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Table of Contents

A Sensitive Scalar Wave Detector

1.
2.
3.
4.
5.
6.
7.
8.
9.

10.
11.

Figure 11. NETWORK OF VIRTUAL TRANSMITTERS

12.

Figure 12. VIRTUAL TRANSMITTERS IN THE
INTERFERENCE GRID

13.

Figure 13. GIANT RADIAL RELATED TO A VIRTUAL
TRANSMITTER

14.

Figure 14. FORMATION OF A SINGLE GIANT RADIAL

15.

Figure 15. FORMATION OF A DOUBLE GIANT RADIAL

16.

Figure 16. DETECTION OF TRANSVERSE AND
LONGITUDINAL WAVES

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Scalar Wave Detector

from STAR WARS NOW!

The Bohm-Aharonov Effect, Scalar Interferometry, and Soviet Weaponization
by

Lt. Col. T.E. Bearden (retd.)

, 1984

Copyright

A Sensitive Scalar Wave Detector

Very briefly we present a method of making a very sensitive scalar wave detector so that direct
measurement and quantization can be established.

First, we regard one oscillation (one wavelength) of the scalar potential wave as a longitudinal
photon. Note that this photon contains a substructure, which may be deliberately determined (when
artificially made) or randomized (when naturally made in the idealized case).

For convenience we represent normal linearized vacuum (spacetime) as a horizontal or longitudinal
vector (Figure 4), implying the direction of motion of the wave in the laboratory frame. By horizontal
position in our diagram, we imply a linear, uncurved spacetime and a non-rotated frame. We
represent the longitudinal scalar wave as a horizontal vector, and the usual Hertzian wave as a
vertical or "transverse" vector. We visualize a normal detector as detecting only a vertical or
"transverse" vector, as we have illustrated in Figure 4.

As can be seen, in a linear, unrotated or uncurved spacetime a pure scalar wave has no vertical
component projected upon the laboratory frame vector, so it is not detectable by normal detectors.

To detect the scalar wave, of course we could bend it so that it has a projected vertical component in
the laboratory frame (Figure 5). However, this would be an impure wave, not a pure scalar wave, and
that is not what we wish.

A better way is to bend or curve spacetime itself in a small region, so that a longitudinal wave that
passes through that region now possesses a vertical component with respect to that region (Figure 6).
Thus a normal detector there will detect that vertical component. We conduct the detection current
out of the "bent spacetime" region to an outside (normal) detector, and we then have a scalar wave
detector.

To illustrate, we show conceptually how this has been successfully done. Figure 7 shows the concept.
First, we utilize a magnetic pole to provide the infolded energy (potential) to bend or curve
spacetime. To reach good sensitivity, we need a pole strength connected with a magnetic field
strength of 40,000 Gauss or higher. We utilize a small superconducting magnet, which can reach field
strengths of from 40,000 to 80,000 Gauss.

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Scalar Wave Detector

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Scalar Wave Detector

Slide 33 - FER DE LANCE

Then to prevent detection of superfluous "normal" radiation, we shield the entire magnet in a
grounded Faraday cage, as shown in the figure. Hertzian waves will be grounded in this shield, while
scalar waves will readily penetrate it undiminished. In other words, the Faraday cage serves as a
"stripper," to strip away the ordinary waves, leaving only the scalar waves to penetrate inside. An
ordinary wire lies at the top of the magnetic pole, in proximity to it. The wire runs out of the Faraday
cage through an insulated port to a resonant tuning circuit, which is sharply tunable over the range of
frequencies we are interested in. A preamp amplifies the output of the tuner, and in turn feeds the
input of an oscilloscope or other detector.

With this detector we can select the frequency desired, and detect any passing scalar waves of that
frequency. By other variations of amps and preamps, regenerative circuits, etc. we can obtain all the

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Scalar Wave Detector

sensitivity desired, and utilize ordinary detection equipment already well-known and highly
developed.

Additional Information about detecting Scalar Waves

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Figure 11. NETWORK OF VIRTUAL TRANSMITTERS

(See Woodpecker Grid)

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Figure 12. VIRTUAL TRANSMITTERS IN THE INTERFERENCE GRID

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Figure 13. GIANT RADIAL RELATED TO A VIRTUAL TRANSMITTER

Fall 1983:

Florida

Alabama

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Figure 14. FORMATION OF A SINGLE GIANT RADIAL

Excerpt P 172
FER DE LANCE

A Briefing on Soviet Scalar Electromagnetic Weapons
by Lt. Col. T.E. Bearden (retd.), 1986
Copyright

2. Continual cloud radials have repeatedly been seen and photographed over Huntsville,
Alabama, associated with weather engineering and grid activity. Typical radials seen by this
author are shown in Bearden, Soviet Weather Engineering Over North America, 1-hr. v1deotape,
1985. Huntsville is apparently a pivot point or "hinge point" for bending and controlling the
jetstream.

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3. Spectacular cloud grid patterns have been seen over Huntsville, Alabama and Los Angeles,
California. An excellent videoclip of one of the Los Angeles area grids, personally observed and
shot by KABC Open Mind talk show host Bill Jenkins, is shown in Bearden, Soviet Weather
Engineering Over North America,;1-hr. videotape, 1985. An artist's sketch of an earlier gigantic
grid, extending from horizon to horizon in every direction, seen over Huntsville, Alabama by
Tom Bearden and Ken Moore, is also shown in the tape. The videotape is available from P.O.
Box 1472, Huntsville, AL 35807. Sketches and details of another highly anomalous grid pattern
observed in the greater Los Angeles area by engineer Ron Cole are shown in figures 5 and 6.

The reason that clouds of water droplets and/or ice particles detect the scalar interferometry and
form signature patterns is simple: Consider each H2O molecule as having two light little
hydrogen atoms hanging on to the much heavier oxygen atom. The covalent sharing with the
oxygen atom of the electron from each hydrogen atom means that

1. the electrostatic scalar potential between the H ion and the O ion it is bonded to, is

rhythmically varying as the electron is shared back and forth,

2. this varying potential contains "electron spin holes" since it is made by the moving

electron,

3. two such varying potentials exist since there are two H atoms sharing covalent electrons

with the O atom,

4. the two H ions are at an angle of over 100 degrees with respect to each other,
5. the molecule assembly thus constitutes one part (one half, so to speak) of a scalar

interferometer with imbedded electron spin holes for electron hooking,

6. Incident scalar waves from outside the system interact with the "half scalar

interferometer." This scalar interferometry interaction is coupled to the covalent bonding
electron because of the internal spin hole pattern of the molecular half of the
interferometer. The coupled electron moves with the sca1ar pattern's changes, causing an
observable interaction with and in the electrical structure and ionic potential of the
molecule,

7. the weak H to H hydrogen bonding between molecules connects resulting ionic potential

changes to the structuring of the entire macroscopic cloud assembly. Thus by scalar
interferometry with the H

2

O "half interferometers", an incident scalar EM pattern is

detected and translated into patterns of E and B force fields. The H

2

O molecules then

"line up" in accord with the electrical patterns detected.

Thus the clouds form "signature patterns" according to the incident scalar EM radiation patterns.
Giant cloud radials in the targeted area are probably due to the type and shape of antennas
including the type and shape of the electrical wires establishing the antennas' ground planes --
used by the Soviet Union to project the scalar waves. Note that such "radial" antenna patterns
were occasionally used by James Harris Rogers in his underground and undersea scalar EM
transmission system.

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Figure 15. FORMATION OF A DOUBLE GIANT RADIAL

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Figure 16. DETECTION OF TRANSVERSE AND LONGITUDINAL

WAVES

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