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Linear systems, determinants and solutions of the Kadomtsev-Petviashvili equation

Gordon Blower, Simon J. Malham

TL;DR

This work connects Kadomtsev–Petviashvili equation solutions with Fredholm determinants of Hankel operators built from linear-system impulse responses. It develops a Lyapunov-based $R_x$ framework in which $\tau(x)=\det(I+R_x)$ yields KP potentials via Gelfand–Levitan–Marchenko-type relations, and embeds this in Pöppe's semi-additive operator theory with a Fedosov-product differential ring to enable efficient tau-function computation. It also provides a robust operator-theoretic foundation through spectral theory for cosine families, allowing a non-self-adjoint extension of the Gelfand–Levitan approach. Numerically, the approach underpins determinant-based and GLM-based schemes (Clenshaw–Curtis, Nyström methods) for computing KP solutions, including two-soliton scenarios. The results advance integrable-systems practice by unifying tau-function formalism, differential rings, and operator-spectral methods for explicit KP solutions.

Abstract

Let $(-A,B,C)$ be a linear system in continuous time $t>0$ with input and output space ${\mathbb C}$ and state space $H$. The scattering (or impulse response) functions $φ_{(x)}(t)=Ce^{-(t+2x)A}B$ determines a Hankel integral operator $Γ_{φ_{(x)}}$; if $Γ_{φ_{(x)}}$ is trace class, then the Fredholm determinant $τ(x)=\det (I+Γ_{φ_{(x)}})$ determines the tau function of $(-A,B,C)$. The paper establishes properties of algebras including $R_x = \int_x^\infty e^{-tA}BCe^{-tA}\,dt$ on $H$, and obtains solutions of the Kadomtsev-Petviashvili PDE. Pöppe's semi-additive operators are identified with orbits of a shift action on integral kernels, and Pöppe's bracket operation is expressed in terms of the Fedosov product. The paper shows that the Fredholm determinant $\det (I+R_x)$ gives an effective method for numerical computation of solutions of $KP$.

Linear systems, determinants and solutions of the Kadomtsev-Petviashvili equation

TL;DR

This work connects Kadomtsev–Petviashvili equation solutions with Fredholm determinants of Hankel operators built from linear-system impulse responses. It develops a Lyapunov-based framework in which yields KP potentials via Gelfand–Levitan–Marchenko-type relations, and embeds this in Pöppe's semi-additive operator theory with a Fedosov-product differential ring to enable efficient tau-function computation. It also provides a robust operator-theoretic foundation through spectral theory for cosine families, allowing a non-self-adjoint extension of the Gelfand–Levitan approach. Numerically, the approach underpins determinant-based and GLM-based schemes (Clenshaw–Curtis, Nyström methods) for computing KP solutions, including two-soliton scenarios. The results advance integrable-systems practice by unifying tau-function formalism, differential rings, and operator-spectral methods for explicit KP solutions.

Abstract

Let be a linear system in continuous time with input and output space and state space . The scattering (or impulse response) functions determines a Hankel integral operator ; if is trace class, then the Fredholm determinant determines the tau function of . The paper establishes properties of algebras including on , and obtains solutions of the Kadomtsev-Petviashvili PDE. Pöppe's semi-additive operators are identified with orbits of a shift action on integral kernels, and Pöppe's bracket operation is expressed in terms of the Fedosov product. The paper shows that the Fredholm determinant gives an effective method for numerical computation of solutions of .

Paper Structure

This paper contains 3 sections, 5 theorems, 27 equations.

Key Result

Lemma 2.1

For a linear map $\partial :\mathcal{L}\rightarrow\mathcal{L}$ with $\partial (1)=0$, the following are equivalent:

Theorems & Definitions (17)

  • Lemma 2.1
  • proof
  • Proposition 2.2
  • proof
  • Definition 2.3
  • Theorem 2.4
  • proof
  • Example 2.5
  • Remark 2.6
  • Definition 2.7
  • ...and 7 more