UPH-Scanner™ - Universal Photoelectric Scanner - Employing Xerqon's 'Entangled Chromatic Pair'™ Law

A 2.2 m x 1.1 m photo-sensor plate equivalent (to include the tallest people as subjects) is made of Copper Carbide with the highest carbon concentration while still remaining a non-corrodible sheet of insulated metal. It will easily form the hole field - or more easily expressed - the positron field.

The simplest way to achieve plate area coverage is to use a plate of more than body span and small width. It can be slid under the body, lengthwise parallel to the carbon rich, carbide electromagnetic emmitter. To achieve the expected effect, slide both components simultaneously - emitter over sensor. For dense or deep material samples, radio is the best, biologically mild, radiation spectrum to emit.

That is the field derived from the absorption of photons, producing the antiphotons which correspond to the positron field in the copper carbide plate, to then follow as an electron field in the electrical circuit from the copper carbide plate.

The field strength is increased by increasing the voltage perpendicular or orthogonal to the plate, all the way through the circuit to the opposing, display plate. In keeping with the conservation of information, a photon is never its own antiparticle, or the antiparticle would have no meaning. Instead, Pauli's Principle (ideally Pauli's Law) applies.

The photons exist in chromatic pairs - eg Cyan spin to Red spin. The array is infinite and binary in it electromagnetic power sequence. The colour in must be matched by quantum entangled, spectral paired partner colour.

Apply a pincer configured electrode to one length and another to one breadth of the plate, so that the two ends of the pincer wiring configurations each meet at a common, central junction - two of them in total. Their output would be, in series. The final step is to display the result on a monitor plate of carbon rich copper carbide. It will convert the electron field, in the circuit wiring, to continue as an electron field in the darker, copper carbide.

That will emit an electron field (in forcing the plate's bias back to positron state) from that plate and produce a photon field for visual display - in corresponding chromatics of the input of the human body matter's electric reaction to the light, prior to releasing the amplified electron field from the light.

Full, Power Field Path Sequence, in Summary

1. The sample tissue is irradiated with LED, white light and the permeating portion of the photon field radiates through the sample tissue.

2. The photons amplify of forcibly stimulate the voltage of the tissue material against its natural bias of amplification equilibrium.

3. In falling back to the unstimulated equilibrium state, the material of the sample emits photons, in all directions, which are reflective of the material composition.

4. The emitted photons are voltage amplified as converted electrons, across the receiving, dark (high carbon level) carbide plate.

5. The electrons field from the plate is carried to the emitter/display plate of the same material as the first plate.

6. The plate area is best suited as the same shape and proportions as the first plate.

7. It will emit an image when the plate is positively voltage amplified.

The purpose of the single, substrate, pixel plate is to provide much higher resolution than from mechanically tessellated pixel plates.

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