English

Polynomial dynamical systems and Korteweg--de Vries equation

Dynamical Systems 2018-03-13 v1 Mathematical Physics math.MP

Abstract

In this work we explicitly construct polynomial vector fields Lk,  k=0,1,2,3,4,6\mathcal{L}_k,\;k=0,1,2,3,4,6 on the complex linear space C6\mathbb{C}^6 with coordinates X=(x2,x3,x4)X=(x_2,x_3,x_4) and Z=(z4,z5,z6)Z=(z_4,z_5,z_6). The fields Lk\mathcal{L}_k are linearly independent outside their discriminant variety ΔC6\Delta \subset \mathbb{C}^6 and tangent to this variety. We describe a polynomial Lie algebra of the fields Lk\mathcal{L}_k and the structure of the polynomial ring C[X,Z]\mathbb{C}[X, Z] as a graded module with two generators x2x_2 and z4z_4 over this algebra. The fields L1\mathcal{L}_1 and L3\mathcal{L}_3 commute. Any polynomial P(X,Z)C[X,Z]P(X,Z) \in \mathbb{C}[X, Z] determines a hyperelliptic function P(X,Z)(u1,u3)P(X,Z)(u_1, u_3) of genus 22, where u1u_1 and u3u_3 are coordinates of trajectories of the fields L1\mathcal{L}_1 and L3\mathcal{L}_3. The function 2x2(u1,u3)2 x_2(u_1, u_3) is a 2-zone solution of the KdV hierarchy and u1z4(u1,u3)=u3x2(u1,u3)\frac{\partial}{\partial u_1}z_4(u_1, u_3)=\frac{\partial}{\partial u_3}x_2(u_1, u_3).

Keywords

Cite

@article{arxiv.1605.04061,
  title  = {Polynomial dynamical systems and Korteweg--de Vries equation},
  author = {Victor M. Buchstaber},
  journal= {arXiv preprint arXiv:1605.04061},
  year   = {2018}
}
R2 v1 2026-06-22T13:59:54.656Z