Timeline for Experimental proof for isospin conservation of strong interaction
Current License: CC BY-SA 4.0
17 events
when toggle format | what | by | license | comment | |
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Oct 4, 2019 at 14:57 | vote | accept | avitase | ||
Oct 3, 2019 at 16:33 | answer | added | avitase | timeline score: 0 | |
Sep 29, 2019 at 15:52 | history | edited | Qmechanic♦ | CC BY-SA 4.0 |
No need to explain previous edits
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Sep 29, 2019 at 15:23 | comment | added | Cosmas Zachos | Yes, the EM decay swamps the strong I-violating one which is meant to be even weaker! | |
Sep 29, 2019 at 15:21 | comment | added | Cosmas Zachos | 2nd class currents is a separate, long and subtle story. Basically, Weak currents violate C,P, in predictable and precise ways, so G-parity violations are purely due to I violations. You observe such in the decay cited. Caveat: there is lots of nonsense hidden in the literature on this, however.... In my answer, I got you a clean channel. | |
Sep 29, 2019 at 15:18 | comment | added | avitase | So what you are saying is, that the background $\rho^0 \to 2\pi^0 \gamma$ in $\rho^0 \to 2\pi^0$ is too hard to handle? | |
Sep 29, 2019 at 15:13 | comment | added | Cosmas Zachos | For the ρ, no way to compete with $\Gamma_{10}, ~~~ 2\pi^0 \gamma$. You are looking in the wrong place. | |
Sep 29, 2019 at 15:08 | answer | added | user4552 | timeline score: 0 | |
Sep 29, 2019 at 15:00 | comment | added | avitase | Could you explain what you mean with the $\tau \!\to \eta \pi^0 \nu_\tau$ decay? How does isospin conservation enters here? | |
Sep 29, 2019 at 14:42 | comment | added | avitase | Sorry for the confusion. There was a typo. I wanted to refer to $\rho^0 \! \to 2\pi^0$ instead of $\eta$. You are right, $\eta \!\to 2\pi^0$ is indeed measured. | |
Sep 29, 2019 at 14:40 | history | edited | avitase | CC BY-SA 4.0 |
added 106 characters in body
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Sep 28, 2019 at 19:16 | answer | added | Cosmas Zachos | timeline score: 0 | |
Sep 28, 2019 at 11:45 | comment | added | Cosmas Zachos | Tau to eta pi nu is second class. Don’t be stymied by cutting out weak interactions. Weinberg’s book details such. | |
Sep 28, 2019 at 10:52 | comment | added | avitase | Thanks for your help. I searched the PDG. But I failed to find an upper limit for the $\eta$ decay, as well as branching ratios for the $\Delta$ decays. Could you be a bit more precise and / or point me to a specific PDG page / link? | |
Sep 28, 2019 at 10:49 | history | edited | avitase |
edited tags
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Sep 28, 2019 at 10:48 | comment | added | Cosmas Zachos | Second class current decays are suppressed by dint of isospin/G-parity. Go to the PDG, | |
Sep 28, 2019 at 10:36 | history | asked | avitase | CC BY-SA 4.0 |