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Dec 1, 2020 at 23:44 vote accept boink
Dec 1, 2020 at 23:43 vote accept boink
Dec 1, 2020 at 23:44
Dec 1, 2020 at 17:36 comment added Andy Sanders Forgiving historical inaccuracies (and perhaps eliding constants), I would wager it has something to do with the restriction of the (canonical) Liouville one form on $T^{*}\mathbb{R}^{n}$ to the unit co-sphere bundle with respect to the Euclidean metric on $\mathbb{R}^{n}.$
Dec 1, 2020 at 9:13 answer added Marco Golla timeline score: 4
Dec 1, 2020 at 9:03 answer added Thomas Rot timeline score: 4
Dec 1, 2020 at 5:42 comment added Panagiotis Konstantis Like in symplectic geometry, there is a Darboux theorem in contact geometry, which tells you that on a manifold with contact structure there is always a chart such that the given contact structure looks like the standard contact structure on $\mathbb R^n$.
Dec 1, 2020 at 4:56 comment added Deane Yang Given a function $f: \mathbb{R}^n \rightarrow \mathbb{R}$, consider the graph of f and its gradient, $G = \{ (x_1, \partial_1f, \dots, x_n,\partial_nf, f) \}$. The standard contact form $\alpha$ vanishes when restricted to this graph. Conversely, any $n$-dimensional submanifold on which $\alpha$ vanishes but the $n$-form $dx_1 \wedge\cdots\wedge dx_n \ne 0$ at every point is the graph of a function and its gradient. This is how the concept of a contact structure first arose.
Dec 1, 2020 at 4:51 history asked boink CC BY-SA 4.0