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Jun 23, 2020 at 15:35 comment added Charles Hudgins Wish I could upvote this answer more than once. Too many leave undergrad without a good understanding of Noether's theorem and related concepts.
Nov 6, 2015 at 0:36 comment added Robin Ekman Consider Hamiltonian mechanics in canonical coordinates $(x,p)$. Then translations map $(x,p) \mapsto (x+a,p)$. Clearly the vector field that generates this is $\partial/\partial q$. But in canonical coordinates the symplectic form is $dq\wedge dp$, so $\partial/\partial q \mapsto dp$. Thus while it's strictly speaking $\partial/\partial q$ that is the generator of translations, we can associate it with the coordinate p in this way.
Nov 6, 2015 at 0:25 comment added Robin Ekman @fffred I think the analogy is somewhat a "deep" insight that you get after much reading from several sources, but I would recommend Armold's Mathematical Methods of Classical Mechanics, because he talks a lot about the Lie algebra structure in Hamiltonian mechanics.
Nov 6, 2015 at 0:22 comment added fffred Could you explain a bit more? or point to places where to read about it? I have some trouble finding it.
Nov 6, 2015 at 0:21 comment added Robin Ekman The concept of generator of translations applies also to classical mechanics in the Hamiltonian formulation. The difference is that classically the generator is a vector field, whereas the quantum generator is an operator. But they are analogous because vector fields and operators are both Lie algebras.
Nov 6, 2015 at 0:20 comment added fffred I'm confused: definition of momentum as generator of translations appears, to my knowledge, in quantum mechanics. Is there a way to describe the same thing using only special relativity? without waves?
Nov 5, 2015 at 23:24 history edited Robin Ekman CC BY-SA 3.0
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Nov 5, 2015 at 23:16 history answered Robin Ekman CC BY-SA 3.0