title: ÐÐ»Ð¸ÑÐ½Ð¸Ðµ Ð¼ÐµÐ¶Ð°ÑÐ¾Ð¼Ð½Ð¾Ð³Ð¾ Ð´Ð¸Ð¿Ð¾Ð»Ñ-Ð´Ð¸Ð¿Ð¾Ð»ÑÐ½Ð¾Ð³Ð¾ Ð²Ð·Ð°Ð¸Ð¼Ð¾Ð´ÐµÐ¹ÑÑÐ²Ð¸Ñ Ð½Ð° Ð¿ÑÐ¾ÑÐµÑÑ ÑÐ°ÑÐ¿ÑÐ¾ÑÑÑÐ°Ð½ÐµÐ½Ð¸Ñ Ð¸Ð·Ð»ÑÑÐµÐ½Ð¸Ñ Ð² Ð¿Ð»Ð¾ÑÐ½Ð¾Ð¼ Ð¿ÑÐ¾ÑÑÑÐ°Ð½ÑÑÐ²ÐµÐ½Ð½Ð¾ Ð½ÐµÑÐ¿Ð¾ÑÑÐ´Ð¾ÑÐµÐ½Ð½Ð¾Ð¼ Ð°ÑÐ¾Ð¼Ð½Ð¾Ð¼ Ð°Ð½ÑÐ°Ð¼Ð±Ð»Ðµ
title: Ð²ÑÐ¿ÑÑÐºÐ½Ð°Ñ ÐºÐ²Ð°Ð»Ð¸ÑÐ¸ÐºÐ°ÑÐ¸Ð¾Ð½Ð½Ð°Ñ ÑÐ°Ð±Ð¾ÑÐ° Ð±Ð°ÐºÐ°Ð»Ð°Ð²ÑÐ°
titleType: Subtitle
Creators: name: ÐÑÐ½ Ð¥ÑÑÐ¹
Publisher: name: Ð¡Ð°Ð½ÐºÑ-ÐÐµÑÐµÑÐ±ÑÑÐ³ÑÐºÐ¸Ð¹ Ð¿Ð¾Ð»Ð¸ÑÐµÑÐ½Ð¸ÑÐµÑÐºÐ¸Ð¹ ÑÐ½Ð¸Ð²ÐµÑÑÐ¸ÑÐµÑ ÐÐµÑÑÐ° ÐÐµÐ»Ð¸ÐºÐ¾Ð³Ð¾
Year: 2021
Subjects: Ð´Ð¸Ð¿Ð¾Ð»Ñ-Ð´Ð¸Ð¿Ð¾Ð»Ð½Ð¾Ðµ Ð²Ð·Ð°Ð¸Ð¼Ð¾Ð´ÐµÐ¹ÑÑÐ²Ð¸Ðµ
Ñ Ð¾Ð»Ð¾Ð´Ð½ÑÐ¹ Ð°ÑÐ¾Ð¼
ÑÐ²ÐµÑÐ´ÑÐ¹ Ð´Ð¸ÑÐ»ÐµÐºÑÑÐ¸Ðº
ÐºÐ¾ÑÑÑÐ¸ÑÐ¸ÐµÐ½Ñ Ð¿ÑÐ¾Ð¿ÑÑÐºÐ°Ð½Ð¸Ñ
Ð°Ð¼Ð¿Ð»Ð¸ÑÑÐ´Ñ ÑÐ¾ÑÑÐ¾ÑÐ½Ð¸Ð¹
ÑÑÐ°ÑÐ¸Ð¾Ð½Ð°ÑÐ½Ð¾Ðµ Ð²Ð¾Ð·Ð±ÑÐ¶Ð´ÐµÐ½Ð¸Ðµ
ÐºÐ²Ð°Ð·Ð¸ÑÐµÐ·Ð¾Ð½Ð°Ð½ÑÐ½ÑÐ¹ ÑÐ²ÐµÑ
ÑÐ¾Ð»ÑÐ¸Ð½Ð° ÑÑÐµÐ´Ñ
dipole-dipole interaction
cold atom
solid dielectric
transmission coefficient
amplitudes of states
stationary excitation
quasi-resonant light
medium thickness

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description: The given work is devoted to the study of the influence of the dipole-dipole interaction between atoms on the propagation of radiation in a densely located disordered atomic ensemble, the general goal is to create a theory and calculate the transmission coefficient for a specific problem. The general theory of this work mainly uses basic methods and approximate techniques to solve related problems. The amplitude of the state is introduced. In a closed unified system based on the wave function of the nonstationary Schrodinger equation, the Hamiltonian and the dipole approximation are used considering the atomic system and the system of combined fields. Then the Fourier transform is used to obtain a finite system of linear algebraic equations, calculate the integral, derivative, sum of polarization, obtain the reradiation matrix , and then obtain an expression for the amplitude of the atomic state. We use the passage to the limit, that is, the width of the transition line tends to zero, and the time tends to infinity, and the description of the quasi-static state is obtained using two limit transitions. We use an atomic detector transmittance calculation, an âatom detectorâ only picks up light, but does not emit it back. We set the horizontal dimensions for A and B, then adjust the size of the average thickness C and observe the average intensity of the transmitted light. From the data, we know that as the thickness of the medium C increases, our average value converges, and at At the same time, we plot the transmittance versus the thickness of the medium, T (C), where A = 10, B = 10. It can be seen that the dependence f (C) goes beyond the growth constant of the thickness of the medium. is inversely proportional to the thickness of the medium. In the course of the work, the problem of calculating the quantum-mechanical amplitude of a single excited state of an atom in a dense and disordered set of arbitrary spatial configuration was solved, and the method for calculating the intensity of scattered radiation at any point was analyzed. The medium is statically excited by external monochromatic light, and the calculation is performed in space. The transmittance of quasi-resonant light is calculated by the atomic detector method, we came to the conclusion that with an increase in the thickness of the sample, the dependence of the transmission on the thickness of the medium approaches hyperbolic asymptotics, that is, the transmission and dense atomic assembly has a diffusion property.