Timeline for Commutator generating transformations
Current License: CC BY-SA 4.0
6 events
| when toggle format | what | by | license | comment | |
|---|---|---|---|---|---|
| Jan 2, 2019 at 14:56 | vote | accept | Luthien | ||
| Jan 2, 2019 at 9:22 | answer | added | Qmechanic♦ | timeline score: 0 | |
| Jan 2, 2019 at 8:46 | history | edited | Qmechanic♦ | CC BY-SA 4.0 |
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| Jan 2, 2019 at 8:35 | answer | added | InertialObserver | timeline score: 1 | |
| Jan 1, 2019 at 22:53 | comment | added | Cosmas Zachos | This is just the physicist's convention of speaking: The composition of two symmetry transformations generates a trivial "sum part", but, significantly, a further commutator part. Think of the beginning of the CBH expansion and the form of the relevant exponent. Your question might equally well apply to ordinary rotations about different axes, and the composition of the relevant generators. | |
| Jan 1, 2019 at 22:45 | history | asked | Luthien | CC BY-SA 4.0 |