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| ZP OWER C ORPORATION PAGE OF 352 Z ERO P OINT E NERGY personal power. In the old adage, power corrupts and absolute power corrupts absolutely. Please use it wisely. Notes And References 1. Fora good discussion of the modern quantum mechanical view of the vacuum, see I. JR. Aitchison, "Nothings plenty the vacuum in modern field theory" Contemporary Physics, 26(4), 1985, p. 333-391. See also TD. Lee, Particle Physics and Introduction to Field Theory, Harwood Academic Publishers, New York, 1981 __ particularly Chapter 16, "Vacuum as the source of asymmetry" See Timothy Boyer, "The classical vacuum" Scientific American, Aug. 1985, p. 70; Walter Greiner and Joseph Hamilton, "Is the Vacuum really Empty, American Scientist, Mar.-Apr. 1980, p. 154; Jack S. Greenberg and Walter Greiner, "Search for the sparking of the vacuum" Physics Today, Aug. 1982, p. 24-32; Richard E. Prange and Peter Strance, "The superconducting vacuum, " American Journal of Physics, 52(1), Jan. 1984, p. 19-21; R. Jackiw and JR. Schrieffer, "The decay of the vacuum" Nuclear Physics B, Vol. 190, 1981, p. 944. See Paul Davies, Superforce, Simon and Schuster, 1984 fora layman's overview of modern physics, including the modern view of the vacuum. 2. ET. Whittaker, "On the partial differential equations of mathematical physics" Mathematische Annalen, Vol. 57, 1903, p. 333-355. Since the scalar potential actually consists totally of a set of hidden bidirectional EM waves, then scalar interferometry is possible, and not just an oxymoron as it would seem without considering the inner wave structure of the scalar potential. Two scalar potentials (each of which is a multi-biwave set) can interfere it is just a special kind of multiple wave interferometry between their internal wave compositions. This is a major point of profound impact on physics. Whittaker in fact showed that all classical EM could be replaced by such scalar EM potential interferometry. See ET. Whittaker, "On an expression of the electromagnetic field due to electrons by means of two scalar potential functions" Proceedings of the London Mathematical Society, Series 2, Vol. 1, 1904, p. 367-372. Further, scalar interferometry has been proven today it is called the Aharonov-Bohm Effect. See Y. Aharonov and D. Bohm, "Significance of Electromagnetic Potentials in the Quantum Theory" Physical Review, Second Series, 115(3), Aug. 1, 1959, p. 458-491. For confirmation and discussion, see Bertram Schwarzschild, "Currents in normal-metal rings exhibit Aharonov-Bohm Effect" Physics Today, 39(1), |