Editing 2351: Standard Model Changes
Warning: You are not logged in. Your IP address will be publicly visible if you make any edits. If you log in or create an account, your edits will be attributed to your username, along with other benefits.
The edit can be undone.
Please check the comparison below to verify that this is what you want to do, and then save the changes below to finish undoing the edit.
Latest revision | Your text | ||
Line 70: | Line 70: | ||
| Muon || µ || {{w|Muon}} || µ || No change. | | Muon || µ || {{w|Muon}} || µ || No change. | ||
|- | |- | ||
− | | <span style="color:#e31f22">(no one needs Tau | + | | <span style="color:#e31f22">(no one needs Tau lepstons)</span> || (none) || {{w|Tau (particle)|Tau lepton}} || τ || The tau lepton is a lepton with average lifetime much shorter than the electron or the muon. Randall apparently considers this particle redundant and states "No one needs tau leptons". |
|- | |- | ||
| <span style="color:#e31f22">Strange</span> boson || <span style="color:#e31f22">S</span> || {{w|Z boson}} || Z || The Z boson is one of two particles (three, counting the W boson's different charges) that mediate the {{w|weak force}}, named for having '''z'''ero charge. Randall suggests the strange quark's name would be better suited for this particle. | | <span style="color:#e31f22">Strange</span> boson || <span style="color:#e31f22">S</span> || {{w|Z boson}} || Z || The Z boson is one of two particles (three, counting the W boson's different charges) that mediate the {{w|weak force}}, named for having '''z'''ero charge. Randall suggests the strange quark's name would be better suited for this particle. |