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eRA-7
       International
         Scientific                 A. A. Fotopoulosb, E. Petrakia, E. M. Vlamakisb, X. A. Argyrioub,
        Conference                     N. N. Chatzisavvasb, T. J. Sevvosb, A. Zisosc, C. Nomicosd,
                                    A. Louizie, J. Stonhama, P. H. Yannakopoulosb, D. Nikolopoulosc

                                       a   Brunel University, Dept. of Engineering and Design, UK
                                    b Department of Computer Systems Engineering, Technological

                                                 Educational Institute of Piraeus, Greece
                                        c Department of Physics, Chemistry and Material Science,

                                         Technological Educational Institute of Piraeus, Greece
                                          d Department of Electronics, Technological Educational

                                                      Institution of Athens, Greece
                                      e Medical Physics Department, Medical School, University of

                                                              Athens, Greece
http://env-hum-comp-res.teipir.gr
 Address  the analogous behavior of the MHz
  electromagnetic signals to soil radon
 Analysis of both signals with multivariate
  statistics, fractal evolving techniques and
  Detrended Fluctuation Analysis (DFA)
   Radon (222Rn) is a radioactive gas which is present in
    porous materials, underground and surface waters. It
    has been used as a trace gas in several studies of
    Earth, hydro-geology and atmosphere, because of its
    ability to travel to comparatively long distances and
    the efficiency of detecting it at very low levels.
   Well established criteria have been published for the
    identification, both of the radon precursors (Cicerone
    et. al,2009; Ghosh et. al.,2009) and of the precursors
    of the electromagnetic radiation in the ULF-kHz- MHz
    range (Eftaxias et. al., 2009; Eftaxias et. al., 2010).
    According to the earthquake classification of
    Hayakawa and Hobarra (2010), radon may be
    considered as a short-term earthquake predictor.
   A station for the surveillance
    of soil radon has been
    installed in Peloponnese,
    Ileia Prefecture in South
    West Greece.
   More than 600 Earthquakes
    of M>4,0 have been occurred
    in the last Century in Ileia
   Radon in soil is monitored by       Atmospheric pressure
    Alpha Guard (AG) Genitron            (AP), relative humidity
    Ltd. via a properly designed         (RH) and temperature (T)
    unit(Soil Gas Unit, Genitron         are continuously
    Ltd.) and accompanying               monitored as well
    equipment (Genitron, 1997)
 EM signals are continuously
  monitored by a telemetric
  network which consists of
  twelve stations (Nomikos and
  Vallianatos, 1998).
 MHz EM radiation is detected by
  bipolar antennas synchronised
  in the 41MHz and 46MHz
  frequencies.
 Stations are equipped with
  novel data-loggers designed
  adequately for the collection of
  data of the EM Network
  (Koulouras et al., 2005).
Fractal evolution of the EM
signals of Vamos station, 41
MHz signal, day 45, year 2008.
 i) Time evolution of the
    spectral exponent b
    ( 𝑺 ( 𝒇 )= 𝒂⋅𝒇− 𝒃)
ii) Spectral exponent log(a) ,
iii) Square of the Spearman's
     correlation coefficient
iv) Scalogram of the DWT
     respectively.

•   Power law beta values in the range
    1,5<b<2 indicate anti-persistency and
    values above 2 (b>2) persistency
•   Switching between persistency and
    anti-persistency identifies the long
    memory of the system


Spearman correlation coefficient takes
values very close to 1, i.e., the fit to the
power-law is excellent. This is a strong
indicator of the fractal character of the
underlying processes and structures
(Eftaxias et al.,2010).
Vamos Station 46 MHz EM signal days 48-51 year 2008           Neapoli Station 46 MHz EM signal days 75-78 year 2008




  High power-law-beta-
                                               Long-range temporal                     Each value correlates to
 values presented a very
                                               correlations indicate                    its long-term history in
peculiar increase, as high
                                              strong system memory.                          fractal manner
           as 4.
Background noise presents
 Scalogram of the DWT      0<b(t)<1, moving from the the first
of the 2008 radon signal   stage of general disorder to the
                           final stage of general failure
                           presenting stability and self-
                           organisements


                           For the power law spectrum
                            𝑺 (𝒇 )=𝒂⋅𝒇−𝒃
                           • The area between the two radon
                              spikes is very critical and presents
 Time evolution of the        fractal behaviour (b values above 1,5)
 power-law-beta values     • This low frequency enhancement
                              reveals the predominance of the
                              larger fracture events which is
                              considered as a footprint of the
                              preparation of earthquakes
                              (Eftaxias et al.,2009)


                              Anomalies detected in radon
                              concentrations in 2008 3 & 2
 Levels of soil radon        months before 6,5 Earthquake of
concentration in 2008                  6/8/2008


                           International Scientific Conference eRA-7
Examples of the application of the DWT. (a) Radon 2008 during the five-day
disturbance of the first radon spike (Nikolopoulos et al., 2012). (b) Vamos EM
station, 41 MHz signal, day 45, year 2008. The example corresponds to the
period between the EM bursts which exhibited successive and high values of the
spectral exponent b.
When high frequencies (low negative logarithms) are superimposed on the Power
Spectrum Density, the log-log slope is reduced and, subsequently, the calculated
power-law b-value and the Spearman correlation coefficient.
   DFA is a modified root-       For a given bin size n , the root-mean-square
                                  (rms) fluctuations for this integrated and
    mean-square analysis of a     detrended signal is calculated:
    random walk based on the                             𝑁
    following concept: a                            1
                                           𝐹 𝑛 =              *𝑦 𝑘 − 𝑛(𝑘)+2
                                                    𝑁
    stationary time series with                         𝑘=1

    long-range correlations       Where:
    can be integrated.            1. i=1,…N a time series of length N
                                  2. k the different time scales
   The measurement of the        3. y(k) the intergrated signal
    self-similarity scaling       4. n the length of each bin

    exponent of the               •   F(n) is repeated for a broad range of
    integrated series show the        scales box sizes (n).
    long-range correlation        •   A power-law relation between the
                                      average root-mean square fluctuation
    properties of the original        F(n) and the bin size n indicates the
    time series (Peng et              presence of scaling: 𝐹 (𝑛) ∼ 𝑛 𝑎
    al.,1998).                    •   The scaling exponent α quantifies the
                                      strength of the long-range power-law
                                      correlations in the time series.
Example for the case of the       DFA scatter plot for the      DFA scatter plot for the
2008 radon signal. This           2008 radon time-series.       the EM MHz time-series
figure corresponds to the         Exponents a1 and a2           of Vamos & Neapoli
period between the two radon
                                  separate radon background     Station of EM Telematic
spikes.
The short time scales exhibit     from high power-law-beta      Network.
lower slope (α1=1.19), while      values.                       These DFA values are in
the large time scales, higher     The high power-law-beta       close agreement to the
(α2=1.55). According to Peng et   values are characterised by   corresponding values of
al. (1994), these results show    much larger a1 and a2         the radon background.
persistent long range power
law correlations.
 Simultaneous appearance of high radon
  anomalies, high power-law b-values and high
  power spectral amplitudes, manifests that the
  wavelet power spectrum can be used as an
  alternative method for the recognition and
  visualisation of candidate precursory anomalies
  in a radon signal.
 New MHz EM signals that were derived
  concurrently to the 2008 radon signal. The
  signals were analysed with the methods applied
  to radon. The results indicated analogous
  behaviour between radon and MHz EM pre-
  earthquake time-series.
   Peng,C.-K., Hausdor, J.M., Havlin, S., Mietus, J.E., Stanley, H.E., Goldberger,A.L.,
    1998. Multiple-time scales analysis of physiological time series under neural
    control. Physica A 249, 491–500.
   Kapiris, P.G., Eftaxias, K.A., Nomikos, K.D., Polygiannakis, J., Dologlou, E.,
    Balasis, G. T., Bogris, N.G., Peratzakis, A.S., Hadjicontis, V.E., 2003. Evolving
    towards a critical point: A possible electromagnetic way in which the critical
    regime is reached as the rupture approaches. Nonlinear Proc. Geoph. 10, 1-14.
   Koulouras, G., Kontakos,K., Stavrakas, I., Stonham,J., Nomicos, C., 2005.A new
    data storage system designed for an embedded compact flash based data
    acquisition system.IEEE Circ. Dev. Mag. July/August 27-34.
   Nomikos, K., Vallianatos, F., 1998. Electromagnetic variations associated with the
    seismicity of the frontal Hellenic arc, Geol. Carpath. 49, 57–60.
   Smirnova, N.A., Hayakawa, M., 2007. Fractal characteristics of the ground-
    observed ULF emissions in relation to geomagnetic and seismic activities. J.
    Atmos. Sol.-Ter. Phy. 69,1833-1841.
   Cicerone, R.D., Ebel, J.E., Britton, J., 2009. A systematic compilation of
    earthquake precursors. Tectonophysics. 476, 371-396.
   Eftaxias, K., Balasis, G., Contoyiannis, Y., Papadimitriou, C., Kalimeri, M.,
    Athanasopoulou, L., Nikolopoulos, S., Kopanas, J. , Antonopoulos, G., Nomicos,
    C., 2010. Unfolding the procedure of characterizing recorded ultra low frequency,
    kHZ and MHz electromagnetic anomalies prior to the L’Aquila earthquake as pre-
    seismic ones – Part 2. Nat. Hazard. Earth Sys. 10, 275–94.
   Eftaxias, K., Balasis, G., Contoyiannis, Y., Papadimitriou, C., Kalimeri, M.,
    Athanasopoulou, L., Nikolopoulos, S., Kopanas, J. , Antonopoulos, G., Nomicos,
    C., 2009. Unfolding the procedure of characterizing recorded ultra low frequency,
    kHZ and MHz electromagnetic anomalies prior to the L’Aquila earthquake as pre-
    seismic ones – Part 1, Nat. Hazard. Earth Sys. 9, 1953–1971.
   Contoyiannis Y.F., Kapiris P.G., Eftaxias K.A., 2005. Monitoring of a preseismic
    phase from its electromagnetic precursors. Phys. Rev. E 71, 066123-1-066123-14.
   Ghosh, D., Deb, A., Dutta, S., Sengupta, R., 2012. Multifractality of radon
    concentration fluctuation in earthquake related signal. Fractals. 20 (01), 33.
   Erees, F.S., Aytas, S., Sac, M.M., Yener, G., Salk, M., 2007. Radon concentrations
    in thermalwaters related to seismic events along faults in the Denizli
    Basin,Western Turkey. Radiat. Meas. 42, 80-86.
   Hayakawa, M., Hobara, Y., 2010. Current status of seismo-electromagnetics for
    short-term earthquake prediction. Geomatics, Natural Hazards and Risk 1(2), 115-
    155.
   Kapiris, P., Polygiannakis, J., Peratzakis, A., Nomicos, K., Eftaxias, K., 2002.
    VHFelectromagnetic evidence of the underlying pre-seismic critical stage. Earth
    Planets Space 54, 1237–1246.
http://env-hum-comp-res.teipir.gr/

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Similarities in the self organised critical characteristics between radon and m-hz em disturbances during a very seismic period in Greece

  • 1. eRA-7 International Scientific A. A. Fotopoulosb, E. Petrakia, E. M. Vlamakisb, X. A. Argyrioub, Conference N. N. Chatzisavvasb, T. J. Sevvosb, A. Zisosc, C. Nomicosd, A. Louizie, J. Stonhama, P. H. Yannakopoulosb, D. Nikolopoulosc a Brunel University, Dept. of Engineering and Design, UK b Department of Computer Systems Engineering, Technological Educational Institute of Piraeus, Greece c Department of Physics, Chemistry and Material Science, Technological Educational Institute of Piraeus, Greece d Department of Electronics, Technological Educational Institution of Athens, Greece e Medical Physics Department, Medical School, University of Athens, Greece http://env-hum-comp-res.teipir.gr
  • 2.  Address the analogous behavior of the MHz electromagnetic signals to soil radon  Analysis of both signals with multivariate statistics, fractal evolving techniques and Detrended Fluctuation Analysis (DFA)
  • 3. Radon (222Rn) is a radioactive gas which is present in porous materials, underground and surface waters. It has been used as a trace gas in several studies of Earth, hydro-geology and atmosphere, because of its ability to travel to comparatively long distances and the efficiency of detecting it at very low levels.  Well established criteria have been published for the identification, both of the radon precursors (Cicerone et. al,2009; Ghosh et. al.,2009) and of the precursors of the electromagnetic radiation in the ULF-kHz- MHz range (Eftaxias et. al., 2009; Eftaxias et. al., 2010). According to the earthquake classification of Hayakawa and Hobarra (2010), radon may be considered as a short-term earthquake predictor.
  • 4. A station for the surveillance of soil radon has been installed in Peloponnese, Ileia Prefecture in South West Greece.  More than 600 Earthquakes of M>4,0 have been occurred in the last Century in Ileia  Radon in soil is monitored by  Atmospheric pressure Alpha Guard (AG) Genitron (AP), relative humidity Ltd. via a properly designed (RH) and temperature (T) unit(Soil Gas Unit, Genitron are continuously Ltd.) and accompanying monitored as well equipment (Genitron, 1997)
  • 5.  EM signals are continuously monitored by a telemetric network which consists of twelve stations (Nomikos and Vallianatos, 1998).  MHz EM radiation is detected by bipolar antennas synchronised in the 41MHz and 46MHz frequencies.  Stations are equipped with novel data-loggers designed adequately for the collection of data of the EM Network (Koulouras et al., 2005).
  • 6. Fractal evolution of the EM signals of Vamos station, 41 MHz signal, day 45, year 2008. i) Time evolution of the spectral exponent b ( 𝑺 ( 𝒇 )= 𝒂⋅𝒇− 𝒃) ii) Spectral exponent log(a) , iii) Square of the Spearman's correlation coefficient iv) Scalogram of the DWT respectively. • Power law beta values in the range 1,5<b<2 indicate anti-persistency and values above 2 (b>2) persistency • Switching between persistency and anti-persistency identifies the long memory of the system Spearman correlation coefficient takes values very close to 1, i.e., the fit to the power-law is excellent. This is a strong indicator of the fractal character of the underlying processes and structures (Eftaxias et al.,2010).
  • 7. Vamos Station 46 MHz EM signal days 48-51 year 2008 Neapoli Station 46 MHz EM signal days 75-78 year 2008 High power-law-beta- Long-range temporal Each value correlates to values presented a very correlations indicate its long-term history in peculiar increase, as high strong system memory. fractal manner as 4.
  • 8. Background noise presents Scalogram of the DWT 0<b(t)<1, moving from the the first of the 2008 radon signal stage of general disorder to the final stage of general failure presenting stability and self- organisements For the power law spectrum 𝑺 (𝒇 )=𝒂⋅𝒇−𝒃 • The area between the two radon spikes is very critical and presents Time evolution of the fractal behaviour (b values above 1,5) power-law-beta values • This low frequency enhancement reveals the predominance of the larger fracture events which is considered as a footprint of the preparation of earthquakes (Eftaxias et al.,2009) Anomalies detected in radon concentrations in 2008 3 & 2 Levels of soil radon months before 6,5 Earthquake of concentration in 2008 6/8/2008 International Scientific Conference eRA-7
  • 9. Examples of the application of the DWT. (a) Radon 2008 during the five-day disturbance of the first radon spike (Nikolopoulos et al., 2012). (b) Vamos EM station, 41 MHz signal, day 45, year 2008. The example corresponds to the period between the EM bursts which exhibited successive and high values of the spectral exponent b. When high frequencies (low negative logarithms) are superimposed on the Power Spectrum Density, the log-log slope is reduced and, subsequently, the calculated power-law b-value and the Spearman correlation coefficient.
  • 10. DFA is a modified root- For a given bin size n , the root-mean-square (rms) fluctuations for this integrated and mean-square analysis of a detrended signal is calculated: random walk based on the 𝑁 following concept: a 1 𝐹 𝑛 = *𝑦 𝑘 − 𝑛(𝑘)+2 𝑁 stationary time series with 𝑘=1 long-range correlations Where: can be integrated. 1. i=1,…N a time series of length N 2. k the different time scales  The measurement of the 3. y(k) the intergrated signal self-similarity scaling 4. n the length of each bin exponent of the • F(n) is repeated for a broad range of integrated series show the scales box sizes (n). long-range correlation • A power-law relation between the average root-mean square fluctuation properties of the original F(n) and the bin size n indicates the time series (Peng et presence of scaling: 𝐹 (𝑛) ∼ 𝑛 𝑎 al.,1998). • The scaling exponent α quantifies the strength of the long-range power-law correlations in the time series.
  • 11. Example for the case of the DFA scatter plot for the DFA scatter plot for the 2008 radon signal. This 2008 radon time-series. the EM MHz time-series figure corresponds to the Exponents a1 and a2 of Vamos & Neapoli period between the two radon separate radon background Station of EM Telematic spikes. The short time scales exhibit from high power-law-beta Network. lower slope (α1=1.19), while values. These DFA values are in the large time scales, higher The high power-law-beta close agreement to the (α2=1.55). According to Peng et values are characterised by corresponding values of al. (1994), these results show much larger a1 and a2 the radon background. persistent long range power law correlations.
  • 12.  Simultaneous appearance of high radon anomalies, high power-law b-values and high power spectral amplitudes, manifests that the wavelet power spectrum can be used as an alternative method for the recognition and visualisation of candidate precursory anomalies in a radon signal.  New MHz EM signals that were derived concurrently to the 2008 radon signal. The signals were analysed with the methods applied to radon. The results indicated analogous behaviour between radon and MHz EM pre- earthquake time-series.
  • 13. Peng,C.-K., Hausdor, J.M., Havlin, S., Mietus, J.E., Stanley, H.E., Goldberger,A.L., 1998. Multiple-time scales analysis of physiological time series under neural control. Physica A 249, 491–500.  Kapiris, P.G., Eftaxias, K.A., Nomikos, K.D., Polygiannakis, J., Dologlou, E., Balasis, G. T., Bogris, N.G., Peratzakis, A.S., Hadjicontis, V.E., 2003. Evolving towards a critical point: A possible electromagnetic way in which the critical regime is reached as the rupture approaches. Nonlinear Proc. Geoph. 10, 1-14.  Koulouras, G., Kontakos,K., Stavrakas, I., Stonham,J., Nomicos, C., 2005.A new data storage system designed for an embedded compact flash based data acquisition system.IEEE Circ. Dev. Mag. July/August 27-34.  Nomikos, K., Vallianatos, F., 1998. Electromagnetic variations associated with the seismicity of the frontal Hellenic arc, Geol. Carpath. 49, 57–60.  Smirnova, N.A., Hayakawa, M., 2007. Fractal characteristics of the ground- observed ULF emissions in relation to geomagnetic and seismic activities. J. Atmos. Sol.-Ter. Phy. 69,1833-1841.  Cicerone, R.D., Ebel, J.E., Britton, J., 2009. A systematic compilation of earthquake precursors. Tectonophysics. 476, 371-396.  Eftaxias, K., Balasis, G., Contoyiannis, Y., Papadimitriou, C., Kalimeri, M., Athanasopoulou, L., Nikolopoulos, S., Kopanas, J. , Antonopoulos, G., Nomicos, C., 2010. Unfolding the procedure of characterizing recorded ultra low frequency, kHZ and MHz electromagnetic anomalies prior to the L’Aquila earthquake as pre- seismic ones – Part 2. Nat. Hazard. Earth Sys. 10, 275–94.
  • 14. Eftaxias, K., Balasis, G., Contoyiannis, Y., Papadimitriou, C., Kalimeri, M., Athanasopoulou, L., Nikolopoulos, S., Kopanas, J. , Antonopoulos, G., Nomicos, C., 2009. Unfolding the procedure of characterizing recorded ultra low frequency, kHZ and MHz electromagnetic anomalies prior to the L’Aquila earthquake as pre- seismic ones – Part 1, Nat. Hazard. Earth Sys. 9, 1953–1971.  Contoyiannis Y.F., Kapiris P.G., Eftaxias K.A., 2005. Monitoring of a preseismic phase from its electromagnetic precursors. Phys. Rev. E 71, 066123-1-066123-14.  Ghosh, D., Deb, A., Dutta, S., Sengupta, R., 2012. Multifractality of radon concentration fluctuation in earthquake related signal. Fractals. 20 (01), 33.  Erees, F.S., Aytas, S., Sac, M.M., Yener, G., Salk, M., 2007. Radon concentrations in thermalwaters related to seismic events along faults in the Denizli Basin,Western Turkey. Radiat. Meas. 42, 80-86.  Hayakawa, M., Hobara, Y., 2010. Current status of seismo-electromagnetics for short-term earthquake prediction. Geomatics, Natural Hazards and Risk 1(2), 115- 155.  Kapiris, P., Polygiannakis, J., Peratzakis, A., Nomicos, K., Eftaxias, K., 2002. VHFelectromagnetic evidence of the underlying pre-seismic critical stage. Earth Planets Space 54, 1237–1246.