SearcharxivSearch

arXiv · 2110.14175

Hamilton-Jacobi Equations of Controlled Magnetic Hamiltonian System with Nonholonomic Constraint

Abstract

In order to describe the impact of different geometric structures and constraints for the dynamics of a regular controlled Hamiltonian system, in this paper, we first define a kind of controlled magnetic Hamiltonian (CMH) system, and give a good expression of the dynamical vector field of the CMH system, such that we can describe the magnetic vanishing condition and the CMH-equivalence, and derive precisely the geometric constraint conditions of the magnetic symplectic form for the dynamical vector field of the CMH system, which are called the Type I and Type II of Hamilton-Jacobi equation. Secondly, we prove that the CMH-equivalence for the CMH systems leaves the solutions of corresponding to Hamilton-Jacobi equations invariant, if the associated magnetic Hamiltonian systems are equivalent. Thirdly, we consider the CMH system with nonholonomic constraint, and derive a distributional CMH system, which is determined by a non-degenerate distributional two-form induced from the magnetic symplectic form. Then we drive precisely two types of Hamilton-Jacobi equation for the distributional CMH system. Moreover, we generalize the above results for the nonholonomic reducible CMH system with symmetry, and prove two types of Hamilton-Jacobi theorems for the nonholonomic reduced distributional CMH system. These research works reveal the deeply internal relationships of the magnetic symplectic forms, the nonholonomic constraints, the dynamical vector fields and controls of the CMH systems.

Explore related subjects

Keep this discovery

BibTeXRIS

Hong Wang. 2021-10-27. Hamilton-Jacobi Equations of Controlled Magnetic Hamiltonian System with Nonholonomic Constraint. https://arxiv.org/abs/2110.14175

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Extended Future Tube Conjecture for Unipotent Subgroups

Let $\Omega$ be the Lorentz future cone in $\mathbb{R}^{d+1}$ with respect to the Lorentz product and let $T^M$ be the $M$-fold product of the future tube $T=\mathbb{R}^{d+1}+i\Omega$. The Lorentz group $\mathrm{SO}_0(1,d)$ acts diagonally on $T^M$, and its complexification $\mathrm{SO}(1,d)^\mathbb{C}$ acts on $\mathbb{C}^{(d+1)\times M}$. We prove that the domain $G^\mathbb{C}\cdot T^M$ is a Stein manifold for any connected unipotent subgroup $G$ of $\mathrm{SO}_0(1,d)$.

math.SG

The First Correction Term in the Asymptotic Expansion of Bohr--Sommerfeld Lagrangian States

Let $\Lambda$ be a compact Bohr--Sommerfeld Lagrangian submanifold of a compact K\"ahler manifold equipped with a holomorphic prequantum line bundle. We study the asymptotic expansion of the Lagrangian states associated with $\Lambda$. In particular, we compute explicitly the first nontrivial correction term and show that it is expressed in terms of geometric invariants of the ambient K\"ahler manifold and the Lagrangian submanifold, including their scalar curvatures, the second fundamental form, and the mean curvature. As a consequence, we obtain the corresponding second-order asymptotic formula for the $L^2$-norm of the Lagrangian states.

math.SG

Classification of Legendrian doubles and suspensions

We define a construction of Legendrians inside contact manifolds that arise by doubling an exact Lagrangian filling in the page of an open book decomposition. This can be seen as a generalization of a previous construction by Courte and Ekholm to arbitrary open books. These Legendrians, called Legendrian doubles, are shown to admit regular flexible exact Lagrangian fillings, and they are thus classified up to Legendrian isotopy by classical data. Finally, we show that the Legendrian suspension construction, as defined by Arikan and the author in previous work,-this is a Legendrian contained inside a page of an open book that is obtained by using Seidel's suspension of Lefschetz fibrations- is a Legendrian double.

math.SG