Timeline for Showing that the angular momentum operators and Laplace-Runge-Lenz operator together are generators of $SO(4)$
Current License: CC BY-SA 4.0
6 events
| when toggle format | what | by | license | comment | |
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| Jul 30 at 14:13 | comment | added | Cosmas Zachos | Divide both sides by $H (...)$, and then slip the $1/\sqrt H$ s into each entry in the commutator to obtain the D s... | |
| Jul 30 at 7:13 | comment | added | Jonathan Huang | I would like some clarification on what you meant by $H$ can be moved out of their commutators like a constant number. As far as I understand, we have $[A_j, A_k] = i()\varepsilon_{jkl}HL_l$, where $H$ appears on the right hand side only; so are you saying we need ot calculate some "commutator of commutators", which is why the italicised property is important? | |
| Jul 28 at 19:51 | history | edited | Cosmas Zachos | CC BY-SA 4.0 |
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| Jul 27 at 23:05 | history | edited | Cosmas Zachos | CC BY-SA 4.0 |
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| Jul 27 at 19:58 | history | edited | Cosmas Zachos | CC BY-SA 4.0 |
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| Jul 27 at 16:21 | history | answered | Cosmas Zachos | CC BY-SA 4.0 |