- 51 - If one takes a further look at the spread of electro-magnetic energy under these circumstances, one will also find some very interesting aspects. Electro-magnetic energy is usually absorbed by matter under normal circumstances. This happens on the one hand in isolators through direct losses and on the other hand in electrical conductors through the interaction between electrons and the crystal lattice. Let’s look at the spread in isolators (no loss mechanisms caused by conductor electrons). The possibility exists in this case that we are dealing with an inversion of occupation conditions similar to Maser, that in conjunction with the incidental electro-magnetic wave induced emission, makes a coherent amplification mechanism possible. This can lead to a reduction of the damper losses (di-electrical losses) that appear during the spreading. The inversion of the occupation conditions could produce higher frequencies in the present high frequency energy (pumpfrequency). With the spread of an electro-magnetic wave through water, this would for instance mean that due to the absorption of suitable high frequency energy, that can either stem from the sun, thunderstorm activity or other atmospheric conditions, or also from the worldwide utilisation of electric energy, states of energy in the corresponding inversion appear in the water. If a high frequency signal of a suitable frequency is now introduced to the water, it would be quite conceivable that through induced emissions, the spread of electro-magnetic waves becomes possible across vast distances according to what was indicated above. The intensity of the high frequency electrical, respectively magnetic strength of the field can be extraordinarily weak - well, possibly be even under the thermic noise level. What is required is that the half-value range in the induced emission of the associated resonance processes are accordingly small, that is to say, that the lifespan of the inversion conditions are accordingly high. The possibility could arise from this that signals and with them information, can be transmitted over vast distances through water and possibly even through water-bearing layers. Prerequisite for an affective information transmission would be a suitable narrow band receiver system with bandwidths of a few hertz. No accurate accounts about the required frequencies for such transmissions can presently be furnished. According to the previous experimental results, these can be within the ultrashort wave range or possibly also in the microwave range. The spread of electro-magnetic energy though metallic conductors can, against popular opinion, exhibit modifications, if the intensity of the wave in the electro-magnetic field becomes very small. If an electro-magnetic wave were for instance to hit a metallic surface, the free electrons in the metal would be agitated to resonate through the electrical field vector. This resonance happens coherently with higher field amplitudes, that is to say, a positive phase relationship between the resonating electrons exists within the larger local regions. The result of this is that the electromagnetic fields of the incidental electro-magnetic waves, produced by the oscillating electrons, overlap and eliminate then through superposition. This is what’s called the skin-effect. The elimination through interference is disturbed if the unambiguous relationship between the resonating electrons is disturbed, this is the case if the electrons are conceded to the grid through energy impacts. The coherence is disturbed, because these impacts happen completely irregular, so that the depth of penetration of the skin-effect also increases with the increasing interplay between the conductor’s electrons and the grid - ergo with an increasing specific resistance of the material. Let us now look at an electro-magnetic wave where the electrical field vector is so minute that the energy increase of the conductor electrons is small compared to the thermic energy of the electrons. This scenario shows that a different type of behaviour is apparent from the one of the normal skineffect. When explaining the skin-effect, one generally assumes that the energy of the oscillating electrons is greater than its medium thermic energy. By taking the thermic energy of the conductor
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