Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency

This research presents the results of investigation of laser polarization fluorescence of biological layers (histological sections of the myocardium). The polarized structure of autofluorescence imaging layers of biological tissues was detected and investigated. Proposed in this work is the model fo...

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Datum:2015
Hauptverfasser: Dubolazov, O.V., Sidor, M.I., Karachevtsev, A.O.
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Veröffentlicht: Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України 2015
Schriftenreihe:Semiconductor Physics Quantum Electronics & Optoelectronics
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spelling irk-123456789-1218082017-06-19T03:02:43Z Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency Dubolazov, O.V. Sidor, M.I. Karachevtsev, A.O. This research presents the results of investigation of laser polarization fluorescence of biological layers (histological sections of the myocardium). The polarized structure of autofluorescence imaging layers of biological tissues was detected and investigated. Proposed in this work is the model for describing formation of polarization inhomogeneity in autofluorescent images of biological optically anisotropic layers. On its basis, analytically and experimentally tested is the method of laser autofluorescent polarimetry. Analyzed has been the effectiveness of this method in the postmortem diagnosis of infarction. The objective criteria (statistical moments) of differentiation of autofluorescent images of histological sections myocardium have been determined. The operational characteristics (sensitivity, specificity, accuracy) of this technique have been ascertained. 2015 Article Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency / O.V. Dubolazov, M.I. Sidor, A.O. Karachevtsev // Semiconductor Physics Quantum Electronics & Optoelectronics. — 2015. — Т. 18, № 2. — С. 152-157. — Бібліогр.: 28 назв. — англ. 1560-8034 DOI: 10.15407/spqeo18.02.152 PACS 87.50.wp, 87.57.-s, 87.64.-t, 87.85.Pq http://dspace.nbuv.gov.ua/handle/123456789/121808 en Semiconductor Physics Quantum Electronics & Optoelectronics Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description This research presents the results of investigation of laser polarization fluorescence of biological layers (histological sections of the myocardium). The polarized structure of autofluorescence imaging layers of biological tissues was detected and investigated. Proposed in this work is the model for describing formation of polarization inhomogeneity in autofluorescent images of biological optically anisotropic layers. On its basis, analytically and experimentally tested is the method of laser autofluorescent polarimetry. Analyzed has been the effectiveness of this method in the postmortem diagnosis of infarction. The objective criteria (statistical moments) of differentiation of autofluorescent images of histological sections myocardium have been determined. The operational characteristics (sensitivity, specificity, accuracy) of this technique have been ascertained.
format Article
author Dubolazov, O.V.
Sidor, M.I.
Karachevtsev, A.O.
spellingShingle Dubolazov, O.V.
Sidor, M.I.
Karachevtsev, A.O.
Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency
Semiconductor Physics Quantum Electronics & Optoelectronics
author_facet Dubolazov, O.V.
Sidor, M.I.
Karachevtsev, A.O.
author_sort Dubolazov, O.V.
title Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency
title_short Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency
title_full Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency
title_fullStr Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency
title_full_unstemmed Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency
title_sort statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency
publisher Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України
publishDate 2015
url http://dspace.nbuv.gov.ua/handle/123456789/121808
citation_txt Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency / O.V. Dubolazov, M.I. Sidor, A.O. Karachevtsev // Semiconductor Physics Quantum Electronics & Optoelectronics. — 2015. — Т. 18, № 2. — С. 152-157. — Бібліогр.: 28 назв. — англ.
series Semiconductor Physics Quantum Electronics & Optoelectronics
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AT sidormi statisticalandfractalanalysesofautofluorescenceofmyocardiumtissueimagesindiagnosticsofacutecoronaryinsufficiency
AT karachevtsevao statisticalandfractalanalysesofautofluorescenceofmyocardiumtissueimagesindiagnosticsofacutecoronaryinsufficiency
first_indexed 2025-07-08T20:33:22Z
last_indexed 2025-07-08T20:33:22Z
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fulltext Semiconductor Physics, Quantum Electronics & Optoelectronics, 2015. V. 18, N 2. P. 152-157. doi: 10.15407/spqeo18.02.152 © 2015, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 152 PACS 87.50.wp, 87.57.-s, 87.64.-t, 87.85.Pq Statistical and fractal analyses of autofluorescence of myocardium tissue images in diagnostics of acute coronary insufficiency O.V. Dubolazov, M.I. Sidor, A.O. Karachevtsev Chernivtsi National University, Optics and Publishing Department, 2, Kotsyubinsky str., 58012 Chernivtsi, Ukraine E-mail: a.dubolazov@chnu.edu.ua Abstract. This research presents the results of investigation of laser polarization fluorescence of biological layers (histological sections of the myocardium). The polarized structure of autofluorescence imaging layers of biological tissues was detected and investigated. Proposed in this work is the model for describing formation of polarization inhomogeneity in autofluorescent images of biological optically anisotropic layers. On its basis, analytically and experimentally tested is the method of laser autofluorescent polarimetry. Analyzed has been the effectiveness of this method in the postmortem diagnosis of infarction. The objective criteria (statistical moments) of differentiation of autofluorescent images of histological sections myocardium have been determined. The operational characteristics (sensitivity, specificity, accuracy) of this technique have been ascertained. Keywords: autofluorescence, polarization, birefringence, dichroism, statistical optics, diagnostics, autofluorescence imaging, histological sections of the myocardium. Manuscript received 17.11.14; revised version received 27.02.15; accepted for publication 27.05.15; published online 08.06.15. 1. Introduction Biological tissues represent structurally heterogeneous optical anisotropic media with absorption. To describe interactions of polarized light with these complex systems more generalized approximations are required based on Mueller-matrix formalism. Nowadays, many practical techniques based on the measurement and analysis of Mueller matrices of the investigated samples are applied to biological and medical researches [1-5]. A separate direction – laser polari- metry – was formed in matrix optics in recent 10-15 years [6-10]. On its base, interrelations between the set of statistical moments of the 1 st to 4 th orders were determined, which characterize the distributions of Mueller-matrix elements, and the parameters of linear birefringence of fibrillar protein networks in human biological tissues. Using them, diagnostics of pathological changes in skin derma, epithelial and connective tissues of women’s reproductive sphere organs, etc., has been realized [11-24]. New step in the development of optical diagnostics methods of biological objects is a combination of polarimetry and fluorescence methods [25]. This work is focused on research of interrelation between optical anisotropy of histological sections taken from myocardium and polarization structure of posthumous autofluorescent images in diagnostics of coronary heart disease (CHD) and acute coronary insufficiency (ACI). Semiconductor Physics, Quantum Electronics & Optoelectronics, 2015. V. 18, N 2. P. 152-157. doi: 10.15407/spqeo18.02.152 © 2015, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 153 2. Brief theory In this work, we have limited ourselves by considering the spectral-selective case – luminescence of optically active porphyrins of biological layers in the red (λf = 0.63…0.65 μm) spectral range [25]. The excitation of autofluorescence was realized by a blue solid-state laser with the wavelength λ = 0.405 μm that coincides with the porphyrin’s absorption peak. The following model ideas concerning optical anisotropy of optically thin (extinction coefficient 1.0 ) and non-polarizing biological layers are used as the basis for description of laser polarization autofluorescence of biological tissues. 2.1. Absorption – Amino acids and polypeptide chains (primary structure of protein) made by them form the fibrillar (secondary structure) protein networks possessing the linear dichroism. This absorption has liquid crystalline networks of endogenous porphyrins associated with protein molecules. Availability of complex spiral-like structures or their combinations (third-order structure) of polypeptide protein structures forms the circular dichroism. This mechanism is inherent to optically active porphyrin molecules. 2.2. Fluorescence – Polarization appearance of porphyrin fluorescence is characterized by Mueller- matrix adduced in [25-28]   44 33 2221 12 000 000 00 001 F F FF F F  , where                   .cos2 ,cos2 ,cos1 ,sin ,sin 44 33 2 22 2 2112 2 11 1 11 cF bF bF bFF baF FFik (1) Here,  is the scattering angle; a and b are the interrelated constants for the system of linear oscillators in isotropic medium, defined by following relations:   2cos15.0a , (2)  1cos325.0 2 b , (3) where ε is the angle between the emissive dipole and azimuth of polarization inherent to the exciting beam. The parameter c is undoubtedly related with optical activity. From the classical viewpoint, a “circular oscillator” would be caused by the induced electric and magnetic transition dipole moments being fully parallel or antiparallel and having the same magnitude. Following this description, optically active liquid-crystal molecules are “elliptical oscillators”. 2.3. Phase modulation of fluorescence. Amino acids and polypeptide chains made by them (primary structure of protein) demonstrate optical activity. Fibrillar (secondary structure) protein networks formed by polypeptide chains possess linear birefringence. Considering the effect of all mechanisms of optically anisotropic absorption and phase anisotropy, the Mueller matrix of laser polarization autofluorescence of the protein network in biological tissue can be written as follows:         44434241 34333231 24232221 1413121 MMMM MMMM MMMM MMM FDM  . (4) The analysis of matrix (4) shows that elements Mik characterize superposition of mechanisms of linear Δτ and circular Δg dichroism; fluorescence of linear F12;21;22;33 and elliptical F44 oscillators with the following phase modulation of this radiation by optically active molecules θ and birefringent δ networks of them. The “information content” of matrix elements is different. The set of elements  124;3;2;1;1 FM ki  characterizes the fluorescence of linear oscillators originated due to the anisotropic absorption. The elements  33;22;214;3;2;1;3;2 FM ki  define the phase- modulated (δ, θ) fluorescence of linear oscillators. Finally, the values of elements  4433;22;214;3;2;1;4 ,FFM ki  contain complex information concerning fluorescence of linear (F21;22;33) and elliptical (F44) oscillators in optically anisotropic medium with linear and circular birefringence. The process of forming the polarization structure of the autofluorescence image can be described by the vector parametric equation [14]   0SMS  . (5) Here S0, S are the Stokes vectors of probing (illuminating) and autofluorescence (polarization modulated) radiation. From (5), we obtain expressions for the autofluo- rescence polarization parameters   , : 2421 3431arctg5.0 MM MM    , (6) 14 4441 1 arcsin5.0 M MM    . (7) 3. Analysis and discussion of experimental results 3.1. Measuring the distributions of autofluorescence images polarization parameters Experimental measurements were performed in the set of Stokes polarimeter [14] with the use of spectrally selective band-pass light filters (Fig. 1). Semiconductor Physics, Quantum Electronics & Optoelectronics, 2015. V. 18, N 2. P. 152-157. doi: 10.15407/spqeo18.02.152 © 2015, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 154 Fig. 1. Optical scheme of Stokes-polarimeter. Explanations are in the text. To excite autofluorescence, we used the “blue” solid-state laser with the wavelength λ = 0.405 μm and variable power W (in this research we used W = 50 mW). A polarization illuminator consists of quarter-wave plates 3, 5 (Achromatic True Zero-Order Waveplate) and polarizer 4. The image of the myocardium 6 by means of polarization microscope objective 7 (Nikon CFI Achro- mat P, focal distance 30 mm, numerical aperture 0.1, magnification 4×) was projected in the plane of light- sensitive CCD-camera 11 (The Imaging Source DMK 41AU02.AS, monochrome 1/2" CCD, Sony ICX205AL (progressive scan), overall amount of pixels m×n = 1280×960, light sensitive area size 7600×6200 μm, sensitivity 0.05 lx, dynamic range 8 bit, deviation of photosensitive characteristics from the linear ones is no more than 12%). Polarization analysis of coordinate distribution of intensity from the sample 6 was carried out by means of quarter-wave plate 8 and polarizer 9. 3.2. Polarization autofluorescence biopsy As objects of investigation, two groups of optically thin (extinction coefficient τ ≈ 0.087…0.093) histological sections of biopsy taken from the myocardium inherent to two groups of patients with the following diagnoses: - group 1 – CHD; - group 2 – ACI. The potentiality of this technique is illustrated by the data presented in Figs. 2 and 3. Here, the polarization maps  nm ,  nm and histograms  G ,  G are presented. These data show (Figs. 2 and 3), that for all the histological sections of samples from both groups realized are various two-dimensional (fragments (1), (3)) and statistical (fragments (2), (4)) distributions of polarization parameters of autofluorescent images. The comparative analysis of polarization maps for autofluorescent images of histological layers of myocardium revealed certain difference between them. The histograms  G of the histological section of ACI are characterized by asymmetric structure (Fig. 2, fragments (2), (4)). For ACI process detected by the following changes of    4;3;2;1iZ , there is the decrease of mean Z1 and dispersion Z2 of histograms  G . Statistical moments (skewness 3Z , kurtosis 4Z ) are increased. For coordinate distributions of the polarization ellipticity  nm , autofluorescence images found that the halfwidth of distributions  G for the sample of the group 2 is 1.5 times higher than the histogram for the group 1 sample (Fig. 3, fragments (2), (4)). This transformation of the statistical structure of the polarization ellipticity is accompanied by following changes of    4;3;2;1iZ – 1Z , 2Z , 3Z , 4Z . 3.3. Statistical intergroup analysis The diagnosis of CHD (group 1) and ACI (group 2) was determined by the gold standard method. By means of software product Statmate for 95% confidence interval ( 05.0p ) a reliable quantity of people was determined – n = 52. Fig. 2. Polarization maps of azimuth autofluorescence imaging of myocardium with CHD ((1), (2)) and ACI ((3), (4)). Semiconductor Physics, Quantum Electronics & Optoelectronics, 2015. V. 18, N 2. P. 152-157. doi: 10.15407/spqeo18.02.152 © 2015, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 155 Fig. 3. Polarization maps of ellipticity autofluorescence imaging of myocardium with CHD ((1), (2)) and ACI ((3), (4)). Determined within each group of samples are:  averages of statistical moments  qZi 4;3;2;1 , their standard deviations  and histograms  iZN – Tables 1 and 2.  traditional characteristics for demonstrative medicine operational – sensitivity %100 ba a Se   , specificity %100 dc c Sp   and balanced accuracy 2 SpSe Ac   , where a and b are the numbers of correct and incorrect diagnoses within the group 2; c and d are the same in the group 1 – Tables 3 and 4. Table 1. Average    4;3;2;1iZ and standard deviations ±σ statistical moments Zi =1;2;3;4 of polarization maps of azimuth autofluorescence images distributions. Parameters Myocardium (n1 = n2= 52) Group 1 Group 2 Z1 1.31±0.29 1.13±0. 23 Z2 0.92±0.15 0.86±0.14 Z3 1.18±0.21 1.61±0.39 Z4 0.94±0.14 1.23±0.27 Table 2. Average    4;3;2;1iZ and standard deviations ±σ statistical moments Zi =1;2;3;4 of polarization maps of ellipticity autofluorescence images distributions. Parameters Myocardium (n1 = n2= 52) Group 1 Group 2 Z1 0.33±0.056 0.37±0.061 Z2 0.46±0.11 0.64±0.15 Z3 0.81±0.16 0.72±0.14 Z4 1.61±0.39 1.16±0.24 Table 3. Operational characteristics of the autofluorescence laser polarimetry azimuths method. Zi Biopsy (n1 = n2= 52) Ac (Zi),% Z1 59.6 a = 32, b = 20 c = 30, d = 22 Z2 58.65 a = 31, b = 21 c = 30, d = 22 Z3 85.55 a = 45, b = 7 c = 44, d = 8 Z4 86.55 a = 46, b = 6 c = 44, d = 8 Table 4. Operational characteristics of the autofluorescence laser polarimetry ellipticity method. Zi Biopsy (n1 = n2= 52) Ac (Zi),% Z1 55.75 a = 30, b = 22 c = 28, d = 24 Z2 88.3 a = 47, b = 5 c = 45, d = 7 Z3 59.6 a = 32, b = 20 c = 30, d = 22 Z4 90.4 a = 48, b = 4 c = 46, d = 6 The following quantitative difference between     ,4;3;2;1iZ was determined – the difference between statistical moments 4;3;2;1iZ         .39.1,13.1,39.1,12.1 ;31.1,36.1,07.1,16.1 4321 4321 ZZZZ ZZZZ The obtained results suggest a rather high level of accuracy obtained using this method. According to the criteria of demonstrative medicine parameters are    %85~4;3 ZAc ,   %90~4;3 ZAc . Semiconductor Physics, Quantum Electronics & Optoelectronics, 2015. V. 18, N 2. P. 152-157. doi: 10.15407/spqeo18.02.152 © 2015, V. Lashkaryov Institute of Semiconductor Physics, National Academy of Sciences of Ukraine 156 4. Conclusions 1. 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