Hilbert Transformation and Properties of Solar Cycles in “Envelope−Instantaneous Frequency” Variables

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Abstract

During analyzing a narrowband signal, the Hilbert transform is often used, which makes it possible to describe the process through slowly changing functions: the envelope (amplitude) and, weakly dependent on time, the characteristic frequency of the signal - the “instantaneous” frequency. Based on the smoothness of these characteristics, one can evaluate the process and compare it at different periods. This approach was used to analyze the spectral components of a series of average monthly Wolf numbers. This description of the main and second harmonics, supplemented by the properties of the long-period component, gives a fairly complete picture of the entire series of monthly averages. The work examines the correspondence of the characteristics of reliable data, with this approach, to the accepted description through the parameters of cycles (maximum of the cycle, duration of the cycle and its growth branches) and constructs an “envelope” of the maxima of the cycles. The time dynamics of the “instantaneous” frequencies of the fundamental and second harmonics of the entire series are also presented and significant differences in their behavior are noted in the intervals corresponding to the reconstructed and reliable parts.

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About the authors

I. G. Shibaev

Pushkov Institute of Terrestrial Magnetism, Ionosphere and Radio Wave Propagation Russian Academy of Science (IZMIRAN)

Author for correspondence.
Email: ishib@izmiran.ru
Russian Federation, Troitsk, Moscow

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Supplementary files

Supplementary Files
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1. JATS XML
2. Fig. 1. Overview of the relationship between the new and old versions of the WSN series, the OX axis is the date.

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3. Fig. 2. (a) - spectrum of the Wtool series, OX axis in inverse months; (b) - overview of the P1÷P3 components, OX axis - date; (c) - mean values of cycles () and mean values of P1(Wtool) (+) at the intervals corresponding to these cycles, OX axis - cycle number; (d) - comparison of the W*, P13 series and overview of the constructed A13 series, OX axis - date.

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4. Fig. 3. Envelope-moment frequency representation of the P2 (left side) and P3 components of the Wtool series. The bottom panel of the figure shows the difference between the P2(Wtool) / P3(Wtool) series and their narrowband images. On the OX axis is the date.

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5. Fig. 4. Overview of the “instantaneous” frequencies of the P2 (left) and P3 components of the entire W series, the OX axis is the date.

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