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Nov 7, 2022 at 3:07 vote accept Dutonic
Nov 7, 2022 at 1:56 answer added ACuriousMind timeline score: 9
Nov 7, 2022 at 1:40 answer added ZeroTheHero timeline score: 2
Nov 7, 2022 at 1:36 history edited Buzz CC BY-SA 4.0
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Nov 7, 2022 at 1:35 answer added Buzz timeline score: 6
Nov 7, 2022 at 0:55 history edited Dutonic CC BY-SA 4.0
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Nov 7, 2022 at 0:42 history edited Qmechanic
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Nov 7, 2022 at 0:35 comment added d_b @Dutonic It's hard to imagine what a proof would be. One argument that you could make is that the angular momentum is the symmetry charge associated with rotational symmetry, so whatever the angular momentum operator is it should be the generator of rotations. But then the whole idea that symmetry charges generate the corresponding symmetries is really just a postulate that needs to be verified experimentally... like the whole rest of the theoretical apparatus.
Nov 7, 2022 at 0:33 comment added Ghoster You seem to have the misconception that physical theories can ever be proved. They can’t.
Nov 7, 2022 at 0:33 answer added don't train ai on me timeline score: -2
Nov 7, 2022 at 0:16 comment added Dutonic @Ghoster To clarify, the purpose of this question is to gain an understanding of the theoretical foundations for why we make this assumption. Are we postulating this relationship between quantum operators and their classical counterparts, or is there a proof behind it? I'm perfectly aware of how experimentalists check the accuracy of theories...
Nov 7, 2022 at 0:02 comment added Ghoster By assuming it and then testing whether theoretical predictions following from that assumption match observation… the same way we become confident in any theoretical idea.
Nov 6, 2022 at 23:55 comment added Dutonic @basics Obviously L = r x p in classical mechanics. The question is about how we can definitively demonstrate that this definition holds for quantum operators
Nov 6, 2022 at 23:52 comment added basics it's like the definition of the angular momentum in classical mechanics
Nov 6, 2022 at 23:44 history asked Dutonic CC BY-SA 4.0