
{"id":3239,"date":"2016-05-12T20:58:55","date_gmt":"2016-05-12T16:58:55","guid":{"rendered":"http:\/\/www.ire.kharkov.ua\/?page_id=3239"},"modified":"2016-05-12T21:25:22","modified_gmt":"2016-05-12T17:25:22","slug":"radiophysics-and-electronics","status":"publish","type":"page","link":"https:\/\/www.ire.kharkov.ua\/en\/radiophysics-and-electronics.html","title":{"rendered":"Radiophysics and Electronics"},"content":{"rendered":"<p><\/p>\n<div class=\"Section1\">\n<p class=\"MsoFooter18\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\">2016,<br \/>\nVol.\u00a07(21), \u2116 1<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\">\u00a0<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\">\u00a0<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\">\u00a0<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">ENERGY CHARACTERISTICS OF A RECTANGULAR WAVEGUIDE<br \/>\nT-JUNCTION INTERACTING WITH A MULTIELEMENT VIBRATOR-SLOT COUPLING STRUCTURE<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">S.\u00a0L.\u00a0Berdnik,<br \/>\nV.\u00a0A.\u00a0Katrich, V.\u00a0I.\u00a0Kiyko, M.\u00a0V.\u00a0Nesterenko,<br \/>\nYu.\u00a0M.\u00a0Penkin<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">4-14<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">The study of peculiarity of influence of the impedance<br \/>\ninsertions on the electrodynamic characteristics of the<\/span> <span lang=\"EN-US\" style=\"font-size: 10.0pt;\">rectangular<br \/>\nwaveguide junctions,<\/span> <span lang=\"EN-US\" style=\"font-size: 10.0pt;\">which are widely used in the<br \/>\nantenna-waveguide devices, is important for practical applications. A<br \/>\nmathe-matical model for <i>E<\/i>-plane T-junction<\/span> <span lang=\"EN-US\" style=\"font-size: 10.0pt;\">of<br \/>\nrectangular waveguides with a three-element vibrator-slot coupling structure<br \/>\nwas built using approximate analytical solutions of equations for induced<br \/>\ncurrents by a generalized method of electro-magneto-motive forces. The<br \/>\ndistinctive feature of the model is the usage of variable surface impedance<br \/>\nalong the monopole axes and constant impedance, distributed over the end wall<br \/>\nof the <\/span><span lang=\"UK\" style=\"font-size: 10.0pt;\">lateral<\/span><span lang=\"EN-US\" style=\"font-size: 10.0pt;\"> semi-infinite waveguide. Multiparameter<br \/>\nenergy characteristics of the junction in the single-mode waveguides are<br \/>\npresented including the case of meta-material coating the end wall of the<br \/>\nlateral waveguide. The possibility of efficient use of impedance coatings as<br \/>\ncontrol element for power division between the output waveguide junction arms<br \/>\nis shown.<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">REFLECTION RESONANCES IN A RECTANGULAR WAVEGUIDE<br \/>\nSECTION WITH A PAIR OF ANTIPODAL RECTANGULAR POSTS<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">L.\u00a0P.\u00a0Mospan,<br \/>\nS.\u00a0A.\u00a0Prikolotin, \u0410.\u00a0\u0410.\u00a0\u041airilenko<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">15-21<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">Intentional and controllable introduction of<br \/>\nattenuation poles into the frequency responses of frequency-selective devices<br \/>\nis in the great demand in the design of modern filters with complicated<br \/>\nperformance. Successful implementation of such an approach is possible using<br \/>\nrectangular waveguide sections with metallic inserts. Here, the scattering<br \/>\ncharacteristics of such sections with a pair of antipodal rectangular posts as<br \/>\nwaveguide units with rotational symmetry are studied. Comparative analysis with<br \/>\nthe characteristics of a section with a pair of unidirectional posts is performed.<br \/>\nSpectral theory of open waveguide resonators is used in order to interpret the<br \/>\nresonant phenomena. Within the frames of spectral theory the reflection<br \/>\nresonances formed by such sections are the responses to the excitation of eigen<br \/>\noscillations of complex frequencies. It is shown that the spectral theory<br \/>\nenables an order of magnitude more accurate (in comparison with the<br \/>\nconventional modal analysis) evaluation for basic parameters of the resonance<br \/>\nreflection, namely its frequency and the quality factor. The results obtained<br \/>\nmake preliminary synthesis of frequency selective devices based on such<br \/>\nsections physically transparent and more accurate.<\/span><\/p>\n<p class=\"MsoFooter18\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoFooter18\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">RADAR<\/span><\/b><b> <\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">ELEVATION<br \/>\nANGLES MEASUREMENTS OF LOW-ALTITUDE TARGETS OVER THE SEA BY ROOT-MUSIC<\/span><\/b><b> <\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">METHOD UNDER INTERFERENCE FROM MULTIPATH AND THERMAL<br \/>\nNOISE <\/span><\/b><b><span style=\"font-size: 10.0pt;\">\u041e<\/span><\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">F DIRECTION FINDER<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">Yu.\u00a0A.\u00a0Pedenko<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">22-30<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">The work is devoted to improvement of the accuracy of<br \/>\nradar measurements of elevation angles of low-altitude targets above sea level<br \/>\nwhen using the <i>root-MUSIC<\/i>, which is considered by experts as one of the<br \/>\nmeans to solve this problem. Unlike previous studies, which take into account<br \/>\nthe multipath only, in this study the clutter is complicated by thermal noise<br \/>\nof radar. This allows to evaluate the capabilities of the method and provide<br \/>\nguidance on its application in the conditions close to reality. The study was<br \/>\ncarried out by computer simulation. It covered various sea states at which the<br \/>\nconditions from specula to strong diffuse reflection were complied. In the<br \/>\nsimulation a wide range of signal\/noise ratio was used. The main focus was the<br \/>\nstudy of effects on measurement errors of a priori parameters of the method:<br \/>\nthe signal subspace dimension and the order of autocorrelation matrix of<br \/>\nsignals received by a multi-element antenna array. The recommendations of their<br \/>\nchoice, allowing to minimize the errors of elevation measurement in different<br \/>\nconditions, have been developed. The results of the study extend the knowledge<br \/>\nof how to improve the methods for measuring the target elevation angle above<br \/>\nthe sea.<\/span><\/p>\n<p class=\"MsoFooter18\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoFooter18\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"UK\" style=\"font-size: 10.0pt;\">RESEARCH <\/span><\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">ON<\/span><\/b><b><span lang=\"UK\" style=\"font-size: 10.0pt;\"> THE UNDERLYING SURFACE BY RADIATION OF GLOBAL NAVIGATION SATELLITE SYSTEM<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">V. I. Lutsenko, D. O. Popov, I. V. Lutsenko<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">31-39<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">The investigation of the scattering signals features<br \/>\non the land surface can be used to study the physics of scattering processes,<br \/>\nas well as for the establishment of multipath compensation methods for reducing<br \/>\npositioning errors in global navigation satellite systems. The possibility of<br \/>\ndetecting the reflection areas on the underlying surface and estimating their<br \/>\nparameters by using radiation of global navigation satellite systems is shown.<br \/>\nThe behavior of the signal levels for different satellites in urban areas is<br \/>\nanalyzed. The influence of the reflection area\u2019s characteristics on the<br \/>\nspectrum of the received radiations is considered; the method of determining<br \/>\ntheir location is proposed.<\/span><\/p>\n<p class=\"MsoFooter18\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoFooter18\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"UK\" style=\"font-size: 10.0pt;\">R<\/span><\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">ADIANT<\/span><\/b><b><span lang=\"UK\" style=\"font-size: 10.0pt;\"> S<\/span><\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">YSTEM<\/span><\/b><b> <\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">BASED<\/span><\/b><b> <\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">ON<\/span><\/b><b> <\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">COLD<\/span><\/b><b> <\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">PLASMA<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">V. V. Ovsyanikov<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">40-47<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">The actual problem of studying the basic properties and searching for methods<br \/>\nof improving the plasma radiator array, which is similar to the array of metal<br \/>\nor dielectric antennas, has been considered. This problem is not sufficiently<br \/>\ncovered in the well-known publications, however, the great interest of<br \/>\nprofessionals to emitters based on cold plasma is due to the prospect of<br \/>\ncreating effective multi-beam scanning selective plasma reconfigurable systems<br \/>\nor the plasma array of radiators (PAR). The article studies the main<br \/>\nelectrodynamics parameters of PAR in the microwave range, characterizing it on<br \/>\nthe one hand, as the load for the generator (receiver) of electromagnetic (EM)<br \/>\nsignal. On the other hand, PAR is tested as transmitter of EM energy from the<br \/>\npoint of view of its direction pattern (DP) and the main parameters of<br \/>\nradiation of PAR. When scanning DP beam, impedance distortion of PAR<br \/>\ntransmitters and DP deformation are investigated. For comparison, similar<br \/>\nstudies were carried out for the same design and configuration of the pattern<br \/>\nantenna (PA) of metal antennas. The studies have been carried out by PAR<br \/>\nmodeling and their parameters calculations on computer in software environment<br \/>\nFEKO by integral equation method and method of moments for linear PAR from 4<br \/>\nemitters in the form of loop dielectric tubes filled with cold plasma under<br \/>\nreduced pressure. When studying the self and mutual impedances of the PAR and<br \/>\nmetal PA in common mode for the distance between the transmitters 0.5\u03bb<sub>0<\/sub>, where \u03bb<sub>0<\/sub> is the central wavelength<br \/>\nof the test range, it has been determined that electromagnetic interference<br \/>\nbetween antennas in PAR is less than in the metal antenna array, and when<br \/>\nreducing the distance between transmitters grating with 0.5\u03bb<sub>0<\/sub> \u2013 0.25\u03bb<sub>0<\/sub> the relative change in<br \/>\nvalue of units of the input impedance of each radiator of PAR is twice less<br \/>\nthan for a lattice of aluminum, which allows to bring together the radiator of<br \/>\nPAR without a substantial increase in interference between them. From<br \/>\ncomparison of DP of radiant systems of PAR and aluminum arrays while scanning,<br \/>\nit is obvious that DP of PAR are less distorted than aluminum array. The<br \/>\nobtained results can be used for calculations and design of plasma array of<br \/>\nradiators.<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">PLASMA-BEAM SUPERHETERODYNE FREE ELECTRON LASER WITH <i>H<\/i>-UBITRON<br \/>\nPUMP WITH NON-AXIAL INJECTION OF ELECTRON BEAM<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">A. V.\u00a0Lysenko, G. A.\u00a0Oleksiienko<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">48-54<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify; text-autospace: none;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">A cubic-nonlinear theory of a plasma-beam<br \/>\nsuperheterodyne free electron laser (PBSFEL) with H-ubitron pump and non-axial<br \/>\ninjection of electron beam has been constructed. In the investigated system the<br \/>\nparametric resonance interaction between a space-charge wave and cyclotron wave<br \/>\nis realized. The signal wave saturation levels have been determined. It has<br \/>\nbeen found that the mode using a slow cyclotron wave has the highest saturation<br \/>\nlevel among all possible operation modes of the PBSFEL with <i>H<\/i>-ubitron<br \/>\npump. The injection angle of the beam at which the electromagnetic signal gain<br \/>\nis maximal has been determined. It has been shown that PBSFELs using slow<br \/>\ncyclotron waves are able to create a powerful coherent electromagnetic<br \/>\nradiation in the millimeter wavelength range.<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoFooter18\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">OPERATING MODES OF AVALANCHE-GENERATOR DIODES OF<br \/>\nMICROWAVE RANGE<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">P. P. Maksymov<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">55-60<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify; text-autospace: none;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">Construction of powerful sources of<br \/>\nelectromagnetic oscillations of microwave range is an actual task for creating<br \/>\nmodern semiconductor devices. In this paper the creation of powerful sources of<br \/>\nelectromagnetic oscillations based on reverse-biased abrupt <i>p\u2013n<\/i>-junctions<br \/>\nof avalanche-generator diodes (AGD) with external signal has been theoretically<br \/>\ngrounded. Classification of modes of avalanche-generator diodes has been<br \/>\ncarried out. The choice of oscillations generation mode is determined by the<br \/>\nparameters of AGD and input signal. It is shown that coherent, multifrequency<br \/>\nand broadband oscillations are generated in AGD. Power and spectral<br \/>\ndescriptions of oscillations of AGD are presented. The research results are of<br \/>\ninterest for the developers of powerful diode generators with the required<br \/>\nrange, power and spectral characteristics.<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">THREE-CHANNEL PHASE METERS BASED ON THE <i>AD<\/i>8302<br \/>\nAND <span class=\"translation-chunk\">FIELD PROGRAMMABLE GATE ARRAYS <\/span>FOR<br \/>\nHETERODYNE MILLIMETER WAVE INTERFEROMETER<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">A. V. Varavin, G. P. Ermak, A. S. Vasilev, A.<br \/>\nS. Fateev, N. Varavin, F. Zacek, J. Zajac<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">61-70<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify; text-autospace: none;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">The paper presents the results of research<br \/>\nand development of two types of phase meters for heterodyne two-wave<br \/>\n\u201cunambiguous\u201d interferometer designed to measure the plasma density in tokamak <i>COMPASS.<\/i> The aim of this work is the creation of a phase meter capable of measuring fast<br \/>\nphase changes of each probing wave, and their phase difference. Plasma is<br \/>\nprobed by two microwave signals with different wavelengths propagating along<br \/>\nidentical paths to meet each other. Each analyzed signal acquires a certain phase<br \/>\nshift \u03c6<sub>1<\/sub> and \u03c6<sub>2<\/sub>, and the \u201cunambiguous\u201d interferometer<br \/>\ndetermines the difference (\u03c6<sub>1<\/sub>\u2013\u03c6<sub>2<\/sub>). The phase measurement is carried out by using<br \/>\nthree-channel phase meters: a phase meter based on the pairs of the <i>AD<\/i>8302<br \/>\nand a phase meter based on field programmable gate arrays (<i>FPGA<\/i>). The<br \/>\nproposed circuit decisions and algorithms of signal processing allow to measure<br \/>\nphases in the range 0\u2026360\u00b0 in real time.<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoFooter18\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">ELECTROMECHANICAL RESONATOR UNDER THE INFLUENCE OF<br \/>\nTELEGRAPH <\/span><\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">UNBALANCED NOISE<br \/>\nOF FREQUENCY<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">Z. \u0410. Maizelis<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">71-76<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify; text-autospace: none;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">For detecting and establishing the nature<br \/>\nof frequency noises in the oscillating system, it is very important to separate<br \/>\ndifferent types of noises. For determination of characteristics of the<br \/>\nfrequency noise it is necessary to study statistical properties not of actual<br \/>\ncoordinate and its derivative, but of complex coordinate of oscillator. Its<br \/>\nmoments do not depend on the amplitude noises that often can prevail in the<br \/>\nsystem. The growing interest in noises of frequency is related to the fact that<br \/>\nthey determine the loss of coherence of vibrations in many systems, from the<br \/>\ndevices based on Josephson contacts, to the nanomechanical resonators. The<br \/>\nknowledge of statistical characteristics of frequency noises inevitably present<br \/>\nin the devices of information read-out in quantum computers will allow correct<br \/>\nprocessing of the information in them. Here the influence of the telegraph<br \/>\nunbalanced noise of frequency on properties of electromechanical resonator is<br \/>\nstudied. It is shown that the dependencies of the higher cumulants contain<br \/>\nfeatures, which allow to separate the effects related to the presence of noise<br \/>\nof frequency. The results may be useful in the theory of nanomechanical<br \/>\nresonators, in processing the data, obtained in the radio-technical devices and<br \/>\ndevices, based on Josephson contacts, in quantum computers, in the estimation<br \/>\nof precision of atomic clock.<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">RECONSTRUCTION OF IMAGES WITH LARGE NON-UNIFORM<br \/>\nINCREMENTS<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">S. I. Melnyk, S. S. Melnyk<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">77-84<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify; text-autospace: none;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">In recent years, the range of tasks related<br \/>\nto the study of structures image elements of which are beyond the resolution of<br \/>\nmatrix type sensors is becoming wider. Thus, the problem of their<br \/>\nreconstruction by applying algorithmic and information image processing<br \/>\ntechniques is relevant. The problems emerging when observing objects whose<br \/>\ndimensions do not exceed several pixels of matrix of recorders have been<br \/>\nconsidered. It is shown that motion of the object relative to the matrix and<br \/>\nthe use of multiple consecutive frames allow to improve the fidelity of shape<br \/>\nand true size of the object. This measurement information can be represented as<br \/>\nintegrals along the trajectories on a three-dimensional lattice of space-time<br \/>\npixels. The reconstruction of a heterogeneity function of pixels through the<br \/>\nuse of the controlled motion of the test object and methods of computer<br \/>\ntomography. The possibility of determining the relative velocity of the object<br \/>\nin each of the frames using the blind method has been shown. The algorithm of<br \/>\nreconstructing images with large non-uniform increment during their arbitrary<br \/>\nand controlled relative motion has been elaborated.<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoNormal1\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">\u00a0<\/span><\/p>\n<p class=\"MsoFooter18\" style=\"text-align: center;\" align=\"center\"><b><span lang=\"UK\" style=\"font-size: 10.0pt;\">JITTER<\/span><\/b><b><span lang=\"EN-US\" style=\"font-size: 10.0pt;\"> OF <\/span><\/b><b><span lang=\"UK\" style=\"font-size: 10.0pt;\">SYNCHRONIZATION<br \/>\nOF THE STROBOSCOPIC CONVERTER<\/span><\/b><\/p>\n<p class=\"MsoNormal1\" style=\"margin-top: 6.0pt; text-align: center;\" align=\"center\"><i><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">V.\u00a0P.\u00a0Ruban<\/span><\/i><\/p>\n<p class=\"MsoFooter18\" style=\"margin-bottom: 6.0pt; text-align: right;\" align=\"right\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">85-91<\/span><\/p>\n<p class=\"MsoNormal1\" style=\"text-align: justify; text-autospace: none;\"><span lang=\"EN-US\" style=\"font-size: 10.0pt;\">The estimation of synchronization<br \/>\ninstability becomes actual in GPR due to the fact that this phenomenon affects<br \/>\nthe accuracy of recording and reproducing the received signal forms and,<br \/>\naccordingly, the efficiency of use of digital signal processing algorithms. The<br \/>\nexisting method for estimation of jitter of the GPR receiver using errors of<br \/>\nthe converted signal amplitude is not universal and should be corrected for the<br \/>\ncase of converter with incomplete charging of the storage capacitor. Simulation<br \/>\nof the stroboscopic conversion with instability of sampling interval for cases<br \/>\nof full charging (when the evaluation method gives correct results) and<br \/>\nincomplete charging of the storage capacitor has been done in this paper. The<br \/>\nrelationship between the forms of probabilistic distribution of jitter and<br \/>\nerrors of amplitude after stroboscopic conversion has been analyzed. The jitter<br \/>\nvalues originally specified in the simulation and the ones calculated<br \/>\n(reconstructed) by a known method also have been analyzed. According to the<br \/>\nsimulation results, the limits of applicability of this method were determined.<br \/>\nIt is shown that the direct application of the jitter evaluation method which<br \/>\nis right for the converter with a full charging gives incorrect estimates for<br \/>\nthe one with incomplete charging of storage capacitor. Due to this, the signal<br \/>\namplitude recovery procedure which allows obtaining a correct estimate of the<br \/>\njitter of synchronization of GPR receivers operating in the mode of incomplete<br \/>\ncharge storage capacitor has been suggested.<\/span><\/p>\n<\/div>\n<p><\/p>","protected":false},"excerpt":{"rendered":"<p>2016, Vol.\u00a07(21), \u2116 1 \u00a0 \u00a0 \u00a0 ENERGY CHARACTERISTICS OF A RECTANGULAR WAVEGUIDE T-JUNCTION INTERACTING WITH A MULTIELEMENT VIBRATOR-SLOT COUPLING STRUCTURE S.\u00a0L.\u00a0Berdnik, V.\u00a0A.\u00a0Katrich, V.\u00a0I.\u00a0Kiyko, M.\u00a0V.\u00a0Nesterenko, Yu.\u00a0M.\u00a0Penkin 4-14 The study of peculiarity of influence of the impedance insertions on the electrodynamic characteristics of the rectangular waveguide junctions, which are widely used in the antenna-waveguide devices, is [&hellip;]<\/p>\n","protected":false},"author":5,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-3239","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.ire.kharkov.ua\/en\/wp-json\/wp\/v2\/pages\/3239","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.ire.kharkov.ua\/en\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.ire.kharkov.ua\/en\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.ire.kharkov.ua\/en\/wp-json\/wp\/v2\/users\/5"}],"replies":[{"embeddable":true,"href":"https:\/\/www.ire.kharkov.ua\/en\/wp-json\/wp\/v2\/comments?post=3239"}],"version-history":[{"count":4,"href":"https:\/\/www.ire.kharkov.ua\/en\/wp-json\/wp\/v2\/pages\/3239\/revisions"}],"predecessor-version":[{"id":3243,"href":"https:\/\/www.ire.kharkov.ua\/en\/wp-json\/wp\/v2\/pages\/3239\/revisions\/3243"}],"wp:attachment":[{"href":"https:\/\/www.ire.kharkov.ua\/en\/wp-json\/wp\/v2\/media?parent=3239"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}