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broken symmetry
Broken Symmetry of the Dipole
Last Updated on Sat, 19 Dec 2020 | Energy from Vacuum
To recap from Chapters 1 and 2: In 1956, Lee and Yang {187} strongly predicted broken symmetry in physics, suggesting experiments to detect it in the weak interaction. In early 1957, Wu et al. {188} experimentally demonstrated broken symmetry, thus furnishing the experimental substantiation of broken parity in the weak interaction. The emergence of broken symmetry was such a dramatic change to the view of physics, that in December of the same year, 1957, Lee and Yang were awarded the Nobel Prize.
One of the asymmetries shown by Lee et al. is the asymmetry of opposite charges. That means that a dipole, which consists of slightly separated opposite charges, exhibits broken symmetry in the seething vacuum virtual particle flux. In short, a dipole — any dipole or dipolarity — must absorb or receive virtual photon energy from the active vacuum, integrate at least some of it to observable state, and re-radiate that integrated EM energy in observable form in 3-space.
We stress: The ends of a dipole, being oppositely charged, exhibit broken symmetry. An 'isolated' charge, considered with its clustering virtual charges of opposite sign, is a set ofcomposite dipoles and also exhibits broken symmetry.
Electricity Flow Experiment
Figure 3-1 The source dipole experiment, demonstrating continuous energy flow.
https://www.freeenergyplanet.biz/energy-from-vacuum/broken-symmetry-of-the-dipole.html
Wu experiment
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Chien-Shiung Wu, after whom the Wu experiment is named, designed the experiment and led the team that carried out the test of the conservation of parity in 1956.
The Wu experiment was a nuclear physics experiment conducted in 1956 by the Chinese American physicist Chien-Shiung Wu in collaboration with the Low Temperature Group of the US National Bureau of Standards.[1] The experiment's purpose was to establish whether or not conservation of parity (P-conservation), which was previously established in the electromagnetic and strong interactions, also applied to weak interactions. If P-conservation were true, a mirrored version of the world (where left is right and right is left) would behave as the mirror image of the current world. If P-conservation were violated, then it would be possible to distinguish between a mirrored version of the world and the mirror image of the current world.
https://en.wikipedia.org/wiki/Wu_experiment
Broken Symmetry
For the open-minded reader, let me explain what broken symmetry means, and what the broken symmetry of a dipole means with respect to powering any dipolar EM circuit.
The strong prediction of broken symmetry by Lee and Yang and its experimental proof by Wu et al. in 1957, initiated a great revolution across physics and won a nearly instant Nobel Prize in December 1957 for Lee and Yang.
One of the broken symmetries proven by Wu et al. and published in 1957 is the broken symmetry of opposite charges, as on the ends of a dipole.
That asymmetry is used by charges and dipoles for extracting and pouring out Electromagnetic energy from the vacuum, yet not one current Electrical Engineering or classical electromagnetics textbook mentions the energy implications of dipolar asymmetry. Nor do they mention that every charge and dipole freely pours out real observable EM energy continuously, with no observable energy input.
www.cheniere.org/references/brokensymmetry.htm