2002
DOI: 10.1103/physreve.65.046107
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Quantification of heart rate variability by discrete nonstationary non-Markov stochastic processes

Abstract: We develop the statistical theory of discrete nonstationary non-Markov random processes in complex systems. The objective of this paper is to find the chain of finite-difference non-Markov kinetic equations for time correlation functions (TCF) in terms of nonstationary effects. The developed theory starts from careful analysis of time correlation through nonstationary dynamics of vectors of initial and final states and nonstationary normalized TCF. Using the projection operators technique we find the chain of … Show more

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Cited by 51 publications
(91 citation statements)
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“…Considerable effort has gone into methods based on the assumption that, in view of the complexity of the activity of the autonomous nervous system, at least a major part of the variability of the heart rate may treated as a noise 4 driven process [6,7,8]. Most of these methods use fractal or multifractal scaling analysis [9]. The approach has also yielded stochastic models of heart rate variability [10,11].…”
Section: Introductionmentioning
confidence: 99%
“…Considerable effort has gone into methods based on the assumption that, in view of the complexity of the activity of the autonomous nervous system, at least a major part of the variability of the heart rate may treated as a noise 4 driven process [6,7,8]. Most of these methods use fractal or multifractal scaling analysis [9]. The approach has also yielded stochastic models of heart rate variability [10,11].…”
Section: Introductionmentioning
confidence: 99%
“…It was shown in Refs. [2,10,11] that the finite-difference kinetic equation of a nonMarkov type for TCF M 0 ðtÞ can be written by means of the technique of projection operators of Zwanzig'-Mori's type [14,15] …”
Section: Macroscopic Description In the Analysis Of Stochastic Processesmentioning
confidence: 99%
“…We have taken the interval of 40 points as the starting point and have calculated all the noise low-order parameters l i ði ¼ 1; 2; 3Þ and L j ðj ¼ 1; 2Þ by Eqs. (9) and (10). Then the interval was consistently increased by unit time segment t and the relaxation parameters l i , L j were calculated every time at the increase of the interval.…”
Section: Local Noisy Parametersmentioning
confidence: 99%
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