Exploring Lepton Annihilation and Hadron Formation in the Standard Model

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The discussion focuses on the differences between electron-positron annihilation and electron-proton interactions within the Standard Model. It highlights that electron and positron are antiparticles, allowing for annihilation, while the proton's additional quantum numbers prevent similar annihilation with an electron, resulting in the formation of hydrogen instead. Conservation laws, particularly related to quantum numbers like flavor and color, play a crucial role in these interactions. The conversation also touches on the nature of forces and symmetries in particle physics, emphasizing that there is no repulsive force preventing electron-proton annihilation, but rather a lack of available states for such a process. Ultimately, the thread illustrates the complexities of particle interactions and the importance of understanding underlying principles in quantum mechanics.
  • #31
When a positron approaches an electron, it first gets captured into atomic states, just like the states that bind the electron to the proton in hydrogen. The positron then gets captured by the electron and annihilated in several nanoseconds. If the mass of the neutron were slightly less than the mass of the proton, then the electron in the hydrogen atom would eventually get absorbed by the proton to produce a neutron and a neutrino. However, the neutron is heavier than the proton, and the neutron decays into a proton, an electron, and a (nearly) massless neutrino. In nuclei, beta (electron)decay is an example of neutron decay. Beta (positron) decay in nuclei is an example of proton decay in nuclei.
There is one additional effect called K capture, in which a proton in a nucleus "captures" an electron in the atomic K shell and becomes a neutron with the emission of a neutrino. This is also called inverse beta decay.
 
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