A Sensitive Scalar Wave Detector


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

by Lt. Col. T.E. Bearden (retd.), 1984

Copyright

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

 Additional Information about detecting Scalar Waves

En su artículo “Appendix 1: Some important indicators and destructive testing”, Tom Bearden explica y describe el método como se puede hacer visible la energía de armas electrónicas sacando fotos con un filtro especial que elimina la luz del día. Ese artículo lo había descargado hace unos años desde la página Web del autor en: www.cheniere.org/books/ferelance/appendix1.htm#scalar_photography, donde ya no está. Por eso inserto aquí la parte sobre “fotografía escalar”. Si alguien sepa, donde se puede conseguir ese tipo de filtro, por favor, me lo comunique. The reason is that Bob Gladwin’s camara was utilizing a form of photography pioneered – to the best of my knowledge – by Trevor James Constable. At least I learned about it from Constable’s books and articles. I then told it to my good friend, Joe Gambill, and Joe applied and adapted it to the unusual photography which he performs. Both Constable and Gambill are masters of this type of photography. Once I got deeply into scalar electromagnetics, I finally figured out what was going on in this methodology.
Briefly, here’s the way it works. Scalar energy, of course, has to be detected by some sort of interference phenomenon. There exists a very special way to get a camera to perform such interference for you.
In the EM spectrum, the infrared and the ultraviolet have a special relationship to each other. The ultraviolet is exactly twice the frequency of the infrared, if the two zones are properly chosen. In other words, the UV is the first harmonic of the IR.
The scalar EM energy, since it operates in the Kaluza hyperspace surrounding every point in ordinary space, may be considered to be composed of pure spin. (That is, it’s moving in a dimension where each particle of that dimension is spinning). Harmonics there are spin harmonics.
In this photon-interaction produced level of reality (the ordinary world), the IR and UV bands are more closely connected to the “shadow world” in which scalar energy moves. Thus, there is a sort of shadow “swirling” of the scalar energy near the IR and the UV. Entry of the scalar energy into this world, through the IR and UV windows by a kind of “harmonic interferometry”, is normally prevented by the presence of visible light. That is, visible light “squelches” the “paranormal channel” that lurks beneath the IR and UV zones.
To make use of the IR and UV interference source zones, Constable covered his camara lens with a special filter (18A), which is opaque to the visible light spectrum and transparent to the IR and UV spectrum. The scalar energy surges through these two source windows and phaselocks harmonically. That is, the scalar energy interference, on the film, is (recall) swirling in frequency. The net result is that the film records the interfering scalar energy as visible spectrum energy.
Infrared film can be used to increase the response in many circumstances.
Both Constable and Gambill have rigorously proven this technique in literally thousands of “paranormal” photographs. (They do no necessarily use my scalar EM terminology, but the technique is rigorous and works, regardless of terms.)
Under nighttime conditions, sometimes the particular lens and film combination will phaselock between IR and UV for incident scalar EM energy. This is particularly when a relatively strong source of IR is in the vicinity. 

While Bob Gladwin was taking his photographs, there was no suppression of the IR/UV phase-lock effect by visible light because it was night and there was hardly any visible light entering his lens.” 

FROM STAR WARS NOW!