Timeline for Coupling constant in electroweak theory
Current License: CC BY-SA 3.0
7 events
| when toggle format | what | by | license | comment | |
|---|---|---|---|---|---|
| Jul 17, 2017 at 12:34 | vote | accept | user31694 | ||
| Jun 1, 2014 at 8:37 | answer | added | Neuneck | timeline score: 9 | |
| Jun 1, 2014 at 8:33 | answer | added | TwoBs | timeline score: 1 | |
| Jun 1, 2014 at 8:24 | comment | added | Anne O'Nyme | You are indeed correct that the $SU(2)_L\times U(1)$ is not a complete unification. This is however achieved when one embed $SU(2)_L\times U(1)$ in a simple Lie Group, for example $SU(5)$. The latter is called the Georgi-Glashow model:en.wikipedia.org/wiki/Georgi%E2%80%93Glashow_model: In this model the standard model gauge groups $SU(3) × SU(2) × U(1)$ are combined into a single simple gauge group $SU(5)$. | |
| S Jun 1, 2014 at 7:42 | history | suggested | 299792458 | CC BY-SA 3.0 |
Symmetry Breaking Tag, and a relevant hyperlink
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| Jun 1, 2014 at 6:44 | review | Suggested edits | |||
| S Jun 1, 2014 at 7:42 | |||||
| Jun 1, 2014 at 6:26 | history | asked | user31694 | CC BY-SA 3.0 |