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Stream: deprecated: thermodynamics

Topic: symplectic geometry and Dirac structures


view this post on Zulip Owen Lynch (Feb 08 2022 at 04:06):

If XX is a symplectic manifold, there is a natural dirac structure on TX×XTXTX \times_X T^\ast X, and I will demonstrate it here.

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:09):

The Dirac structure is the graph of the map TXTXT^\ast X \to T X that sends a cotangent vector ϕTxX\phi \in T^\ast_x X to the tangent vector vv such that ω(,v)=ϕ\omega(-,v) = \phi.

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:10):

Or really, I suppose it is the other way around.

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:11):

It is the graph of the map TXTXT X \to T^\ast X that sends the tangent vector vTxXv \in T_x X to the cotangent vector ω(,v)\omega(-,v).

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:12):

This is a Dirac structure because v,ω(,v)=ω(v,v)=0\langle v, \omega(-,v) \rangle = \omega(v,v) = 0.

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:13):

And it is of dimension nn, where dim(TxX×TxX)=2n\dim(T_x X \times T_x^\ast X) = 2n

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:16):

We can think of this Dirac structure as giving a port-Hamiltonian system with no ports, as it is a relation between TX×XTXTX \times_X T^\ast X and R0×(R0)\mathbb{R}^0 \times (\mathbb{R}^0)^\ast.

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:19):

The rules of time-evolution for a port-Hamiltonian system say that (x(t),dHx(t))(x'(t), dH_{x(t)}) must be an element of the Dirac structure for all tt, where x:IXx : I \to X is a differentiable curve, H:XRH : X \to \mathbb{R} is the Hamiltonian, and dHx(t)Tx(t)XdH_{x(t)} \in T^\ast_{x(t)} X is the differential of HH at point x(t)x(t).

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:20):

We can see that this is precisely requiring ω(,x(t))=dHx(t)\omega(-,x'(t)) = dH_{x(t)}, which is Hamilton's equation.

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:22):

Thus, we should not think of the bilinear symmetric 2-form of signature (n,n)(n,n) as analogous to the symplectic form

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:22):

The Dirac structure itself is analogous to the symplectic form.

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:23):

Each symplectic form produces a Dirac structure, though not all Dirac structures may arise from symplectic forms

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:26):

In fact, there are Dirac structures which cannot arise from symplectic forms.

view this post on Zulip Owen Lynch (Feb 08 2022 at 04:27):

Because there are Dirac structures even when XX is odd-dimensional.

view this post on Zulip John Baez (Feb 08 2022 at 04:37):

Okay, great. So it sounds like from this point of view we should think of Dirac operators as generalized symplectic structures. That sounds familiar to me.

view this post on Zulip John Baez (Feb 08 2022 at 04:38):

Does a Poisson structure on XX also give a Dirac structure on TX×XTXTX \times_X T^\ast X?

view this post on Zulip John Baez (Feb 08 2022 at 04:40):

A Poisson structure on XX is a bivector field, i.e. a section Π\Pi of the second exterior power Λ2TX\Lambda^2 TX, such that if we define

{f,g}=Π(dfdg)\{f,g\} = \Pi(df \wedge dg)

for smooth real-valued functions f,gf,g on XX, then {f,g}\{f,g\} obeys all the usual identities that Poisson brackets should.

view this post on Zulip John Baez (Feb 08 2022 at 04:42):

Poisson structures are strictly more general than symplectic structures: a symplectic structure ω\omega on XX sets up a vector bundle isomorphism TXTXTX \cong T^\ast X and we can use this to turn ωΛ2TX\omega \in \Lambda^2 T^\ast X into a Poisson structure ΠΛ2TX\Pi \in \Lambda^2 TX.

Unlike symplectic structures, Poisson structures exist on odd-dimensional manifolds.

view this post on Zulip Owen Lynch (Feb 08 2022 at 21:48):

John Baez said:

Okay, great. So it sounds like from this point of view we should think of Dirac operators as generalized symplectic structures. That sounds familiar to me.

You mean Dirac structures?

view this post on Zulip Owen Lynch (Feb 08 2022 at 21:50):

I'll think about the Poisson structure question

view this post on Zulip Owen Lynch (Feb 08 2022 at 21:52):

So, the Poisson structure gives a map TXTXT^\ast X \to T^{\ast\ast} X, sending ϕ\phi to Π(ϕ)\Pi(\phi \wedge -).

view this post on Zulip Owen Lynch (Feb 08 2022 at 21:53):

Thus, it defines a map TXTXT^\ast X \to T X

view this post on Zulip Owen Lynch (Feb 08 2022 at 21:54):

And the graph of this map is indeed a Dirac structure, as Π(ϕϕ)=0\Pi(\phi \wedge \phi) = 0.

view this post on Zulip John Baez (Feb 08 2022 at 21:59):

Owen Lynch said:

John Baez said:

Okay, great. So it sounds like from this point of view we should think of Dirac operators as generalized symplectic structures. That sounds familiar to me.

You mean Dirac structures?

Yes. Right now I'm writing a paper on the hydrogen atom and the Dirac operator. :smirk:

view this post on Zulip John Baez (Feb 08 2022 at 22:02):

Owen Lynch said:

And the graph of this map is indeed a Dirac structure, as Π(ϕϕ)=0\Pi(\phi \wedge \phi) = 0.

Okay, that was easy! Nice!

Actually I think there must be some 'integrability condition' in the definition of Dirac structure - some differential equation that has to hold. This is certainly true for the definition of symplectic structure (dω=0d \omega = 0) and Poisson structure ([Π,Π]=0[\Pi, \Pi] = 0, where the bracket is the Schouten bracket, the generalization of the Lie bracket on vector fields to multivector fields). So, there should be some exercise where you prove that [Π,Π]=0[\Pi, \Pi] = 0 implies the integrability condition for the Dirac structure (whatever that is).

view this post on Zulip John Baez (Feb 08 2022 at 22:02):

Someone must have done this already.

view this post on Zulip Owen Lynch (Feb 09 2022 at 00:33):

Yeah, that sounds about right, I'll look into it

view this post on Zulip Owen Lynch (Feb 09 2022 at 00:33):

I should do both of these constructions out in more detail

view this post on Zulip John Baez (Feb 09 2022 at 02:18):

This paper says:

As we shall see shortly, in geometric mechanics, almost Dirac structures provide a simultaneous generalization of both two-forms (not necessarily closed, and possibly degenerate) as well as almost Poisson structures (that is brackets that need not satisfy the Jacobi identity). A Dirac structure, which corresponds in geometric mechanics to assuming the two-form is closed or to assuming Jacobi’s identity for the Poisson tensor, is one that satisfies...

[some differential equation]

view this post on Zulip John Baez (Feb 09 2022 at 03:06):

A possibly degenerate closed 2-form is called a presymplectic structure. You can't turn all presymplectic structures into Poisson structures, and you can't turn all Poisson structures into presymplectic structures. The intersection of the two are the symplectic structures. The union of the two is included in the Dirac structures.

view this post on Zulip John Baez (Feb 09 2022 at 03:07):

This makes me happier about Dirac structures, since I've messed with Poisson structures a lot and presymplectic structures a little too.