What is a Liouville Isomorphism in the Context of Symplectization?

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In summary, a Liouville domain is a compact manifold with boundary that has a symplectic form and a one-form defined on the boundary that satisfies certain conditions. A Liouville isomorphism is a diffeomorphism between the symplectizations of two Liouville domains that preserves the one-form up to an exact form. This definition is used to generate symplectomorphisms of exact symplectic manifolds and the collaring construction used in the definition is considered to be canonical.
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Kreizhn
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I shall use Seidel's definition of a Liouville domain; in particular, a Liouville domain is a compact manifold [itex] M [/itex] with boundary together with a one-form [itex] \theta \in \Omega^1(M) [/itex] such that [itex] \omega = d\theta [/itex] is a symplectic form and the vector field Z defined by [itex] \iota_Z \omega = \theta [/itex] is always strictly outward pointing along [itex] \partial M[/itex]. Let [itex] \alpha = \theta_{\partial M} [/itex] be the contact form on the boundary.

Let [itex] \hat M [/itex] denote the symplectization of [itex] M [/itex] given by the natural collaring induced by the flow of Z. Namely, we attach an infinite cone to the boundary [itex] \partial M [/itex] and extend [itex] \theta [/itex] to [itex] e^r \alpha [/itex], and Z to [itex] \frac\partial{\partial r} [/itex] where [itex] r [/itex] is the [itex] \mathbb (-\infty,0] [/itex] coordinate of the symplectization.

Now a Liouville isomorphism of two Liouville domains [itex] M_1, M_2 [/itex] is defined to be a diffeomorphism on the symplectizations [itex] \hat M_1,\hat M_2 [/itex] such that [itex] \phi^*\theta_2 = \theta_1 + dg [/itex] where g is a compactly supported smooth function.

First question: Why do we define a Liouville isomorphism at the level of symplectization? Is the collaring argument really so canonical that it is essentially inherent to the definition of a Liouville domain?

Second question: Why do we only require that the one-form is preserved up to an exact form? I have heard an argument that demanding that the pullback preserve the form completely is too restrictive. Perhaps this could be elaborated upon. Furthermore, why do we need to the form to be exact? It seems to me that any argument about the preservation of structure could be done by using a compactly supported closed form, hence generalizing the space of Liouville isomorphisms even further.
 
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Well, I am not aware of the context of these definitions, but apparently, the reason for the definition of a Liouville iso is to generate symplectomorphisms of exact symplectic manifolds that are of the type "symplectification of Liouville domains". Indeed, take the exterior derivative of the defining formula for phi. So this class of symplectomorphism is in a sense simpler to identify than a general symplectomorphism since instead of asking for diffeos that preserve a two-form, we ask for those that preserve a 1-form... and not even that, we need only ask for those that preserve a 1-form up to an exact differential! Hopefully, this answers your second question?

As for question 1, yes the collaring construction is canonical. And it seems to me that a Liouville isomorphism between M1 and M2 has little to do with maps M1-->M2. Indeed, it is defined as a diffeomorphism btw the symplectifications which need not restrict to a diffeo M1-->M2! Mmmh, but I guess what you're really asking is if the map [itex]M\mapsto \hat{M}[/itex] is injective (up to symplectomorphism).
 

FAQ: What is a Liouville Isomorphism in the Context of Symplectization?

What is Liouville isomorphism?

Liouville isomorphism is a mathematical concept that relates the symmetries of a Hamiltonian system to the solutions of its equations of motion. It states that two Hamiltonian systems with the same symmetry properties are isomorphic and therefore share the same solutions.

Why is Liouville isomorphism important?

Liouville isomorphism is important because it allows us to simplify complex Hamiltonian systems by identifying and exploiting their symmetry properties. This can lead to significant reductions in computational effort and provide deeper insights into the behavior of the system.

How is Liouville isomorphism related to Hamiltonian mechanics?

Liouville isomorphism is a fundamental concept in Hamiltonian mechanics. It is based on the notion that symmetries of a Hamiltonian system correspond to conserved quantities, which are crucial in understanding the dynamics of the system.

Can Liouville isomorphism be applied to classical and quantum systems?

Yes, Liouville isomorphism can be applied to both classical and quantum systems. In classical mechanics, it relates symmetries of the Hamiltonian to conserved quantities, while in quantum mechanics, it relates unitary transformations of the Hamiltonian to symmetries of the system.

How is Liouville isomorphism used in practical applications?

Liouville isomorphism is used in a variety of practical applications, including celestial mechanics, molecular dynamics simulations, and quantum information processing. It allows for the simplification and optimization of complex systems and can lead to more efficient and accurate calculations.

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