Key Result

Theorem 1.1

For all $r\geq 1$, there exists $\beta_r \geq 1$, such that for almost all $\rho >0$, all $\delta>0$, all $K\geq 1$ and all $h>0$ satisfying there exists $\varepsilon_0(r,\rho)>0$ depending only on $r$ and $\rho$ such that if $(q^n,p^n)_{n\geq 0}$ is a sequence of real-valued functions on $\mathbb{T}_K$ solution of the fully discretized nonlinear Klein--Gordon equation eq:KG_fd and whose initial

Figures (1)

  • Figure 1: Evolution of the logarithm of the super actions $\log_{10} J_k(q^n,p^n)$ for different regularity exponents $s_0$ and index ranges $k$ and for times $hn\leq T=4000$.

Theorems & Definitions (58)

  • Theorem 1.1
  • Definition 2.1: Poisson bracket
  • Remark 2.2
  • Definition 2.3: Adjoint representation $\mathrm{ad}$
  • Definition 2.4: Symplectic Map
  • Definition 2.5: Momentum $\mathcal{M}(j,\sigma)$
  • Definition 2.6
  • Definition 2.7
  • Lemma 2.8
  • proof
  • ...and 48 more