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While reading a paper I encountered the following:

Let $(\mathbf{q,p}) \in \mathbb{R}^{2n}$ be canonical coordinates and let $H: \mathbb{R}^{2n} \to \mathbb{R}$ be a smooth function.

The continuous-time Hamiltonian system

$\mathbf{q}_t = + \nabla_p H(q, p)$

$\mathbf{p}_t = - \nabla_q H(q, p)$

preserves exactly the symplectic form $\mathbf{\omega = dp \wedge dq}$, that is $(d/dt)\omega = 0$

Here $\mathbf{p} , \mathbf{q} \in \mathbb{R}^n$

How is $(d/dt)\omega $ even defined? I have seen exterior derivatives of differential forms, but this is evidently something else.

Also, how can we prove that (for the given Hamiltonian system) $(d/dt)\omega = 0$?

Any help will be greatly appreciated.

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  • $\begingroup$ As per their definitions, $\mathbf{p}$ and $\mathbf{q}$ are functions of $t$. Therefore, $\omega$ is a function of $t$, i.e. given a real number $t$ one obtains a form $\omega(t)$. Then $\frac{d\omega}{dt}$ is defined component-wise. $\endgroup$ – florence Jul 4 '16 at 13:46
  • $\begingroup$ So, to clarify, if we have coordinates $x^1, .. x^{2n}$, and $\omega = \sum _{i < j} a_{i,j}(t) dx^i \wedge dx^j$ then $\frac{d\omega}{dt} = \sum _{i < j} \frac{a_{i,j}(t) }{dt} dx^i \wedge dx^j$? $\endgroup$ – Milen Ivanov Jul 4 '16 at 13:54
  • $\begingroup$ I think that in the second Hamilton equation you forgot a minus sign $\endgroup$ – guestDiego Jul 4 '16 at 13:59
  • $\begingroup$ Indeed, thanks :) $\endgroup$ – Milen Ivanov Jul 4 '16 at 14:00
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As mentioned in the comments, you may simply differentiate componentwise.

Alternatively, given any time-dependent $k$-form $\omega_t$ on a manifold $M$, note that at each point $p \in M$, $\omega_t(p)$ may be viewed as a curve $\mathbb{R} \to \bigwedge^k(T_p^*M)$ in a finite-dimensional vector space, defined by $t \mapsto \omega_t(p)$. There is a canonical smooth structure on any finite-dimensional vector space, and so it makes sense to differentiate this curve. Verify that this agrees with the previous definition!

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$\def\L{\mathcal L}$From what you've written there is no dependence of the Hamiltonian on time (indeed a time variable is not introduced at all), so the interpretation in the comments doesn't feel right. Without more context, I would assume that by $(d/dt)\omega$ the author means the Lie derivative $\L_X \omega$ where

$$X = \sum_j \left(\nabla_{p_j} H \frac{\partial}{\partial q^j}-\nabla_{q^j} H \frac{\partial}{\partial p_j}\right)$$ is the Hamiltonian vector field, whose flow gives the time evolution of the system (thus the notation $d/dt$).

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