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Such a picture could only be obtained if the particle behaved like a wave, then it could form with itself and at the moments of opposite peaks extinguish each other, forming dark areas and in reverse positive moments, on the contrary, reinforcing each other, creating the above described bands.
However, the corpuscular properties of particles are also highlighted, for example, in experiments with the photoelectric effect, it is the corpuscular nature of particles that acts. Based on the above, we had to conclude that particles are both waves and corpuscles, but how could this happen when it contradicted itself? In the quantum world, this was a reality, but for the macrocosm it still remained a mystery until the so-called dense «walking droplets» were used as an explanation.
This effect is formed when a medium-density liquid, for example oil, begins to vibrate and during the interaction of the liquid surface with a pointed object, it begins to divide into droplets, which immediately have to connect with the liquid, but this does not happen due to vibrations and they literally jump on the surface. Each of these drops is held under the influence of vibration, but moreover, such drops have the property of moving, because under the influence of vibrations they create standing waves that propagate across the surface, however, during the interaction of the drop with it, it begins to change its direction, which is why the effect of the movement of the drop is formed.
The present explanation can be applied to Jungs experiment by directing the droplets towards two slits. It is worth clarifying before this that the drop itself expresses in this case a corpuscle-particle, when vibrations are the probabilistic nature of the existence of quantum objects the particles under study in the person of photons, electrons, ions and others. When a particle begins to move towards the slit, its wave, which begins to oscillate at the level of spacetime, due to the vibrational nature of the particle the variable probability of its being at a specific point, since its movement is discrete, according to the tunneling effect, begins to interact with the particle itself.
So, when it approaches the gap, it passes through one of the slits, when its wave passes through both, as a result of which, after passing through the barrier, the particle begins to interact with the formed wave, changing its trajectory. Thus, one can clearly see how the interference pattern is formed using the example of explaining Youngs experiment with two slits by means of jumping droplets.
In addition, during the explanation of the experiment, the concept of tunneling was demonstrated, which can also be represented by jumping droplets. The fact is that any space, according to the quantum vacuum model, has an infinite number of particles that are immediately born, annihilate with each other, disappear, etc., that is, according to the quantum vacuum model, there is practically no particle free space, from which it can be concluded that in order for a particle to be able to overcome no matter how small the distance, it needs energy through which it could overcome this distance, but it also happens that a particle overcomes the same distance without practically losing energy, which is called tunneling.
In this case, there is a barrier in front of the particle that is moving, which it must overcome by making a certain leap through it, but without expending energy to overcome it. Surprisingly, this effect can also be represented in the form of a drip model, according to which, if a certain wall is placed in front of a drop, then each time it will try to jump over it, but it will not work, however, at a certain moment, interaction with its own standing wave may be sufficient to obtain additional energy and to overcome the barrier. In such a phenomenon, the probability is surprisingly determined in the macrocosm in the same way as it is determined in the quantum measurement and description of the phenomenon of quantum tunneling of particles.
Moreover, the generality of the described phenomena for a wide variety of particles, from elementary particles to ions, is important, which in a sense makes the droplet model of demonstration almost universal. However, a large number of phenomena still remain unexplained, which means that not a few works should be done on the basis of available data and the drip model, as one of the most progressive analogies, will have to overcome quite a few tests on the way to achieving the goals set.
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TECHNICAL SCIENCES
DETERMINATION OF THE SURFACE RECOMBINATION RATE IN POLYCRYSTALLINE FILMS FROM THE CDTE-SIO
2
SI-AL COMPOUND BY THE MW-PC METHODUDC 544.22
Alimov Nodir Esonalievich
Doctor of Philosophy in Physical and Mathematical Sciences, Lecturer at the Department of Physics, Faculty of Physics and Technology, Ferghana State University
Ferghana State University, Ferghana, Uzbekistan
E-mail: alimov.nodir.esonaliyevich@gmail.com
Annotation. In this article, the rates of surface recombination in polycrystalline CdTe films obtained on oxidized substrates are studied, and the results of the action of corona discharge into the CdTe-SiO2Si-Al structure are presented. In the static mode, a shift of the short-circuit current spectra to the short-wave region was observed. To analyze the displacement of the short-circuit current spectra, the microwave probe photoconductivity (MW-PC) method was used and contactless registration of transient decay processes for redundant carriers was performed. From the data obtained, it was found that the rate of surface recombination was estimated at 19 ns. It was determined that filling of surface traps in CdTe leads to a decrease in the effect of surface recombination.