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Physical and mathematical model of the digital coherent optical spectrum analyser

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Warianty tytułu
Języki publikacji
EN
Abstrakty
EN
A physical and mathematical model of digital coherent optical spectrum analyzers is discussed. In digital coherent optical spectrum analyzers the input signal is forming as a two-dimensional transparency by means of a spatial light modulator. After Fourier transformation with a lens, multiplication by a spatial filter and second Fourier transformation, the signal is captured by a matrix detector for further computer processing. A lot of digital coherent optical spectrum analyzers and their components (laser, lighting system, spatial light modulator, Fourier lens and matrix detector) models were developed to calculate the signal at the matrix detector output. They use the impulse response and transfer function to evaluate the effectiveness of digital coherent optical spectrum analyzers. The analysis of mathematical relationships shows that the use of a discrete spatial light modulator for the signal input and a matrix detector for light field registration in the spectral domain when combined with computer technology greatly extends the functionality of digital coherent optical spectrum analyzer. The formulas for impulse response and transfer function calculations were obtained, which allows to analyze and optimize the digital coherent optical spectrum analyzer basic characteristics.
Czasopismo
Rocznik
Strony
273--282
Opis fizyczny
Bibliogr. 13 poz., rys.
Twórcy
  • National Technical University of Ukraine “Kyiv Polytechnic Institute”, 37, Prosp. Peremohy, Kyiv, Ukraine, 03056
  • National Technical University of Ukraine “Kyiv Polytechnic Institute”, 37, Prosp. Peremohy, Kyiv, Ukraine, 03056
  • National Technical University of Ukraine “Kyiv Polytechnic Institute”, 37, Prosp. Peremohy, Kyiv, Ukraine, 03056
  • National Technical University of Ukraine “Kyiv Polytechnic Institute”, 37, Prosp. Peremohy, Kyiv, Ukraine, 03056
Bibliografia
  • [1] STARK H. [Ed.], Applications of Optical Fourier Transforms, Academic Press, 1982.
  • [2] ZENKOVA C.YU., GORSKY M.P., SOLTYS I.V., ANGELSKY P.O., Use of motion peculiarities of test particles for estimating degree of coherence of optical fields, Ukrainian Journal of Physical Optics 13(4), 2012, pp. 183–195.
  • [3] CURATU G., HARVEY J.E., Analysis and design of wide-angle foveated optical systems based on transmissive liquid crystal spatial light modulators, Optical Engineering 48(4), 2009, article ID 043001.
  • [4] NEUYMIN O., DYACHENKO S., “CCD”, Visnyk NTUU “KPI”, Ser. Radiotekhnika, Radioaparatobuduvannya, No. 41, 2010, pp. 182–189.
  • [5] KOLOBRODOV V.G., TYMCHYK G.S., Analysis of optical systems of coherent spectrum analyzers, Rus. J. Opto-Mechanical Industry 10, 1982, pp. 4–7.
  • [6] SALEH B.E.A., TEICH M.C., Fundamentals of Photonics, Wiley, New York, 1991.
  • [7] KOLOBRODOV V.G., TYMCHYK G.S., Applied Diffractive Optics, Politekhnika, Kyiv, 2014.
  • [8] KOLOBRODOV V.G., TYMCHYK G.S., KOLOBRODOV M.S., Geometrical noise bandwidth of the optical spectrum analyzer, Ukr. J. Visnik Kremenchuk Mykhailo Ostohradskyi National University 5, 2015, pp. 50–55.
  • [9] KLIMKOV YU.M., Bases of Calculation of Optoelectronic Devices with Lasers, Sovetskoe Radio, Moscow, 1978.
  • [10] BOGATYIREVA V.V., DMITRIEV A.L., Optical Methods of Information Processing, ITMO University, St. Petersburg, 2009.
  • [11] KOLOBRODOV V.G., TYMCHYK G.S., QUYNH ANH, Defining generalized characteristics of coherent spectrum ANALYZER, Ukr. J. Naukovi visti NTUU “KPI”, No. 5, 2012, pp. 102–108.
  • [12] BURALLI D.A., MORRIS G.M., Design of a wide field diffractive landscape lens, Applied Optics 28(18), 1989, pp. 3950–3959.
  • [13] KOLOBRODOV V.G., TYMCHYK G.S., KOLOBRODOV M.S., Coherent Optical Spectrum Analyzer: Monograph, Politekhnika, Kyiv, 2015.
Uwagi
Opracowanie ze środków MNiSW w ramach umowy 812/P-DUN/2016 na działalność upowszechniającą naukę (zadania 2017).
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-6fbc6036-b4eb-4067-bfd3-70f8d0667b64
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