496 lines
30 KiB
Plaintext
496 lines
30 KiB
Plaintext
![]() |
|
|||
|
|
|||
|
(word processor parameters LM=8, RM=75, TM=2, BM=2)
|
|||
|
Taken from KeelyNet BBS (214) 324-3501
|
|||
|
Sponsored by Vangard Sciences
|
|||
|
PO BOX 1031
|
|||
|
Mesquite, TX 75150
|
|||
|
|
|||
|
There are ABSOLUTELY NO RESTRICTIONS
|
|||
|
on duplicating, publishing or distributing the
|
|||
|
files on KeelyNet except where noted!
|
|||
|
|
|||
|
March 1, 1992
|
|||
|
|
|||
|
SWEET4C.ASC
|
|||
|
--------------------------------------------------------------------
|
|||
|
This file shared with KeelyNet courtesy of Guy Resh.
|
|||
|
--------------------------------------------------------------------
|
|||
|
|
|||
|
NOTES AND REFERENCES
|
|||
|
|
|||
|
1. E.g., T. E. Bearden and Walter Rosenthal, "On a testable
|
|||
|
unification of electromagnetics, general relativity, and
|
|||
|
quantum mechanics, Proceedings of the 26th Intersociety
|
|||
|
Energy Conversion Engineering Conference (IECEC '91), Aug.
|
|||
|
4-9, 1991, Boston, Massachusetts, p. 487-492.
|
|||
|
|
|||
|
2. E.g., Floyd Sweet and T. E. Bearden, "Utilizing scalar
|
|||
|
electromagnetics to tap vacuum energy," Proceedings of the
|
|||
|
26th Intersociety Energy Conversion Engineering Conference
|
|||
|
(IECEC '91), Aug. 4-9, 1991, Boston, Massachusetts, p. 370-
|
|||
|
375.
|
|||
|
|
|||
|
3. E. T. Whittaker, "On the partial differential equations of
|
|||
|
mathematical physics," Mathematische Annalen, Vol. 57, 1903,
|
|||
|
p. 333-355. In this paper Whittaker proved that all scalar
|
|||
|
EM potentials have an internal, organized, bidirectional EM
|
|||
|
plane-wave structure. Thus there exists an electromagnetics
|
|||
|
that is totally internal to the scalar EM potential. Since
|
|||
|
vacuum/spacetime is scalar potential, then this internal EM
|
|||
|
is in fact "internal" to the local potentialized
|
|||
|
vacuum/spacetime. For discovery of the Whittaker-type
|
|||
|
structure in sonic potentials, see Richard W. Ziolkowski,
|
|||
|
"Localized transmission of wave energy," Proc. SPIE Vol.
|
|||
|
1061, Microwave and Particle Beam Sources and Directed
|
|||
|
Energy Concepts, Jan. 1989, p. 396-397. For a mention of
|
|||
|
this same type of bidirectional EM wave Whittaker structure
|
|||
|
in the potential connected with the Schroedinger equation,
|
|||
|
see V.K. Ignatovich, "The remarkable capabilities of
|
|||
|
recursive relations," American Journal of Physics, 57(10),
|
|||
|
Oct. 1989, p. 873-878. So far, American physicists have
|
|||
|
shown by their nonreaction to Ignatovich's paper that they
|
|||
|
have not yet realized that this is a methodology for
|
|||
|
directly engineering quantum change, and hence physical
|
|||
|
reality itself.
|
|||
|
|
|||
|
4. E. T. 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. In this paper Whittaker
|
|||
|
|
|||
|
Page 1
|
|||
|
|
|||
|
showed that all the classical electromagnetics can be
|
|||
|
replaced by scalar potential interferometry. This ignored
|
|||
|
paper anticipated the Aharonov-Bohm (AB) effect by 55 years,
|
|||
|
and drastically extended it as well. Indeed, it prescribes
|
|||
|
a macroscopic AB effect that is distance-independent,
|
|||
|
providing a direct and engineerable mechanism for action-at-
|
|||
|
a-distance. It also provides a testable hidden-variable
|
|||
|
theory that predicts drastically new and novel effects.
|
|||
|
|
|||
|
5. See Carl Barus, "A curious inversion in the wave mechanism
|
|||
|
of the electromagnetic theory of light," American Journal of
|
|||
|
Science, Vol. 5, Fourth Series, May 1898, p. 343-348. Even
|
|||
|
though Barus actually discovered the "backward-traveling"
|
|||
|
Maxwellian EM wave in 1898, modern Western scientists
|
|||
|
essentially ignored his work, and did not rediscover the
|
|||
|
time-reversed EM wave until it appeared in the open Soviet
|
|||
|
literature. See also Robert A. Fisher, Ed., Optical Phase
|
|||
|
Conjugation, Academic Press, New York, 1983, p. xv. In 1972
|
|||
|
two Soviet scientists, from the P.N. Lebedev Physical
|
|||
|
Institute in Moscow, visited Lawrence Livermore National
|
|||
|
Laboratory and mentioned to U.S. scientists Dr. B. Ya.
|
|||
|
Zel'dovich's observation of an extremely curious "distortion
|
|||
|
undoing" property of the stimulated Brillouin backscattering
|
|||
|
process in a CS2-filled waveguide. This of course was
|
|||
|
nonlinear optical phase conjugation and its production of a
|
|||
|
time-reversed EM wave, the strange new EM wave that
|
|||
|
"reversed disorder and restored order." Thereafter, U.S.
|
|||
|
scientists gradually began working in optical phase
|
|||
|
conjugation. Most of them, however, still have difficulty
|
|||
|
with the fact that the phase conjugate wave is a true time-
|
|||
|
reversed wave. Many do not understand the difference
|
|||
|
between true time reversal (true phase conjugation) and
|
|||
|
pseudo-phase-conjugation.
|
|||
|
|
|||
|
6. Amnon Yariv, Optical Electronics, 3rd edn., Holt, Rinehart
|
|||
|
and Winston, New York, 1985. See particularly Chapter 16:
|
|||
|
"Phase Conjugate Optics __ Theory and Applications."
|
|||
|
|
|||
|
7. David M. Pepper, "Nonlinear optical phase conjugation,"
|
|||
|
Optical Engineering, 21(2), March/April 1982, p. 156-183.
|
|||
|
On p. 156, Pepper specifically notes that "...these
|
|||
|
processing techniques can, in principle, be extended to
|
|||
|
other portions of the EM spectrum (e.g., rt, radio,
|
|||
|
microwave, radars, UV, etc.); and can also involve other
|
|||
|
fields (e.g., acoustic waves), given the proper nonlinear
|
|||
|
medium." In other words, phase conjugation is a universal
|
|||
|
nonlinear phenomenon, unknown until recently. Pepper's
|
|||
|
paper is presently the best all-around introduction to
|
|||
|
nonlinear optical phase conjugation in the English language.
|
|||
|
|
|||
|
8. See also David M. Pepper, "Applications of optical phase
|
|||
|
conjugation," Scientific American, 254(1), Jan. 1986, p. 74-
|
|||
|
83. See particularly the striking photographic
|
|||
|
demonstration of time reversal of disorder on p. 75.
|
|||
|
|
|||
|
9. Robert G. Sachs, The Physics of Time Reversal, University of
|
|||
|
Chicago Press, Chicago, Illinois, 1987.
|
|||
|
|
|||
|
10. For the theoretical proof, see E.V. Smetanin,
|
|||
|
|
|||
|
Page 2
|
|||
|
|
|||
|
"Electromagnetic field in a space with curvature __ new
|
|||
|
solutions," Soviet Physics Journal, 25(2), Feb. 1982, p.
|
|||
|
107-111. A classical particle can have both a magnetic
|
|||
|
moment and a nonzero magnetic charge density in a curved
|
|||
|
spacetime.
|
|||
|
|
|||
|
11. There is a good reason for using two frequencies. To first
|
|||
|
(rough) order, the earth may be approximated as an isotropic
|
|||
|
nonlinear material. In that case, a sine-wave transmitted
|
|||
|
into the earth will simply break up, due to the
|
|||
|
nonlinearities. However, if two sine waves separated
|
|||
|
somewhat in frequency are input into the earth, but one
|
|||
|
pretends that one transmitted the difference frequency
|
|||
|
between them, the difference frequency will act as if it
|
|||
|
were a sign wave transmitted through a linear, nondistorting
|
|||
|
medium __ even though the individual two waves suffer all
|
|||
|
sorts of distortion, breakdown, etc. This is a way of
|
|||
|
"linearizing" a nonlinear situation if it isn't too
|
|||
|
nonlinear.
|
|||
|
|
|||
|
12. Yariv, ibid., p. 500-501. Go back also and take a relook at
|
|||
|
the photo on p. 75 of Pepper, Scientific American, 254(1),
|
|||
|
Jan. 1986. Do you see that, if a heat source scatters EM
|
|||
|
energy into a surrounding phase conjugate mirror, you will
|
|||
|
get some of the scattered energy re-ordered and returned to
|
|||
|
the source?
|
|||
|
|
|||
|
13. An amusing lay description of Tesla's experiment with the
|
|||
|
accidental build-up of "earthquake-like" resonance in the
|
|||
|
buildings and area surrounding his New York laboratory, from
|
|||
|
induction by a tiny electromechanical oscillator, is
|
|||
|
contained in Margaret Cheney, Tesla: Man Out of Time,
|
|||
|
Prentice-Hall, Inc., Englewood Cliffs, New Jersey, 1981, p.
|
|||
|
115-116. Slightly more light is shed on the incident by
|
|||
|
John J. O'Neill, Prodigal Genius: The Life of Nikola Tesla,
|
|||
|
Angriff Press, Hollywood, California, 1981, New Printing, p.
|
|||
|
155-165.
|
|||
|
|
|||
|
14. See John J. O'Neill, Prodigal Genius, p. 164-165. Tesla
|
|||
|
stated that his telegeodynamic oscillator, so small it could
|
|||
|
be slipped into a pocket, could be attached to any part of
|
|||
|
the Empire State Building and in 12 to 13 minutes would
|
|||
|
bring the building to full resonance, and destroy it.
|
|||
|
O'Neill could not make out the decimal point in his notes,
|
|||
|
so could not be sure Tesla stated it would require 0.25 HP
|
|||
|
or 2.5 HP. We point out that it must have been 0.25 if it
|
|||
|
was to be slipped into a rather large pocket. A 2.5 HP
|
|||
|
electric motor of the time would rather definitely not fit
|
|||
|
in one's pocket! See also Cheney, Tesla: Man Out of Time,
|
|||
|
p. 116-117, 275.
|
|||
|
|
|||
|
Tesla indicated that his telegeodynamics could project
|
|||
|
enormous energy through the earth, essentially without loss.
|
|||
|
In other references he indicated that the energy would
|
|||
|
travel in beams to distant points on the earth, producing
|
|||
|
desired effects there. He also indicated that he was
|
|||
|
utilizing a unique form of resonance not presently
|
|||
|
understood by science. Suppose we assume that Tesla had
|
|||
|
discovered the mechanical analogue of the nonlinear optical
|
|||
|
|
|||
|
Page 3
|
|||
|
|
|||
|
pumped phase conjugate mirror. Then his "oscillator"
|
|||
|
actually involved mechanically pumping (by opposing
|
|||
|
mechanical waves or blows) a suitable nonlinear mechanical
|
|||
|
phase conjugation mirror material. If timed at a mechanical
|
|||
|
resonance frequency of the material, and attached to a
|
|||
|
building, an interesting phenomenon would occur. The scalar
|
|||
|
EM potential base waves for rhythmic scalar mechanical
|
|||
|
stress waves have an affinity for traveling through the
|
|||
|
atomic nucleus and its immediately adjacent vacuum. Recall
|
|||
|
that, in QM, all mechanical forces are generated by exchange
|
|||
|
of virtual photons, so opposing forces in a mechanical
|
|||
|
stress are caused by bidirectional virtual photon exchanges.
|
|||
|
It is "scalar electromagnetic" at base. As the scalar EM
|
|||
|
stress potential wave travels through its vacuum/nuclei
|
|||
|
medium, the normal electron orbital vibrations (including
|
|||
|
those caused from covalent bond vibrations, lattice
|
|||
|
vibrations, and temperature vibrations) constitute "signal
|
|||
|
wave inputs," causing the gating and emission of phase
|
|||
|
conjugate replica waves from the pumped nuclei out into the
|
|||
|
material lattices. If the stress pumping is at a resonance
|
|||
|
frequency of the material/nuclei, or a harmonic or
|
|||
|
subharmonic of it, then nonlinear oscillation theory
|
|||
|
together with E.T. Whittaker's bidirectional EM wave
|
|||
|
composition of the scalar stress potential will result in a
|
|||
|
phase-locked buildup or accumulation of the gated PCR energy
|
|||
|
from the activated vacuum/nuclei internal medium by
|
|||
|
constructive interference of the continually-gated PCR EM
|
|||
|
energy into the material lattice at its resonant frequency.
|
|||
|
In that case a "forced resonance" condition occurs in the
|
|||
|
building, surrounding earth, etc., and this scalar
|
|||
|
mechanical stress resonance spreads and builds, to enormous
|
|||
|
power __ even to the destruction of the building or to an
|
|||
|
earthquake.
|
|||
|
|
|||
|
But since the oscillator itself has certainly not input such
|
|||
|
a large amount of energy, from whence does all the extra
|
|||
|
energy come? The answer is contained in Sweet and Bearden,
|
|||
|
"Utilizing scalar electromagnetics to tap vacuum energy,"
|
|||
|
IECEC '91, ibid. The activated nuclei, in this mechanical
|
|||
|
scalar oscillator case, actually involve an oscillation
|
|||
|
modulated upon the virtual photon flux exchange between the
|
|||
|
activated local vacuum and each activated nucleus, similar
|
|||
|
to the type of oscillation that Sweet traps in the barium
|
|||
|
nuclei of his vacuum triode. This scalar oscillation onto
|
|||
|
the activated nucleus converts that nucleus to a pumped
|
|||
|
phase conjugate mirror (PPCM). Covalent bond oscillations
|
|||
|
and material lattice vibrations introduce "signal wave"
|
|||
|
inputs into the pumped nucleus through the EM coupling with
|
|||
|
its electron shells. Amplified phase conjugate replica
|
|||
|
(PCR) waves are thus emitted by these PPCM nuclei, in
|
|||
|
response to the signal wave inputs. According to standard
|
|||
|
PPCM theory, these amplified PCR waves will thus leave the
|
|||
|
nucleus and travel out through the electron shells into the
|
|||
|
material lattice, being scattered there. This process
|
|||
|
effectively gates energy from the vacuum/nucleus VPF
|
|||
|
exchange into the PCR waves, which "backtrack" the signal
|
|||
|
wave input path, back out into the material lattices, etc.
|
|||
|
If the pumping is at the fundamental, a harmonic, or a
|
|||
|
subharmonic of the resonance frequency of the materials,
|
|||
|
|
|||
|
Page 4
|
|||
|
|
|||
|
then the scattered energy will accumulate "in phase" and the
|
|||
|
materials and building will be in increasing resonance.
|
|||
|
Thus the building and the local earth will begin to build up
|
|||
|
increasing, rumbling oscillations, as the increasing PCR
|
|||
|
waves from the PPCM nuclei scatter increasing energy into
|
|||
|
their constituent materials. The enormous energy involved
|
|||
|
is actually organized and gated from the excited local
|
|||
|
vacuum itself.
|
|||
|
|
|||
|
As to Tesla's telegeodynamics and making mechanical waves
|
|||
|
that are laser-like and travel through the earth, one need
|
|||
|
only apply the known principle of the forward-going PCR
|
|||
|
wave. In other words, one deliberately inputs, say, two
|
|||
|
small signal waves. The PPCM material acts as if a single
|
|||
|
signal wave had been input, as a vector resultant wave. The
|
|||
|
resulting amplified PCR wave thus "backtracks" the
|
|||
|
resultant. If the resultant signal wave input is a sharp
|
|||
|
laser-like incoming beam, then the responding amplified PCR
|
|||
|
wave will be a sharp laser-like beam in the reverse
|
|||
|
direction. In such manner, a laser-like mechanical
|
|||
|
oscillation beam can be launched through the earth. The
|
|||
|
laser-like portion is based on a laser-like scalar potential
|
|||
|
beam that travels through the vacuum and atomic nuclei as
|
|||
|
its natural medium. Such a beam should travel through the
|
|||
|
earth or through the ocean with ease, since the scalar wave
|
|||
|
is gravitational, and not affected by the ionized electron
|
|||
|
shells of seawater, e.g. Note that, by slightly varying the
|
|||
|
signal wave input resultant, one can "steer" the PCR wave
|
|||
|
through its medium (the vacuum/atomic nuclei), much as a
|
|||
|
phased array radar steers its beam through space. It
|
|||
|
strongly suggests that one can make an underwater scalar
|
|||
|
radar or a "through the intervening earth" scalar radar, as
|
|||
|
well.
|
|||
|
|
|||
|
15. 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 an extensive
|
|||
|
discussion of the Aharonov-Bohm effect and an extensive list
|
|||
|
of references, see S. Olariu and I. Iovitzu Popescu, "The
|
|||
|
quantum effects of electromagnetic fluxes," Reviews of
|
|||
|
Modern Physics, 57(2), Apr. 1985. For confirmation that the
|
|||
|
AB effect has been proven to all but the most diehard of
|
|||
|
skeptics, see Bertram Schwarzschild, "Currents in normal-
|
|||
|
metal rings exhibit Aharonov-Bohm effect," Physics Today,
|
|||
|
39(1), Jan. 1986, p. 17-20.
|
|||
|
|
|||
|
16. 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; I.J.R. Aitchison, "Nothing's
|
|||
|
plenty: The vacuum in modern quantum field theory,"
|
|||
|
Contemporary Physics, 26(4), 1985, p. 333-391; 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 semiconducting vacuum,"
|
|||
|
American Journal of Physics, 52(1), Jan. 1984, p. 19-21.
|
|||
|
See also R. Jackiw and J.R. Schrieffer, "The decay of the
|
|||
|
vacuum," Nuclear Physics B 190, 1981, p. 944.
|
|||
|
|
|||
|
|
|||
|
Page 5
|
|||
|
|
|||
|
17. Nick Herbert, Quantum Reality: Beyond the New Physics,
|
|||
|
anchor Books, Doubleday, Garden City, New York, 1987 is
|
|||
|
particularly recommended.
|
|||
|
|
|||
|
18. An excellent and thorough reference is Romon Podolny,
|
|||
|
Something Called Nothing __ Physical Vacuum, What is It?",
|
|||
|
Mir, 1986.
|
|||
|
|
|||
|
19. See particularly H.E. Puthoff, "Source of vacuum
|
|||
|
electromagnetic zero-point energy, Physical Review A, 40(9),
|
|||
|
Nov. 1, 1989, p. 4857-4862; "The energetic vacuum:
|
|||
|
Implications for energy research," Speculations in Science
|
|||
|
and Technology, 13(4), 1990, p. 247-257; "Gravity as a Zero-
|
|||
|
Point Fluctuation Force," Physical Review A, Vol. 39, 1989,
|
|||
|
p. 2333; "Ground State of Hydrogen as a Zero-Point-
|
|||
|
Fluctuation-Determined State," Physical Review D, Vol. 35,
|
|||
|
1987, p. 3266.
|
|||
|
|
|||
|
20. T.D. Lee, Chapter 25: Outlook, "Possibility of vacuum
|
|||
|
engineering," Particle Physics and Introduction to Field
|
|||
|
Theory, Harwood Academic Publishers, New York, 1981, p. 826.
|
|||
|
The application of the extended Whittaker scalar EM is in
|
|||
|
fact the method of accomplishing the very vacuum engineering
|
|||
|
speculated upon by Nobel Laureate Lee.
|
|||
|
|
|||
|
21. Here I particularly recommend B.J. Hiley and F. David Peat,
|
|||
|
Eds., Quantum Implications: Essays in Honour of David Bohm,
|
|||
|
Routledge & Kegan Paul, London and New York, 1987. You
|
|||
|
should of course also be aware of what Bohm's hidden
|
|||
|
variable theory is all about, and its connection with
|
|||
|
consciousness. See D. Bohm, Phys. Rev. 85, 1952, p. 166,
|
|||
|
180; Causality and Chance in Modern Physics, Routledge &
|
|||
|
Kegan Paul, London, 1957; "Hidden variables and the
|
|||
|
implicate order," in Quantum Implications: Essays in Honour
|
|||
|
of David Bohm, Eds. B.J. Hiley and F. David Peat, Routledge
|
|||
|
& Kegan Paul, London & New York, 1987, p. 33. See also D.
|
|||
|
Bohm and B.J. Hiley, Found. Phys. 5, 1975, p. 93; Found.
|
|||
|
Phys. 12, 1982, p. 1001; Found. Phys. 14, 1984, p. 255. See
|
|||
|
also Y. Aharonov and D. Albert, "The issue of retrodiction
|
|||
|
in Bohm's theory," in Quantum Implications: Essays in Honour
|
|||
|
of David Bohm, ibid., p. 223. For a discussion of what
|
|||
|
nonlocal theory may really entail in terms of modular
|
|||
|
variables, see Yakir Aharonov, "Non-local phenomena and the
|
|||
|
Aharonov-Bohm effect," Quantum Concepts in Space and Time,
|
|||
|
Eds. R. Penrose and C.J. Isham, Clarendon Press, Oxford,
|
|||
|
1986, p. 41-64. For other important discussions see Lee
|
|||
|
Smolin, "Stochastic mechanics, hidden variables, and
|
|||
|
gravity," ibid., p. 147-173; and Abner Shimony, "Events and
|
|||
|
processes in the quantum world," ibid., p. 182-203. For a
|
|||
|
new viewpoint on emission processes, see Robert M. Wald,
|
|||
|
"Correlations and causality in quantum field theory," ibid.,
|
|||
|
p. 293-301; and Serge Haroche and Daniel Kleppner, "Cavity
|
|||
|
quantum electrodynamics," Physics Today, Jan. 1989, p. 24-
|
|||
|
30. See David Bohm, Wholeness and the Implicate Order,
|
|||
|
Routledge and Kegan Paul; London, Boston, and Henley; 1980.
|
|||
|
|
|||
|
22. Even Einstein __ who was awarded the Nobel Prize in part for
|
|||
|
explaining the photoelectric effect __ never understood what
|
|||
|
a photon was. In his later years Einstein wrote: "All these
|
|||
|
|
|||
|
Page 7
|
|||
|
|
|||
|
50 years of pondering have not brought me closer to
|
|||
|
answering the question: what are light-quanta?". The
|
|||
|
quotation is contained in P. Speziali, Ed., Albert Einstein-
|
|||
|
Michele Besso Correspondence 1903-1955, Hermann, Paris,
|
|||
|
1972. There are formidable problems with the photon
|
|||
|
concept. E.g., the "energy" of a photon is not localized,
|
|||
|
but is distributed over the entire volume of the field and
|
|||
|
there is, in general, no use in attaching a coordinate to
|
|||
|
the photon. A photon in general cannot be described by a
|
|||
|
wavefunction, but only for special cases. In geometrical
|
|||
|
optics as well as Maxwell's electrodynamics, there is no
|
|||
|
room for photons. The complex one-photon wavefunction
|
|||
|
should not be identified with the electromagnetic field.
|
|||
|
For a given photon number, the electric or magnetic fields
|
|||
|
at a point cannot be measured as a function of time. For
|
|||
|
states with a fixed photon number, the expectation value of
|
|||
|
the electric field is zero even for a very large photon
|
|||
|
number, so that in this case the correspondence principle
|
|||
|
cannot be used. For additional strong anomalies in the
|
|||
|
concept of a photon, see J. Strand, "Photons in introductory
|
|||
|
quantum physics," American Journal of Physics, 54(7), July
|
|||
|
1986, p. 650-652.
|
|||
|
|
|||
|
23. Richard Kidd et Al, "Evolution of the Modern Photon,"
|
|||
|
American Journal of Physics, 57(1), Jan. 1989, p. 27-35.
|
|||
|
Note particularly that detection is actually binary, but
|
|||
|
one-half of each detection/measurement is normally discarded
|
|||
|
[actually, it is just hidden and listed as simply "Newton's
|
|||
|
third law reaction force."]. See also R. Chen,
|
|||
|
"Cancellation of Internal Forces," American Journal of
|
|||
|
Physics, 49(4), Apr. 1981, p. 372 for the fact that the
|
|||
|
internal EM energy is always involved in interactions, but
|
|||
|
usually never taken into account.
|
|||
|
|
|||
|
Indeed, the so-called "photon interaction" is usually a
|
|||
|
spin-2 graviton breakup interaction. The graviton fissions
|
|||
|
(the photon and antiphoton decouple). The photon half
|
|||
|
normally interacts with the electron shells. The antiphoton
|
|||
|
half "burrows back into" the nucleus and interacts with it,
|
|||
|
providing the Newtonian third law recoil and the
|
|||
|
conservation of angular momentum, energy, etc. The
|
|||
|
ubiquitous presence of the Newtonian third law reaction
|
|||
|
force is direct and positive evidence for the fact that not
|
|||
|
only a photon interacts, but an antiphoton interacts also.
|
|||
|
|
|||
|
Consider. Quantum field theory requires that every
|
|||
|
mechanical force be generated by virtual photon
|
|||
|
interactions. Therefore, to be consistent, Newton's third
|
|||
|
law reaction force must be generated by photon interaction.
|
|||
|
Since the 3rd law force is considered to be universal, it
|
|||
|
means that the "photon interaction that is a reverse of the
|
|||
|
normal photon interaction" is universal, and this "reversed
|
|||
|
photon" interaction must normally accompany each normal
|
|||
|
photon interaction. We point out that the only type of
|
|||
|
photon that would consistently produce the exact opposite
|
|||
|
force from the photon interaction would be a phase conjugate
|
|||
|
or time-reversal of that photon. I.e., there must have been
|
|||
|
two photons present in the interaction: the normal or time-
|
|||
|
forward photon, and the time-reversed or antiphoton. This
|
|||
|
|
|||
|
Page 7
|
|||
|
|
|||
|
is actually implied by a quantum field theory statement of
|
|||
|
Newton's third law.
|
|||
|
|
|||
|
However, the point can be even more rigorously proven. In a
|
|||
|
phase conjugate material, one can trick the antiphoton into
|
|||
|
exiting out of the atom, instead of interacting in the
|
|||
|
nucleus. In that case, according to the "photon interaction
|
|||
|
is normally graviton interaction" principle, the agent that
|
|||
|
normally generates Newton's third law recoil did not reach
|
|||
|
the nucleus, and so the recoil should be absent. And it is
|
|||
|
absent, in actual experiments. Such a phase conjugate
|
|||
|
mirror does not recoil if it emits a phase conjugate replica
|
|||
|
wave (phase conjugate photons, or antiphotons). And it
|
|||
|
doesn't recoil no matter how powerful that antiphoton
|
|||
|
emission is __ no matter how many antiphotons it emits. On
|
|||
|
the other hand, if the same material emits an ordinary
|
|||
|
photon, it does recoil, and Newton's third law is present.
|
|||
|
This experiment directly establishes that most photon
|
|||
|
interactions actually are graviton interactions __ paired
|
|||
|
photon/antiphoton interactions.
|
|||
|
|
|||
|
24. To see just how arbitrary and postulational are present
|
|||
|
"definitions" of mass and force, see Robert Bruce Lindsay
|
|||
|
and Henry Margenau, Foundations of Physics, Dover
|
|||
|
Publications, New York, 1963, p. 283-287. Note on page 283
|
|||
|
that a "field of force" at any point is actually defined
|
|||
|
only for the case when a unit mass is present at that point.
|
|||
|
See also Richard P. Feynman, Robert B. Leighton, and Matthew
|
|||
|
Sands, The Feynman Lectures on Physics, Addison-Wesley, New
|
|||
|
York, Vol 1, p. 2-4, for a definition of the electric field
|
|||
|
in context of its potentiality for producing a force. The
|
|||
|
modern view of the field is that, because of vacuum
|
|||
|
fluctuations, rigorously one no longer speaks of "the"
|
|||
|
field, but of the probability of a particular field
|
|||
|
configuration. See Charles W. Misner, Kip S. Thorne, and
|
|||
|
John Archibald Wheeler, Gravitation, W.H. Freeman and Co.,
|
|||
|
San Francisco, 1973, p. 1191. Note that this view is still
|
|||
|
in error when one considers electron precession in the
|
|||
|
interaction of vacuum "fields" and the electron gas inside a
|
|||
|
detecting probe wire.
|
|||
|
|
|||
|
25. Aharonov and Bohm, Physical Review, 1959, ibid.
|
|||
|
|
|||
|
--------------------------------------------------------------------
|
|||
|
|
|||
|
If you have comments or other information relating to such topics
|
|||
|
as this paper covers, please upload to KeelyNet or send to the
|
|||
|
Vangard Sciences address as listed on the first page.
|
|||
|
Thank you for your consideration, interest and support.
|
|||
|
|
|||
|
Jerry W. Decker.........Ron Barker...........Chuck Henderson
|
|||
|
Vangard Sciences/KeelyNet
|
|||
|
|
|||
|
--------------------------------------------------------------------
|
|||
|
If we can be of service, you may contact
|
|||
|
Jerry at (214) 324-8741 or Ron at (214) 242-9346
|
|||
|
--------------------------------------------------------------------
|
|||
|
|
|||
|
|
|||
|
|
|||
|
Page 8
|