Signal time–frequency representation and decomposition using partial fractions

Author:

Ursin Bjorn12,Porsani Milton J23ORCID

Affiliation:

1. Department of Electronic Systems, The Norwegian University of Science and Technology (NTNU), O.S. Bragstads plass 2b, NO-7491 Trondheim, Norway

2. Centro de Pesquisa em Geofísica e Geologia (CPPG/UFBA) and National Institute of Science and Technology of Petroleum Geophysics (INCT-GP/CNPQ), Instituto de Geociências, Universidade Federal da Bahia, Campus Universitário da Federação, Salvador, Bahia 40170-115, Brazil

3. Centro de Pesquisa em Geofísica e Geologia (CPPG/UFBA), Instituto de Geociências, Universidade Federal da Bahia, Campus Universitário da Federação, Salvador, Bahia 40170-115, Brazil

Abstract

Summary The Z-transform of a complex time signal (or the analytic signal of a real signal) is equal to the Z-transform of a prediction error divided by the Z-transform of the prediction error operator. This inverse is decomposed into a sum of partial fractions, which are used to obtain impulse response operators formed by non-causal filters that complex-conjugate symmetric coefficients. The time components are obtained by convolving the filters with the original signal, and the peak frequencies, corresponding to the poles of the prediction error operator, are used for mapping the time components into frequency components. For non-stationary signals, this decomposition is done in sliding time windows, and the signal component values, in the middle of each window, are attributed to the peak value of its frequency response that corresponds to the pole of this partial fraction component. The result is an exact, but non-unique, time–frequency representation of the input signal. A sparse signal decomposition can be obtained by summing along the frequency axis in patches with similar characteristics in the time–frequency domain. The peak amplitude frequency of each new time component is obtained by computing a scalar prediction error operator in sliding time windows, resulting in a sparse time–frequency representation. In both cases, the result is a time–frequency matrix where an estimate of the frequency content of the input signal can be obtained by summation over the time variable. The performance of the new method is demonstrated with excellent results on a synthetic time signal, the LIGO gravitational wave signal and seismic field data.

Funder

CNPq

MCTIC

CAPES

ANP

FINEP

FAPESB

Norwegian Research Council

Publisher

Oxford University Press (OUP)

Subject

Geochemistry and Petrology,Geophysics

Cited by 3 articles. 订阅此论文施引文献 订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献

1. Electromagnetic Situation Awareness Based on Improved STFrFT;2023 19th International Conference on Natural Computation, Fuzzy Systems and Knowledge Discovery (ICNC-FSKD);2023-07-29

2. Real-Time Inspection in Detection Magnetic Flux Leakage by Deep Learning Integrated with Concentrating Non-Destructive Principle and Electromagnetic Induction;IEEE Instrumentation & Measurement Magazine;2022-10

3. Signal Decomposition and Time-Frequency Representation Using Variable-Length Symmetric Filters;Brazilian Journal of Geophysics;2022-03-14

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