Goodbye Quarks: The Onium Theory by Fleming Ray

Author:Fleming, Ray [Fleming, Ray]
Language: eng
Format: azw3, epub
Published: 2020-06-19T16:00:00+00:00

Figure 17-3 A neutron is formed by a quantum electron-positron annihilation-production event when a quantum electron crosses the proton’s potential barrier and is captured.

As discussed before, quantum electron-positron pairs participate in annihilation-production interactions where a free electron annihilates with a quantum positron and the quantum electron becomes free. If the newly freed electron ends up inside a proton’s potential barrier, a neutron will form. In this way it is possible for a free electron to form a neutron without having a large outside source of energy. The energy comes from the quantum field. This is illustrated in Figure 17-3.

Like mass-energy, weak interaction energy is something that arises from quantum field energy and the total energy is conserved by including the quantum field energy.105 Note that Sternglass was able to produce neutrons while accelerating electrons to 35 keV in a hydrogen filled vacuum arc tube. This demonstrated that neutrons can be produced at energies well below 782 keV.106 This is not that unlike deuterium-deuterium fusion which can occur at energies of 10 keV or lower in a Farnsworth fusor while the ideal cross-section energy is greater than 200 keV.

Next we can consider neutron decay as illustrated in Figure 17-4. In this case, a quantum electron-positron particle pair appears in space with its positron within the neutron’s potential barrier. The electron-like component of a neutron then annihilates with the quantum positron turning the neutron into a proton. The quantum electron is left as a free electron outside the proton’s potential barrier.107

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