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Contact geometry in infinite dimensions

Fraser Aidan Kelvin Sanders

TL;DR

The paper develops a coherent framework for infinite-dimensional contact geometry by defining weakly contact structures on manifolds modelled by convenient spaces, thereby extending dissipation-compatible Hamiltonian mechanics beyond finite dimensions. It provides a thorough background, introduces multiple equivalent characterisations (including a generalized De Rham-style flat map $\flat$) and proves a key property $\ η \wedge (dη)^k \neq 0$ for all $k$, which supports a Pfaffian-type theory in the infinite-dimensional setting. It then constructs concrete infinite-dimensional contact manifolds (via products and jet-bundle methods), derives Hamiltonian dynamics on Fréchet spaces, and presents explicit examples such as a damped oscillator and a damped wave equation with a source term, using both cosymplectic and cocontract structures to model time dependence and dissipation. The work culminates with cosymplectic and cocontact generalisations, including a Darboux-type result and explicit wave-equation-with-source formulations, thereby providing mathematical tools to study dissipative PDEs and time-dependent Hamiltonian systems in infinite dimensions with potential physical applications.

Abstract

We generalise the theories of cosymplectic, contact, and cocontact manifolds to the infinite-dimensional setting and calculate model examples of time-dependent and dissipative Hamiltonian systems.

Contact geometry in infinite dimensions

TL;DR

The paper develops a coherent framework for infinite-dimensional contact geometry by defining weakly contact structures on manifolds modelled by convenient spaces, thereby extending dissipation-compatible Hamiltonian mechanics beyond finite dimensions. It provides a thorough background, introduces multiple equivalent characterisations (including a generalized De Rham-style flat map ) and proves a key property for all , which supports a Pfaffian-type theory in the infinite-dimensional setting. It then constructs concrete infinite-dimensional contact manifolds (via products and jet-bundle methods), derives Hamiltonian dynamics on Fréchet spaces, and presents explicit examples such as a damped oscillator and a damped wave equation with a source term, using both cosymplectic and cocontract structures to model time dependence and dissipation. The work culminates with cosymplectic and cocontact generalisations, including a Darboux-type result and explicit wave-equation-with-source formulations, thereby providing mathematical tools to study dissipative PDEs and time-dependent Hamiltonian systems in infinite dimensions with potential physical applications.

Abstract

We generalise the theories of cosymplectic, contact, and cocontact manifolds to the infinite-dimensional setting and calculate model examples of time-dependent and dissipative Hamiltonian systems.

Paper Structure

This paper contains 25 sections, 16 theorems, 143 equations, 1 figure.

Key Result

Theorem 3.2

Let $M$ be an infinite-dimensional manifold, and $\eta\in \Omega^1(M)$ be a 1-form such that $d\eta$ is degenerate (has non-zero kernel). We define the horizontal and vertical distributions (subbundles of $TM$) as $\mathcal{H}:= \ker \eta$ and $\mathcal{V}:= \ker d \eta = \ker (v \mapsto d\eta(v,-))

Figures (1)

  • Figure :

Theorems & Definitions (75)

  • Definition 2.1: TVS and lcTVS
  • Definition 2.2: smooth maps
  • Definition 2.3: Convenient vector space
  • Definition 2.4: seminorm
  • Definition 2.5: Fréchet space
  • Definition 2.6: Banach space
  • Definition 2.7: Manifold
  • Definition 2.8
  • Definition 2.9: Kinematic tangent bundle
  • Definition 2.10: Kinematic cotangent bundle
  • ...and 65 more