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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Phys.</journal-id>
<journal-title>Frontiers in Physics</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Phys.</abbrev-journal-title>
<issn pub-type="epub">2296-424X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fphy.2019.00115</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physics</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Characterization of Visuomotor/Imaginary Movements in EEG: An Information Theory and Complex Network Approach</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Baravalle</surname> <given-names>Roman</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/702695/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Guisande</surname> <given-names>Natal&#x000ED;</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Granado</surname> <given-names>Mauro</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/117002/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Rosso</surname> <given-names>Osvaldo A.</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/658157/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Montani</surname> <given-names>Fernando</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/130420/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Instituto de F&#x000ED;sica La Plata (IFLP), CONICET CCT-La Plata &#x00026; Universidad Nacional de La Plata (UNLP)</institution>, <addr-line>La Plata</addr-line>, <country>Argentina</country></aff>
<aff id="aff2"><sup>2</sup><institution>Departamento de Inform&#x000E1;tica en Salud, CONICET, Hospital Italiano de Buenos Aires</institution>, <addr-line>Buenos Aires</addr-line>, <country>Argentina</country></aff>
<aff id="aff3"><sup>3</sup><institution>Instituto de F&#x000ED;sica, Universidade Federal de Alagoas</institution>, <addr-line>Macei&#x000F3;</addr-line>, <country>Brazil</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Chris G. Antonopoulos, University of Essex, United Kingdom</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Emanuela Formaggio, University of Padova, Italy; Kelly Cristiane Iarosz, University of S&#x000E3;o Paulo, Brazil</p></fn>
<corresp id="c001">&#x0002A;Correspondence: Osvaldo A. Rosso <email>oarosso&#x00040;gmail.com</email></corresp>
<fn fn-type="other" id="fn001"><p>This article was submitted to Biophysics, a section of the journal Frontiers in Physics</p></fn></author-notes>
<pub-date pub-type="epub">
<day>20</day>
<month>08</month>
<year>2019</year>
</pub-date>
<pub-date pub-type="collection">
<year>2019</year>
</pub-date>
<volume>7</volume>
<elocation-id>115</elocation-id>
<history>
<date date-type="received">
<day>12</day>
<month>03</month>
<year>2019</year>
</date>
<date date-type="accepted">
<day>31</day>
<month>07</month>
<year>2019</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2019 Baravalle, Guisande, Granado, Rosso and Montani.</copyright-statement>
<copyright-year>2019</copyright-year>
<copyright-holder>Baravalle, Guisande, Granado, Rosso and Montani</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract><p>Imagined activities could actually be a cognitive basis for creative thinking. However, it is still unknown how they might be related with the architecture of the brain. A recent study has proved the relevance of the imagined activity when investigating neuronal diseases by comparing variations in the neuronal activity of patients with brain diseases and healthy subjects. One important aspect of the scientific methodologies focused on neuronal diseases is therefore to provide a trustable methodology that could allow us to distinguish between realized and imagined activities in the brain. The electroencephalogram is the result of synchronized action of the cerebrum, and our end is portraying the network dynamics through the neuronal responses when the subjects perform visuomotor and specific imaginary assignments. We use a subtle information theoretical approach accounting for the time causality of the signal and the closeness centrality of the different nodes. More specifically we perform estimations of the probability distribution of the data associated to each node using the Bandt and Pompe approach to account for the causality of the electroencephalographic signals. We calculate the Jensen-Shannon distance across different nodes, and then we quantify how fast the information flow would be through a given node to other nodes computing the closeness centrality. We perform a statistical analysis to compare the closeness centrality considering the different rhythmic oscillation bands for each node taking into account imagined and visuomotor tasks. Our discoveries stress the pertinence of the alpha band while performing and distinguishing the specific imaginary or visuomotor assignments.</p></abstract>
<kwd-group>
<kwd>neuronal dynamics</kwd>
<kwd>EEG</kwd>
<kwd>alpha oscillations</kwd>
<kwd>visuomotor tasks</kwd>
<kwd>imagined tasks</kwd>
</kwd-group>
<counts>
<fig-count count="12"/>
<table-count count="1"/>
<equation-count count="7"/>
<ref-count count="83"/>
<page-count count="17"/>
<word-count count="9111"/>
</counts>
</article-meta> 
</front>
<body>
<sec sec-type="intro" id="s1">
<title>1. Introduction</title>
<p>One of the principal assumptions in neuroscience is that the brain computes, and this is accepted by most scientists in the area. That is, the cerebrum takes approaching tangible information, encodes it into a few biophysical factors consisting of membrane voltage or neuronal activation costs, after which a wide variety of dynamic operations are played to extract applicable features of the input. The result is that some of these computations can be stored for later access and ultimately, to control the behavior of the animal in the most convenient way. In addition, the brain processes sensory information in multiple stages in neural circuits. The information is transmitted through trains of action potential or less frequently by local field potentials (LFPs). More specifically for the action potentials, the information can also be transmitted through the counting of spikes, the temporal precision of them, the structure of the time series, the synchronization between groups of neurons, or some combination of these [<xref ref-type="bibr" rid="B1">1</xref>&#x02013;<xref ref-type="bibr" rid="B11">11</xref>]. Thus, the brain does not have a single code but multiple which depend on multiple complex dynamic variables.</p>
<p>In particular, the scalp electroencephalogram (EEG), recorded by means of a given electrode, can be taken into consideration as a spatiotemporally smoothed version of the LFP that is incorporated over an area of 10 cm<sup>2</sup> or greater. Electroencephalography can accurately detect brain activity at a time resolution of a single millisecond [<xref ref-type="bibr" rid="B12">12</xref>]. This technique provides continuous recording of the brain&#x00027;s electrical processes which allows us to relate changes in signal with a particular cognitive task. It is conceivable to extract from the EEG the functional connectivity network. However, the elucidation of the inter-connectivity from sensor level recordings is not straightforward [<xref ref-type="bibr" rid="B13">13</xref>]. In this manner some endeavors to use convenient techniques on the time series dynamics recreated from scalp EEG signals can be found in the literature [<xref ref-type="bibr" rid="B14">14</xref>&#x02013;<xref ref-type="bibr" rid="B17">17</xref>]. Network theory is usually based on graph theory, probability theory, statistical mechanics, and dynamical systems [<xref ref-type="bibr" rid="B14">14</xref>&#x02013;<xref ref-type="bibr" rid="B28">28</xref>].</p>
<p>The brain is a large-scale complex network and discovering interdependencies between at least two EEG electrodes can be described utilizing a few methodologies [<xref ref-type="bibr" rid="B29">29</xref>]. Let us remark that the network analysis of EEG data can help us to gain a deeper understanding of the brain functions as finding the correct functional connectivity of the brain through EEG signal can be used as a biomarker to diagnose mental disorders [<xref ref-type="bibr" rid="B17">17</xref>, <xref ref-type="bibr" rid="B30">30</xref>, <xref ref-type="bibr" rid="B31">31</xref>]. Investigating the dynamics of the EEG signals complex network means to estimate the degree of correlation across the different temporal patterns for the different electrodes or nodes. Fluctuations of electrical activity registered by EEG show correlated neuronal activity [<xref ref-type="bibr" rid="B32">32</xref>]. The extent of oscillatory coupling between two EEG signals can be used as a measure of strength to reflect network activity of the brain. The human brain can be understood as a large-scale complex network [<xref ref-type="bibr" rid="B15">15</xref>, <xref ref-type="bibr" rid="B33">33</xref>, <xref ref-type="bibr" rid="B34">34</xref>], the topological properties of EEG-derived networks describe working memory phases [<xref ref-type="bibr" rid="B35">35</xref>], and variations in the path length connectivity across nodes can be linked with mental diseases [<xref ref-type="bibr" rid="B17">17</xref>, <xref ref-type="bibr" rid="B31">31</xref>].</p>
<p>Methods of EEG analysis are based on the investigation of dynamic changes of electrical activity in time, frequency, and space. A straight methodology for assessing the associations is finding how comparable the signals&#x00027; waveforms are of each frequency when a time-lag is used to one of them. This is evaluated through cross-correlation [<xref ref-type="bibr" rid="B30">30</xref>, <xref ref-type="bibr" rid="B36">36</xref>, <xref ref-type="bibr" rid="B37">37</xref>]. However, non-linear components of coupling can control the neuronal activity. In this way non-linear affinity measures ought to be considered to determine the brain complex network. Bandt and Pompe (BP) proposed a novel methodology that comprises in changing the signal, by means of a symbolic methodology, into a sequence of patterns and then making inference over them [<xref ref-type="bibr" rid="B38">38</xref>&#x02013;<xref ref-type="bibr" rid="B40">40</xref>]. In view of the evaluation of the ordinal structures present in the time series and their neighborhood impact on the related probability density function they include the signals&#x00027; own temporal causality through a methodology of simple application and direct estimation [<xref ref-type="bibr" rid="B38">38</xref>&#x02013;<xref ref-type="bibr" rid="B42">42</xref>]. Thus, the BP approach permits us to find important causative data associated with the hidden non-linear variables that regulate the system. Statistical complexity measures are useful to quantify stochastic systems and to detect whether a system is not deterministic or random. The perfect order and the maximum randomness can be depicted all around effectively on the grounds that they do not have any structure and in the two cases the statistical complexity is zero. In any case, between these two limits there is a wide scope of ordinal structures of important stochastic nature. The complexity measure has been effectively utilized in perception and portrayal of various dynamical regimes [<xref ref-type="bibr" rid="B38">38</xref>&#x02013;<xref ref-type="bibr" rid="B43">43</xref>]. The non-linear elements of the cerebrum are of dissipative nature, and subject to non-equilibrium conditions that describe the developing properties of the neurons and portray the conduct of the neuronal capacities. The Jensen-Shannon divergence, which evaluates the contrast between (at least two) probability distribution functions (PDFs), is particularly valuable to compare the symbol-composition of different sequences. Statistical complexity enables us to measure basic features about the dynamic of the PDF related to the EEG recorded activity [<xref ref-type="bibr" rid="B38">38</xref>&#x02013;<xref ref-type="bibr" rid="B43">43</xref>]. This measure originally obtained from Information Theory enables us to evaluate the non-linear dynamics of the electro-cortical responses [<xref ref-type="bibr" rid="B38">38</xref>&#x02013;<xref ref-type="bibr" rid="B43">43</xref>]. The statistical complexity is the result of two entropies, the Shannon entropy and Jensen&#x02013;Shannon divergence, however it is a non-trivial mathematical relation of the entropy since it relies upon two probability functions, i.e., the one relating to the condition of the system and the uniform PDF taken as reference state. Essentially, in the present work we estimate the normalized Jensen-Shannon distance between two probabilities, however one comparing to the condition of the electrical activity in one electrode and the state PDF taken from another electrode as reference [<xref ref-type="bibr" rid="B44">44</xref>]. The aim of this study is to perform a discrimination of imagined [<xref ref-type="bibr" rid="B45">45</xref>] and non-imagined tasks through the application of the Jensen&#x02013;Shannon divergence of the BP probabilities across different electrodes sites in combination with estimation of the closeness centrality of nodes. We conduct a statistical analysis to examine the closeness centrality for the different rhythmic oscillation bands and nodes, considering imagined and visuomotor tasks. Our current approach allows us to discriminate imagined and non-imagined tasks characterizing the most important nodes within a graph for the different rhythmic oscillation bands using a functional network based on the BP formalism and the Jensen&#x02013;Shannon divergence.</p>
</sec>
<sec sec-type="methods" id="s2">
<title>2. Methodology</title>
<sec>
<title>2.1. Time Series Analysis and Ordinal Patterns</title>
<p>Consider <inline-formula><mml:math id="M1"><mml:mrow><mml:mi mathvariant="-tex-caligraphic">X</mml:mi></mml:mrow><mml:mo>&#x02261;</mml:mo><mml:msubsup><mml:mrow><mml:mrow><mml:mo>{</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>}</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>M</mml:mi></mml:mrow></mml:msubsup></mml:math></inline-formula> a time signal of length <italic>M</italic>, and at first, we expect that there are not equivalent abundance esteems in the time signal, that is the probability <italic>P</italic>(<italic>x</italic><sub><italic>t</italic><sub>1</sub></sub> &#x0003D; <italic>x</italic><sub><italic>t</italic><sub>2</sub></sub>) &#x0003D; 0 &#x02200; <italic>t</italic><sub>1</sub> &#x02260; <italic>t</italic><sub>2</sub>. Bandt and Pompe presented in their foundational paper an effective technique for the assessment of PDF related to a time signal utilizing a symbolization system [<xref ref-type="bibr" rid="B38">38</xref>]. For a point by point portrayal of the methodology we allude the reader to [<xref ref-type="bibr" rid="B46">46</xref>]. The significant symbolic descriptions are (i) made by ranking the magnitudes of the signal and (ii) characterized by reordering the symbols in upward order; this is similar to a state space reconstruction with embedding dimension <italic>D</italic> and time lag &#x003C4;. Further subtleties portraying the focal points that make the BP system more helpful than regular techniques dependent on range dividing (i.e., PDF amplitude histograms) can be discovered in Olivares et al. [<xref ref-type="bibr" rid="B47">47</xref>, <xref ref-type="bibr" rid="B48">48</xref>], Rosso et al. [<xref ref-type="bibr" rid="B49">49</xref>, <xref ref-type="bibr" rid="B50">50</xref>], Rosso and Masoller [<xref ref-type="bibr" rid="B39">39</xref>, <xref ref-type="bibr" rid="B40">40</xref>], Saco et al. [<xref ref-type="bibr" rid="B51">51</xref>], and Keller and Sinn [<xref ref-type="bibr" rid="B52">52</xref>]. The BP approach can be used for any kind of signals, and the main condition for the appropriateness of this procedure is a stationary hypothesis (that is, for <italic>k</italic> &#x02264; <italic>D</italic>, the likelihood for <italic>x</italic><sub><italic>t</italic></sub> &#x0003C; <italic>x</italic><sub><italic>t</italic>&#x0002B;<italic>k</italic></sub> ought not be conditional on <italic>t</italic> [<xref ref-type="bibr" rid="B38">38</xref>]). To utilize the Bandt and Pompe [<xref ref-type="bibr" rid="B38">38</xref>] procedure for assessing the PDF, <italic>P</italic>, related with the signal, one starts considering parcellings of the appropriate <italic>D</italic>-dimensional space that will &#x0201C;uncover&#x0201D; pertinent subtleties of the ordinal structure of a signal <inline-formula><mml:math id="M2"><mml:mrow><mml:mi mathvariant="-tex-caligraphic">X</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mrow><mml:mo>{</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>;</mml:mo><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mo>&#x022EF;</mml:mo><mml:mspace width="0.3em" class="thinspace"/><mml:mo>,</mml:mo><mml:mi>M</mml:mi></mml:mrow><mml:mo>}</mml:mo></mml:mrow></mml:math></inline-formula> with <italic>D</italic> &#x0003E; 1 (<italic>D</italic> &#x02208; &#x02115;) and &#x003C4; (&#x003C4; &#x02208; &#x02115;). Consider the &#x0201C;ordinal pattern&#x0201D; of order (length) <italic>D</italic> produced by (<italic>s</italic>) &#x021A6; (<italic>x</italic><sub><italic>s</italic>&#x02212;(<italic>D</italic>&#x02212;1)&#x003C4;</sub>, <italic>x</italic><sub><italic>s</italic>&#x02212;(<italic>D</italic>&#x02212;2)&#x003C4;</sub>, &#x022EF;&#x000A0;, <italic>x</italic><sub><italic>s</italic>&#x02212;&#x003C4;</sub>, <italic>x</italic><sub><italic>s</italic></sub> ), that gives to each time <italic>s</italic> the <italic>D</italic>-dimensional vector of magnitudes in instants <italic>s,s</italic> &#x02212; &#x003C4;, &#x022EF;&#x000A0;, <italic>s</italic> &#x02212; (<italic>D</italic> &#x02212; 1)&#x003C4;. Notice that when the <italic>D</italic>&#x02212;value is greater, more data about the past are incorporated into our vectors. We designate &#x0201C;ordinal pattern&#x0201D; identified with the time (<italic>s</italic>) to the configuration &#x003C0; &#x0003D; (<italic>r</italic><sub>0</sub>, <italic>r</italic><sub>1</sub>, &#x022EF;&#x000A0;, <italic>r</italic><sub><italic>D</italic>&#x02212;1</sub>) of [0, 1, &#x022EF;&#x000A0;, <italic>D</italic>&#x02212;1] characterized by <italic>x</italic><sub><italic>s</italic>&#x02212;<italic>r</italic><sub><italic>D</italic>&#x02212;1</sub> &#x003C4; </sub> &#x02264; <italic>x</italic><sub><italic>s</italic>&#x02212;<italic>r</italic><sub><italic>D</italic> &#x02212; 2</sub> &#x003C4; </sub> &#x02264; &#x022EF; &#x02264; <italic>x</italic><sub><italic>s</italic>&#x02212;<italic>r</italic><sub>1</sub> &#x003C4; </sub> &#x02264; <italic>x</italic><sub><italic>s</italic>&#x02212;<italic>r</italic><sub>0</sub> &#x003C4; </sub>. Vitally, to get a one of a kind outcome we take <italic>r</italic><sub><italic>i</italic></sub> &#x0003C; <italic>r</italic><sub><italic>i</italic>&#x02212;1</sub> if <italic>x</italic><sub><italic>s</italic>&#x02212;<italic>r</italic><sub><italic>i</italic></sub></sub> &#x0003D; <italic>x</italic><sub><italic>s</italic>&#x02212;<italic>r</italic><sub><italic>i</italic>&#x02212;1</sub></sub>. This can be warranted if the <italic>x</italic><sub><italic>t</italic></sub> comes from a continuous PDF, so similar magnitudes are unlikely. In this manner, for all the <italic>D</italic>! conceivable configurations &#x003C0; of order <italic>D</italic>, their related relative frequencies can be determined by the occasions this specific arrangement is found in the signal divided by the full number of configurations:</p>
<disp-formula id="E1"><label>(1)</label><mml:math id="M3"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mi>p</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>&#x003C0;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mi>&#x0266F;</mml:mi><mml:mrow><mml:mo>{</mml:mo><mml:mrow><mml:mi>s</mml:mi><mml:mo>|</mml:mo><mml:mi>s</mml:mi><mml:mtext>&#x000A0;&#x000A0;</mml:mtext><mml:mo>&#x02264;</mml:mo><mml:mtext>&#x000A0;&#x000A0;</mml:mtext><mml:mi>M</mml:mi><mml:mo>-</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>D</mml:mi><mml:mo>-</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>&#x003C4;</mml:mi><mml:mo>;</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mtext>&#x000A0;&#x000A0;</mml:mtext><mml:mtext class="texttt" mathvariant="monospace">is&#x000A0;of&#x000A0;kind</mml:mtext><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mrow><mml:mi>&#x003C0;</mml:mi></mml:mrow><mml:mrow><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>}</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mi>M</mml:mi><mml:mo>-</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>D</mml:mi><mml:mo>-</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>&#x003C4;</mml:mi></mml:mrow></mml:mfrac><mml:mtext>&#x000A0;</mml:mtext><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>We allude the image &#x0266F; to &#x0201C;number.&#x0201D; That is, an ordinal PDF <italic>P</italic> &#x0003D; {<italic>p</italic>(&#x003C0;<sub><italic>i</italic></sub>), <italic>i</italic> &#x0003D; 1, &#x022EF;&#x000A0;, <italic>D</italic>!} is obtained from the signal. In this way it is conceivable to measure the variety of the permutations of length <italic>D</italic> got from a scalar signal by estimating the Shannon Entropy and MPR statistical complexity. The embedding measurement <italic>D</italic> decides the quantity of possible states <italic>D</italic>!. The signal of length <italic>M</italic> that one needs so as to work with truthful estimators is <italic>M</italic> &#x0226B; <italic>D</italic>! [<xref ref-type="bibr" rid="B49">49</xref>]. We wish to underline that Bandt and Pompe recommended working with 4 &#x02264; <italic>D</italic> &#x02264; 6 and explicitly considered a delay &#x003C4; &#x0003D; 1 in their foundational paper [<xref ref-type="bibr" rid="B38">38</xref>]. Be that as it may, another estimation of &#x003C4; can likewise generate extra knowledge [<xref ref-type="bibr" rid="B47">47</xref>, <xref ref-type="bibr" rid="B48">48</xref>, <xref ref-type="bibr" rid="B53">53</xref>&#x02013;<xref ref-type="bibr" rid="B57">57</xref>].</p>
</sec>
</sec>
<sec id="s3">
<title>3. The Jensen Shannon Divergence</title>
<p>Entropy gives us an amount of incertitude and is the most representative case of the information quantifiers. For a PDF <italic>f</italic>(<italic>x</italic>) with <italic>x</italic> &#x02208; &#x00394; &#x02282; &#x0211D; and <inline-formula><mml:math id="M4"><mml:msub><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mo>&#x00394;</mml:mo></mml:mrow></mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>d</mml:mi><mml:mi>x</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:math></inline-formula>, we characterize the <italic>Shannon Entropy</italic> <italic>S</italic> [<xref ref-type="bibr" rid="B58">58</xref>] as</p>
<disp-formula id="E2"><label>(2)</label><mml:math id="M5"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mi>S</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mtext>&#x000A0;</mml:mtext><mml:mo>=</mml:mo><mml:mtext>&#x000A0;</mml:mtext><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:msub><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mo>&#x00394;</mml:mo></mml:mrow></mml:msub></mml:mstyle><mml:mi>f</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:msub><mml:mrow><mml:mo class="qopname">log</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mi>d</mml:mi><mml:mi>x</mml:mi><mml:mtext>&#x000A0;</mml:mtext><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>In the discrete case, let be <inline-formula><mml:math id="M6"><mml:mrow><mml:mi mathvariant="-tex-caligraphic">X</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>&#x02261;</mml:mo><mml:mrow><mml:mo>{</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>x</mml:mi></mml:mrow><mml:mrow><mml:mi>t</mml:mi></mml:mrow></mml:msub><mml:mo>;</mml:mo><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mo>&#x022EF;</mml:mo><mml:mo>,</mml:mo><mml:mi>M</mml:mi></mml:mrow><mml:mo>}</mml:mo></mml:mrow></mml:math></inline-formula>, a time series with <italic>M</italic> samples and the related PDF, given by <italic>P</italic> &#x02261; {<italic>p</italic><sub><italic>j</italic></sub>; <italic>j</italic> &#x0003D; 1, &#x022EF;, <italic>N</italic>} with <inline-formula><mml:math id="M7"><mml:munderover accentunder="false" accent="false"><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:munderover><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:math></inline-formula> and <italic>N</italic> the quantity of conceivable states of the examined physical system. Then, Shannon&#x00027;s logarithmic data measure [<xref ref-type="bibr" rid="B58">58</xref>] is characterized by</p>
<disp-formula id="E3"><label>(3)</label><mml:math id="M8"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mi>S</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:munderover accentunder="false" accent="false"><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:munderover></mml:mstyle><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mo class="qopname">log</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>This quantity is equivalent to zero when we can anticipate with sureness which of the conceivable outcomes <italic>j</italic>, whose probabilities are given by <inline-formula><mml:math id="M9"><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mrow><mml:mo stretchy="false">{</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi>j</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:mrow></mml:math></inline-formula> <italic>and</italic> <inline-formula><mml:math id="M10"><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mo>&#x02200;</mml:mo><mml:msup><mml:mrow><mml:mi>j</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup><mml:mo>&#x02260;</mml:mo><mml:mi>j</mml:mi><mml:mo stretchy="false">}</mml:mo></mml:math></inline-formula>, it will truly occur. So, in this condition we have maximum information about the hidden procedure. In contrast, this information is negligible for a uniform PDF <italic>P</italic><sub><italic>e</italic></sub> &#x0003D; {<italic>p</italic><sub><italic>j</italic></sub> &#x0003D; 1/<italic>N</italic>, &#x02200;<italic>j</italic> &#x0003D; 1, &#x022EF;&#x000A0;, <italic>N</italic>}. Regarding the interpretation, the entropy of <italic>P</italic>(<italic>X</italic>) indicates the base number of bits expected to encode the estimations of an arbitrary variable <italic>X</italic> with probability density function <italic>P</italic>(<italic>X</italic>). The Shannon entropy <italic>S</italic> is a quantity of &#x0201C;global character&#x0201D; that is not extremely susceptible to high changes in the PDF that happens in a short zone. Nonetheless, it is essential to bring up that ordinal structures present in a signal are not evaluated by haphazardness or randomness measures.</p>
<p>Let us now consider a time series measured by a given electrode that can be represented by a symbolization alphabet to which we assign a probability distribution <italic>Q</italic> &#x0003D; {<italic>q</italic><sub><italic>j</italic></sub>, <italic>j</italic> &#x0003D; 1, &#x022EF;&#x000A0;, <italic>N</italic>}, and another electrode measures a different time series represented also by different symbols that were drawn from a different probability distribution, <italic>P</italic> &#x02261; {<italic>p</italic><sub><italic>j</italic></sub>; <italic>j</italic> &#x0003D; 1, &#x022EF;, <italic>N</italic>}. The &#x0201C;cross-entropy&#x0201D; between <italic>Q</italic> and <italic>P</italic> is the Kullback-Leibler (KL) distance that is a very useful way to measure the difference between two probability distributions. The KL distance is</p>
<disp-formula id="E4"><label>(4)</label><mml:math id="M11"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mi>K</mml:mi><mml:mi>L</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>P</mml:mi><mml:mo>|</mml:mo><mml:mo>|</mml:mo><mml:mi>Q</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:munderover accentunder="false" accent="false"><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:munderover></mml:mstyle><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mrow><mml:mo class="qopname">log</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="true">(</mml:mo><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>q</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mrow><mml:mo stretchy="true">)</mml:mo></mml:mrow><mml:mtext>&#x000A0;</mml:mtext><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>This can be rewritten as</p>
<disp-formula id="E5"><label>(5)</label><mml:math id="M12"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mi>K</mml:mi><mml:mi>L</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>P</mml:mi><mml:mo>|</mml:mo><mml:mo>|</mml:mo><mml:mi>Q</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mi>S</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>P</mml:mi><mml:mo>,</mml:mo><mml:mi>Q</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>-</mml:mo><mml:mi>S</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>Thus the KL divergence represents the number of extra bits necessary to code a source whose symbols were drawn from the distribution <italic>P</italic>, given that the coder was designed for a source whose symbols were drawn from <italic>Q</italic>. Despite KL usually being referred as a distance measure between probability distributions, Kullback&#x02013;Leibler divergence is not a true metric as it does not have the property of symmetry.</p>
<p>On the other hand, Jensen&#x02013;Shannon divergence enables us to quantify the similitude between two distributions and has been utilized in statistics and probability theory. The Jensen&#x02013;Shannon divergence is defined as</p>
<disp-formula id="E6"><label>(6)</label><mml:math id="M13"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mi>J</mml:mi><mml:mi>S</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>P</mml:mi><mml:mo>|</mml:mo><mml:mo>|</mml:mo><mml:mi>Q</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mtext>&#x000A0;</mml:mtext><mml:mo>=</mml:mo><mml:mi>S</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>P</mml:mi><mml:mo>&#x0002B;</mml:mo><mml:mi>Q</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>-</mml:mo><mml:mi>S</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>/</mml:mo><mml:mn>2</mml:mn><mml:mo>-</mml:mo><mml:mi>S</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mi>Q</mml:mi></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mo>/</mml:mo><mml:mn>2</mml:mn><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>It is based on the Kullback&#x02013;Leibler divergence, with some remarkable and important differences: it is symmetric and always provides finite values.</p>
<p>The Jensen&#x02013;Shannon divergence, which evaluates the distinction between PDFs, is very helpful to analyze the symbolic configuration between various symbolic messages [<xref ref-type="bibr" rid="B59">59</xref>]. As non-linear measures ought to be considered to decipher the brain complex network, a straightforward way to investigate this inter-connectivity is using BP formalism in combination with <italic>JS</italic> disparity (or distance). Let us now consider a time series measured by a given electrode in a brain area that can be represented by a BP symbolization alphabet with probability distribution <italic>Q</italic> and another electrode sited in another brain area and with different time series represented by probability distribution, <italic>P</italic>. If we estimate <italic>JS</italic>(<italic>P</italic>||<italic>Q</italic>) a smaller <italic>JS</italic> implies greater interconnectivity between electrodes, and greater values of <italic>JS</italic> implies a lower inter-connectivity across them. Thus, the Jensen&#x02013;Shannon measure in combination with the BP approach can provide us a novel quantification of the network inter-connectivity across EEG electrodes [<xref ref-type="bibr" rid="B44">44</xref>].</p>
</sec>
<sec id="s4">
<title>4. EEG Dataset</title>
<p>Our point in this section is to portray the interconnectivity of the EEG frequency bands when the subjects play out a visuomotor or imagined assignment. We have considered for the present investigation the EEG visuomotor Movement/Imagery Dataset recorded utilizing BCI2000 instrumentation accessible through Physionet [<xref ref-type="bibr" rid="B12">12</xref>, <xref ref-type="bibr" rid="B41">41</xref>&#x02013;<xref ref-type="bibr" rid="B43">43</xref>, <xref ref-type="bibr" rid="B45">45</xref>, <xref ref-type="bibr" rid="B60">60</xref>, <xref ref-type="bibr" rid="B61">61</xref>]. <xref ref-type="fig" rid="F1">Figure 1</xref> shows the experimental setup that comprises an arrangement of various utilized electrodes.</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>Electrode arrangement as per the international 10&#x02013;20 system (as in [<xref ref-type="bibr" rid="B12">12</xref>, <xref ref-type="bibr" rid="B41">41</xref>&#x02013;<xref ref-type="bibr" rid="B43">43</xref>, <xref ref-type="bibr" rid="B45">45</xref>, <xref ref-type="bibr" rid="B61">61</xref>&#x02013;<xref ref-type="bibr" rid="B63">63</xref>]). The numbers below each electrode name indicate the order in which they appear in the recordings.</p></caption>
<graphic xlink:href="fphy-07-00115-g0001.tif"/>
</fig>
<p>The experimental setup of the BCI2000 framework [<xref ref-type="bibr" rid="B12">12</xref>, <xref ref-type="bibr" rid="B45">45</xref>] incorporates a set of 64 electrodes used to register the electrical responses of the cerebrum through the EEG signals while the subjects perform diverse assignments of visuomotor or imaginary kinds [<xref ref-type="bibr" rid="B12">12</xref>, <xref ref-type="bibr" rid="B41">41</xref>&#x02013;<xref ref-type="bibr" rid="B43">43</xref>, <xref ref-type="bibr" rid="B45">45</xref>, <xref ref-type="bibr" rid="B61">61</xref>&#x02013;<xref ref-type="bibr" rid="B63">63</xref>]. Each subject performed one of each of the four after assignments:
<list list-type="order">
<list-item><p>An objective shows up on either the left or the right half of the screen. The subject opens and shuts the matching hand until the objective vanishes. At that point the subject unwinds.</p></list-item>
<list-item><p>An objective shows up on either the left or the right half of the screen. The subject envisions opening and shutting the matching hand until the objective vanishes. At that point the subject unwinds.</p></list-item>
<list-item><p>An objective shows up on either the upper or the lower half of the screen. The subject opens and closes either the two hands (if the objective is on the upper half) or the two feet (if the objective is on the base) until the objective vanishes. At that point the subject unwinds.</p></list-item>
<list-item><p>An objective shows up on either the upper or the lower half of the screen. The subject envisions opening and closing either the two hands (if the objective is on the upper half) or the two feet (if the objective is on the base) until the objective vanishes. At that point the subject unwinds.</p></list-item>
</list></p>
<p>Eye blink artifacts were produced by quick motions of the eyelid along the cornea, for example, amid an eye squint. In any case, muscular artifacts were cautiously checked toward the start of each recording and confirmed all through the experiment [<xref ref-type="bibr" rid="B12">12</xref>, <xref ref-type="bibr" rid="B45">45</xref>, <xref ref-type="bibr" rid="B61">61</xref>&#x02013;<xref ref-type="bibr" rid="B63">63</xref>]. Significantly, in our present investigation the muscular and technical artifacts were discarded following the methodology exhibited in Schalk et al. [<xref ref-type="bibr" rid="B12">12</xref>] and Schalk and Mellinger [<xref ref-type="bibr" rid="B45">45</xref>]. That is, a Common Average Reference (CAR) is carried out before artifact rejection as demonstrated in Schalk et al. [<xref ref-type="bibr" rid="B12">12</xref>] and Schalk and Mellinger [<xref ref-type="bibr" rid="B45">45</xref>].</p>
<p>Various oscillatory rhythms have been connected to various parts of perception that are very significant to see how actions are prepared in the human brain [<xref ref-type="bibr" rid="B12">12</xref>]. The EEG records the electrical activity of the brain that by a sensory incitement, or a visuomotor output, exhibits distinctive rhythms such as delta (&#x02208; [1, 4) Hz), theta (&#x02208; [4, 8) Hz), alpha (&#x02208; [8, 13) Hz), beta (&#x02208; [13, 31) Hz), and gamma (&#x02265;31 Hz).</p>
<p>For a detailed description of the study, the design of the experiment, group of subjects, the condition of the experiment used and the EEG equipment used for the measurements, we refer the reader to [<xref ref-type="bibr" rid="B12">12</xref>, <xref ref-type="bibr" rid="B43">43</xref>, <xref ref-type="bibr" rid="B45">45</xref>, <xref ref-type="bibr" rid="B61">61</xref>&#x02013;<xref ref-type="bibr" rid="B63">63</xref>]. The classic scenario where the subjects are performing the motor action using an event-related desynchronization (ERD) analysis is carefully described for the different oscillation bands by Kim et al. [<xref ref-type="bibr" rid="B64">64</xref>].</p>
<p>For each subject and for each task we obtain the network, using the <italic>BP</italic> symbolization technique for each electrode and obtaining a weighted graph, with each weight given by the <italic>JS</italic> divergence, normalized by taking the maximum value between realized and imagined tasks. For completeness, we show an ERP signal of the current data in the <xref ref-type="supplementary-material" rid="SM1">Supplemental Material</xref>, and for further details we refer the reader to [<xref ref-type="bibr" rid="B43">43</xref>]). Specifically, we utilize the Kaiser filtering window created in Belitski et al. [<xref ref-type="bibr" rid="B65">65</xref>] to filter the raw signals for the diverse oscillation bands. The EEG are sampled at 160<italic>Hz</italic>. But due to the high frequency artifacts that obscured the EEG, and to expel variances at DC level and increment the signal to noise ratio, the records where passed first through a filter between 1 and 50 Hz utilizing a filter created in Belitski et al. [<xref ref-type="bibr" rid="B65">65</xref>].</p>
<p>After this filtering, each EEG signal was decomposed, using the Kaiser filtering window created in Belitski et al. [<xref ref-type="bibr" rid="B65">65</xref>], in the frequency bands given in <xref ref-type="table" rid="T1">Table 1</xref>. For further insights regarding the filtering we allude the reader to [<xref ref-type="bibr" rid="B41">41</xref>].</p>
<table-wrap position="float" id="T1">
<label>Table 1</label>
<caption><p>Frequency bands analyzed.</p></caption>
<table frame="hsides" rules="groups">
<thead><tr>
<th valign="top" align="left"><bold>Band</bold></th>
<th valign="top" align="center"><bold>Frequency interval (Hz)</bold></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Delta</td>
<td valign="top" align="center">[1, 4)</td>
</tr>
<tr>
<td valign="top" align="left">Theta</td>
<td valign="top" align="center">[4, 8)</td>
</tr>
<tr>
<td valign="top" align="left">Alpha 1</td>
<td valign="top" align="center">[8, 10)</td>
</tr>
<tr>
<td valign="top" align="left">Alpha 2</td>
<td valign="top" align="center">[10, 13)</td>
</tr>
<tr>
<td valign="top" align="left">Beta 1</td>
<td valign="top" align="center">[13, 18)</td>
</tr>
<tr>
<td valign="top" align="left">Beta 2</td>
<td valign="top" align="center">[18, 31)</td>
</tr>
<tr>
<td valign="top" align="left">Gamma 1</td>
<td valign="top" align="center">[31, 41)</td>
</tr>
<tr>
<td valign="top" align="left">Gamma 2</td>
<td valign="top" align="center">[41, 50)</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>Networks are usually built considering different thresholds, and then graphs are constructed. This framework allows us to analyze the functional connectome of the brain. We describe the diverse network rhythmic activity of the brain as indicated by unmistakable visuomotor and imagery tasks using an information theory approach. The main idea of the current analysis is to gain a better understanding of situations in which a given oscillation band recruits specific brain networks for a given oscillation supporting a distinction between the forms identified with attention and development of imaginary movements. We estimate the degree of network interconnectivity as the normalized Jensen-Shannon distance <italic>JS</italic> between two probabilities: one corresponding to the state of the system in one electrode and the state distribution taken of another electrode as reference state, that is to say by estimating the normalized Jensen&#x02013;Shannon distance between the BP probabilities across different electrodes sites as in Equation (6). We have normalized the Jensen&#x02013;Shannon distance by taking the maximum value between realized and imagined tasks. Due to the length of time series we consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1 for all BP estimations as in (Bandt and Pompe [<xref ref-type="bibr" rid="B38">38</xref>], Rosso and Masoller [<xref ref-type="bibr" rid="B39">39</xref>, <xref ref-type="bibr" rid="B40">40</xref>], Baravalle et al. [<xref ref-type="bibr" rid="B41">41</xref>, <xref ref-type="bibr" rid="B42">42</xref>]). So as to perform examinations inside the BP formalism, we have to meet the condition (<italic>M</italic> &#x0226B; <italic>D</italic>!); in this case we have 20,000 points for each case.</p>
<sec>
<title>4.1. Centrality</title>
<p>Graph theory is the investigation of systems of interacting elements, which are structures used to pose pairwise and/or multiple relations between them [<xref ref-type="bibr" rid="B66">66</xref>]. A graph in this setting is comprised of nodes which are associated by edges. The centrality of a node in a system <inline-formula><mml:math id="M14"><mml:mrow><mml:mi mathvariant="-tex-caligraphic">C</mml:mi></mml:mrow></mml:math></inline-formula> is a measure of the basic importance of the node. While thinking about a graph, closeness centrality of a given node is a measure of centrality in a system and is evaluated as the quantity of nodes less one, <italic>N</italic> &#x02212; 1, partitioned by the summation of the length of the shortest path between the node of interest and every single other node in the diagram.</p>
<p>That is</p>
<disp-formula id="E7"><label>(7)</label><mml:math id="M15"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="-tex-caligraphic">C</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>i</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mi>N</mml:mi><mml:mo>-</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mstyle displaystyle="true"><mml:msub><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mstyle><mml:mi>d</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow></mml:mfrac><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>where <italic>d</italic>(<italic>j, i</italic>) is the separation between vertices <italic>i</italic> and <italic>j</italic>. Closeness centrality measures how short the shortest paths are from node <italic>i</italic> to all nodes, and we have 62 nodes in total because we exclude the two reference electrodes <italic>T</italic><sub>9</sub> and <italic>T</italic><sub>10</sub>. We choose the closeness centrality because it is a helpful measure to estimate level of efficiency and convenience that gauges how quick the transmission of data would be through a given node all the available nodes [<xref ref-type="bibr" rid="B17">17</xref>, <xref ref-type="bibr" rid="B67">67</xref>&#x02013;<xref ref-type="bibr" rid="B72">72</xref>].</p>
</sec>
<sec>
<title>4.2. Statistical Analysis</title>
<p>As we mentioned previously, our objective is to focus on a better understanding of situations in which a given oscillation band recruits specific brain networks for a given oscillation supporting a distinction between the forms identified with attention and development of imaginary movements. In order to compare the closeness centrality for the different tasks, statistical tests are performed for each node. In consequence, we establish the following statistical analysis protocol for the obtained results of closeness centrality: (a) we first perform a <italic>t</italic>-test between imagined and realized tasks for each of the considered bands, and (b) in order to obtain a more accurate statistical test we also perform a false discovery rate (FDR) correction. We choose the Benjamini&#x02013;Hochberg methodology at a specified FDR of 5% as in Benjamini and Hochberg [<xref ref-type="bibr" rid="B73">73</xref>] and Nielsen et al. [<xref ref-type="bibr" rid="B74">74</xref>].</p>
</sec>
</sec>
<sec sec-type="results" id="s5">
<title>5. Results</title>
<p>In the following we show the analysis performed for the visuomotor task 1 and its corresponding imagined task 2. Our outcomes are equivalent for the visuomotor/imagery tasks 3 and 4. <xref ref-type="fig" rid="F2">Figures 2A,B</xref>, <xref ref-type="fig" rid="F3">3A,B</xref> display the mean of the interconnectivity for the 109 subjects when playing out the visuomotor assignment for the 64-channel EEG considering the diverse rhythms delta, theta, alpha 1 and alpha 2. <xref ref-type="fig" rid="F2">Figures 2C,D</xref>, <xref ref-type="fig" rid="F3">3C,D</xref> are equivalent to <xref ref-type="fig" rid="F2">Figures 2A,B</xref>, <xref ref-type="fig" rid="F3">3A,B</xref> but performing the imagined task. <xref ref-type="fig" rid="F4">Figures 4A,B</xref>, <xref ref-type="fig" rid="F5">5A,B</xref> depict the network averaged values of the interconnectivity for performing the visuomotor task when considering the beta 1, beta 2, gamma 1 and gamma 2 bands, respectively. <xref ref-type="fig" rid="F4">Figures 4C,D</xref>, <xref ref-type="fig" rid="F5">5C,D</xref> are the same as in <xref ref-type="fig" rid="F4">Figures 4A,B</xref>, <xref ref-type="fig" rid="F5">5A,B</xref> but performing the imagined task. Small differences can be appreciated between the network of the realized and imagined tasks. Furthermore, <xref ref-type="fig" rid="F6">Figures 6A,B</xref> show the node interconnectivity when considering the executed visuomotor task in view of the theta and alpha 1 bands for the electrode <italic>O</italic><sub><italic>z</italic></sub> (or node) in the visual cortex. <xref ref-type="fig" rid="F6">Figures 6C,D</xref> show the node interconnectivity when considering the imagined task taking into account the same node in the visual cortex. <xref ref-type="fig" rid="F6">Figures 6A&#x02013;D</xref> depict also the averaged values considering 109 subjects. We can appreciate from the previous figures that there are differences in the network interconnectivity for the different conditions, however the current results are not quantifying how different the networks are. That is to say we can not infer from the previous figures which are the most relevant network structures. For completeness in the <xref ref-type="supplementary-material" rid="SM1">Supplementary Material</xref> we also include the analysis for all the other bands that are not being depicted in <xref ref-type="fig" rid="F6">Figure 6</xref>.</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Network interconnectivity. <bold>(A,B)</bold> Show the network averaged values of the interconnectivity considering 109 subjects when performing the visuomotor task for the 64-channel EEG considering the different oscillation bands delta and theta. <bold>(C,D)</bold> Are the same as <bold>(A,B)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Delta oscillation band corresponds to [1, 4)<italic>Hz</italic> and theta oscillation band to [4, 8)<italic>Hz</italic>.</p></caption>
<graphic xlink:href="fphy-07-00115-g0002.tif"/>
</fig>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>Network interconnectivity. <bold>(A,B)</bold> Show the network averaged values of the interconnectivity considering 109 subjects when performing the visuomotor task for the 64-channel EEG considering the different oscillation bands alpha 1 and alpha 2. <bold>(C,D)</bold> Are the same as <bold>(A,B)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Alpha 1 oscillation band corresponds to [8, 10)<italic>Hz</italic> and alpha 2 oscillation band to [10, 13)<italic>Hz</italic>.</p></caption>
<graphic xlink:href="fphy-07-00115-g0003.tif"/>
</fig>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Network interconnectivity. <bold>(A,B)</bold> Show the network averaged values of the interconnectivity considering 109 subjects when performing the visuomotor task for the 64-channel EEG considering the different oscillation bands beta 1 and beta 2. <bold>(C,D)</bold> Are the same as <bold>(A,B)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Beta 1 oscillation band corresponds to [13, 18)<italic>Hz</italic> and beta 2 oscillation band to [18, 31)<italic>Hz</italic>.</p></caption>
<graphic xlink:href="fphy-07-00115-g0004.tif"/>
</fig>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>Network interconnectivity. <bold>(A,B)</bold> Show the network averaged values of the interconnectivity considering 109 subjects when performing the visuomotor task for the 64-channel EEG considering the different oscillation bands alpha 1 and alpha 2. <bold>(C,D)</bold> Are the same as <bold>(A,B)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Gamma 1 oscillation band corresponds to [31, 41)<italic>Hz</italic> and gamma 2 oscillation band to [41, 50)<italic>Hz</italic>.</p></caption>
<graphic xlink:href="fphy-07-00115-g0005.tif"/>
</fig>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p><bold>(A,B)</bold> Show the node interconnectivity when considering the executed visuomotor task and taking the theta and alpha 1 band for the electrode Oz (or node) in the visual cortex. <bold>(C,D)</bold> Show the node interconnectivity when considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1.</p></caption>
<graphic xlink:href="fphy-07-00115-g0006.tif"/>
</fig>
<p>In order to quantify the structural relevance of each node for the realized and imagined tasks, we investigate the closeness centrality of different nodes. <xref ref-type="fig" rid="F7">Figures 7A,B</xref> show the closeness centrality <inline-formula><mml:math id="M16"><mml:mrow><mml:mi mathvariant="-tex-caligraphic">C</mml:mi></mml:mrow></mml:math></inline-formula>, as in Equation (7), taking into account the average over 109 subjects for the 62-channel EEG considering the realized task when considering delta and theta, respectively. <xref ref-type="fig" rid="F7">Figures 7C,D</xref>, are the same as in <xref ref-type="fig" rid="F7">Figures 7A,B</xref> but performing the imagined task. Let us emphasize that <xref ref-type="fig" rid="F8">Figures 8A</xref>, <xref ref-type="fig" rid="F9">9A</xref> depict the closeness centrality <inline-formula><mml:math id="M17"><mml:mrow><mml:mi mathvariant="-tex-caligraphic">C</mml:mi></mml:mrow></mml:math></inline-formula> [as in Equation (7)] considering the alpha 1 and alpha 2 bands, respectively, taking into account the average over 109 subjects for the 62-channels EEG considering the realized task. <xref ref-type="fig" rid="F8">Figures 8B</xref>, <xref ref-type="fig" rid="F9">9B</xref> are the same as in <xref ref-type="fig" rid="F8">Figures 8A</xref>, <xref ref-type="fig" rid="F9">9A</xref> but executing the imagined task. <xref ref-type="fig" rid="F10">Figures 10A,B</xref>, <xref ref-type="fig" rid="F11">11A,B</xref> depict the closeness centrality <inline-formula><mml:math id="M18"><mml:mrow><mml:mi mathvariant="-tex-caligraphic">C</mml:mi></mml:mrow></mml:math></inline-formula> when realizing the visuomotor task considering the beta 1, beta 2, gamma 1 and gamma 2 bands, respectively. <xref ref-type="fig" rid="F10">Figures 10C,D</xref>, <xref ref-type="fig" rid="F11">11C,D</xref> are the same as in <xref ref-type="fig" rid="F10">Figures 10A,B</xref>, <xref ref-type="fig" rid="F11">11A,B</xref> but performing the imagined task. The electrodes <italic>T</italic><sub>9</sub> and <italic>T</italic><sub>10</sub> have been excluded from the current analysis of the nodes centrality as they are reference electrodes [<xref ref-type="bibr" rid="B43">43</xref>].</p>
<fig id="F7" position="float">
<label>Figure 7</label>
<caption><p>Closeness centrality. <bold>(A,B)</bold> Show the nodes&#x00027; closeness centrality considering 109 subjects when performing the visuomotor task for the 62-channels EEG considering the different oscillation bands delta and theta. <bold>(C,D)</bold> Are the same as <bold>(A,B)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Delta oscillation band corresponds to [1, 4)<italic>Hz</italic> and theta oscillation band to [4, 8)<italic>Hz</italic>.</p></caption>
<graphic xlink:href="fphy-07-00115-g0007.tif"/>
</fig>
<fig id="F8" position="float">
<label>Figure 8</label>
<caption><p>Closeness centrality. <bold>(A)</bold> Shows the node closeness centrality considering 109 subjects when performing the visuomotor task for the 62-channels EEG considering the oscillation band alpha 1. <bold>(B)</bold> Is the same as <bold>(A)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Alpha 1 oscillation band corresponds to [8, 10)<italic>Hz</italic>.</p></caption>
<graphic xlink:href="fphy-07-00115-g0008.tif"/>
</fig>
<fig id="F9" position="float">
<label>Figure 9</label>
<caption><p>Closeness centrality. <bold>(A)</bold> Shows the node closeness centrality considering 109 subjects when performing the visuomotor task for the 62-channels EEG considering the oscillation band alpha 2. <bold>(B)</bold> Is the same as <bold>(A)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Alpha 2 oscillation band corresponds to [10,13)<italic>H</italic>z.</p></caption>
<graphic xlink:href="fphy-07-00115-g0009.tif"/>
</fig>
<fig id="F10" position="float">
<label>Figure 10</label>
<caption><p>Closeness centrality. <bold>(A,B)</bold> Show the nodes&#x00027; closeness centrality considering 109 subjects when performing the visuomotor task for the 62-channels EEG considering the different oscillation bands beta 1 and beta 2. <bold>(C,D)</bold> Are the same as <bold>(A,B)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Beta 1 oscillation band corresponds to [13, 18)<italic>Hz</italic> and beta 2 oscillation band to [18, 31)<italic>Hz</italic>.</p></caption>
<graphic xlink:href="fphy-07-00115-g0010.tif"/>
</fig>
<fig id="F11" position="float">
<label>Figure 11</label>
<caption><p>Closeness centrality. <bold>(A,B)</bold> Show the nodes&#x00027; centrality considering 109 subjects when performing the visuomotor task for the 62-channels EEG considering the different oscillation bands gamma 1 and gamma 2. <bold>(C,D)</bold> Are the same as <bold>(A,B)</bold> but considering the imagined task. We consider <italic>D</italic> &#x0003D; 6 and &#x003C4; &#x0003D; 1. Gamma 1 oscillation band corresponds to [31, 41)<italic>Hz</italic> and gamma 2 oscillation band to [41, 50)<italic>Hz</italic>.</p></caption>
<graphic xlink:href="fphy-07-00115-g0011.tif"/>
</fig>
<p>In the case of the delta band, <italic>TP</italic><sub>7</sub> showed the highest closeness centrality for imagined and realized tasks. While in the theta band <italic>FP</italic><sub>1</sub>, <italic>FP</italic><sub><italic>z</italic></sub>, and <italic>FP</italic><sub>2</sub> depicted the highest centrality, both for both tasks. When considering the beta 1, the highest centrality is given by <italic>AF</italic><sub>8</sub>, <italic>T</italic><sub>8</sub>, <italic>O</italic><sub>2</sub>, and <italic>O</italic><sub><italic>z</italic></sub> for the realized task. In the case of the imagined task, beta 1 has the highest centrality for <italic>AF</italic><sub>7</sub>, <italic>AF</italic><sub>8</sub>, <italic>F</italic><sub>6</sub>, <italic>T</italic><sub>8</sub>, and <italic>O</italic><sub><italic>z</italic></sub>. Beta 2 depicted the highest centrality in <italic>AF</italic><sub>8</sub> for the realized task and <italic>AF</italic><sub>7</sub>, <italic>AF</italic><sub>8</sub> for the imagined task. Alpha 1 displays higher centrality for <italic>FP</italic><sub>1</sub>, <italic>FP</italic><sub><italic>z</italic></sub>, <italic>FP</italic><sub>2</sub>, <italic>F</italic><sub>7</sub>, <italic>F</italic><sub>6</sub>, <italic>FC</italic><sub>2</sub>, <italic>FC</italic><sub>4</sub>, <italic>C</italic><sub>4</sub>, and <italic>P</italic><sub>2</sub> for the realized task. When considering the imagined task alpha 1 showed the highest centrality for the nodes <italic>FP</italic><sub>1</sub>, <italic>FP</italic><sub>2</sub>, <italic>AF</italic><sub>8</sub>, <italic>AF</italic><sub>3</sub>, <italic>F</italic><sub>3</sub>, <italic>F</italic><sub>2</sub>, <italic>FT</italic><sub>7</sub>, <italic>FC</italic><sub>3</sub>, <italic>FC</italic><sub>4</sub>, <italic>P</italic><sub>2</sub>, <italic>P</italic><sub>7</sub>, <italic>T</italic><sub>8</sub>, <italic>PO</italic><sub>4</sub>, <italic>O</italic><sub><italic>z</italic></sub>, and <italic>O</italic><sub>2</sub>. In contrast the highest centrality of the alpha 2 band is given by the nodes <italic>FP</italic><sub><italic>z</italic></sub>, <italic>FP</italic><sub>2</sub>, <italic>T</italic><sub>8</sub>, <italic>O</italic><sub>1</sub>, and <italic>O</italic><sub><italic>z</italic></sub> for the realized task. The highest centrality of the imagined task is given by <italic>FP</italic><sub><italic>z</italic></sub>, <italic>O</italic><sub>1</sub>, and <italic>PO</italic><sub>4</sub> for alpha 2. Gamma 1 and gamma 2 presented the highest centrality in <italic>O</italic><sub><italic>z</italic></sub>, <italic>O</italic><sub>2</sub>, and <italic>T</italic><sub><italic>z</italic></sub> for the realized and imagined tasks. Overall, it is important to point out that delta, theta, beta and gamma bands show lower closeness centrality and therefore depict a lower efficiency of the information of the data that could be transmitted through a given node to all the available nodes.</p>
<p>We find no significant differences between the realized and imagined tasks for most of the different bands, with the exception of the alpha 1 and alpha 2 bands that depict an unequal closeness centrality in several nodes of the network when comparing both tasks (see <xref ref-type="fig" rid="F8">Figures 8A,B</xref>, <xref ref-type="fig" rid="F9">9A,B</xref>). After performing the FDR correction we find no significant differences between realized and imagined tasks when considering the delta, theta, beta 1, beta 2, gamma 1 and gamma 2 bands. In the case of the alpha 1 band (see <xref ref-type="fig" rid="F8">Figures 8A,B</xref>), as mentioned we first performed a t-test between imagined and realized tasks obtaining 26 sites with significant differences. After performing a FDR correction we find 17 nodes/sites that present significant differences between imagined and non-imagined tasks. The electrodes that accomplished both tests were <italic>FP</italic><sub><italic>z</italic></sub>, <italic>AF</italic><sub>8</sub>, <italic>F</italic><sub>7</sub>, <italic>F</italic><sub>8</sub>, <italic>F</italic><sub>3</sub>, <italic>F</italic><sub>2</sub>, <italic>F</italic><sub>6</sub>, <italic>FT</italic><sub>7</sub>, <italic>AF</italic><sub><italic>z</italic></sub>, <italic>FC</italic><sub>3</sub>, <italic>C</italic><sub>5</sub>, <italic>C</italic><sub>2</sub>, <italic>T</italic><sub>8</sub>, <italic>PO</italic><sub>7</sub>, <italic>PO</italic><sub>8</sub>, <italic>C</italic><sub>1</sub>, and <italic>O</italic><sub><italic>z</italic></sub>. In the case of alpha 2 (see <xref ref-type="fig" rid="F9">Figures 9A,B</xref>) there were eight sites that showed significant differences when performing the t-test, and six electrodes presented significant differences when applying a FDR correction between tasks. The electrodes that accomplished both tests were <italic>T</italic><sub>8</sub>, <italic>TP</italic><sub>7</sub>, <italic>P</italic><sub>7</sub>, <italic>O</italic><sub><italic>z</italic></sub>, <italic>I</italic><sub><italic>z</italic></sub>, and <italic>PO</italic><sub>4</sub>. Finally, for completeness, <xref ref-type="fig" rid="F12">Figures 12A&#x02013;C</xref> depict the results of the closeness centrality derived from statistical comparison between realized and imagined tasks for all the significant nodes within alpha 1. <xref ref-type="fig" rid="F12">Figure 12D</xref> shows all the significant nodes within the alpha 2 band. Let us emphasize that the estimation of the network closeness centrality played an ultimate role, as when we implemented other network measures they did not produce any quantifiable difference between realized and imagined tasks for the different analyzed bands. Here, a systematic method in which nodes are weighted by closeness centrality was proposed. We demonstrate how the combination of the estimation of the Jensen&#x02013;Shannon divergence of the BP probabilities across different nodes encompassed with calculations of the nodes closeness centrality has significance to distinguish imagined from realized motor tasks. We found a higher degree of closeness centrality in the case of the imagined task when compared with the realized ones, looking upon the alpha band. Thus these results shows that imagined processes are linked to changes in the alpha levels of centrality of the different nodes in the brain. Overall we emphasize that the alpha 1 band shows a higher level of closeness centrality than the other bands, therefore it depicts a quicker level information flow from a given node to other nodes.</p>
<fig id="F12" position="float">
<label>Figure 12</label>
<caption><p>Statistical comparison and closeness centrality. <bold>(A&#x02013;C)</bold> Depict the closeness centrality for the realized and imagined tasks considering the significant nodes for the alpha 1 band. <bold>(D)</bold> Is the same as <bold>(A&#x02013;C)</bold> but considering the alpha 2 band. In all cases: dark gray bars, realized task; light gray bars, imagined task.</p></caption>
<graphic xlink:href="fphy-07-00115-g0012.tif"/>
</fig>
</sec>
<sec id="s6">
<title>6. Conclusion and Discussions</title>
<p>Attention is a mechanism required for focusing on what is critical at each moment of time, while suppressing any unessential information. This mechanism is also required to perform mental imagery, activating the synchronized network of multiple areas of the brain [<xref ref-type="bibr" rid="B45">45</xref>]. This synchronized activity of many neurons communicating with one another generates brain waves [<xref ref-type="bibr" rid="B45">45</xref>]. Brain waves are rhythmic oscillation patterns that can be registered as macroscopic oscillations utilizing EEG sensors on the scalp. The descriptions are quite broad: delta rhythmic are related to sleep states; theta might be entrance to further understanding learning and memory; alpha is usually related to attention, lucid thinking and integration; beta is present during the state of alert and problem solving; and gamma rhythms modulate perception and consciousness [<xref ref-type="bibr" rid="B45">45</xref>]. Moreover, brain oscillation rhythms can provide hints about the network functionality during imagined and realized tasks. In our current study we have considered the causality of the EEG signals using the BP approach, and through a statistical analysis that combined the Jensen&#x02013;Shannon distance with the estimation of the closeness centrality we estimate the level efficiency on data transmission for a given node to all the available nodes taking into account the different rhythmic oscillation bands. Our current results emphasize the relevance of the alpha 1 band when detecting nodes that spread information with different efficiency through the graph for realized and imagined tasks.</p>
<p>We propose an effective technique that enables us to determine quantitatively the amount of the node closeness centrality inside the diverse rhythms considering the causality of the EEG signals. So as to do it thus, we exactly evaluate the distinctive highlights of oscillatory patterns considering keen estimates representing the causal structure of the signal utilizing the BP procedure. More specifically, we estimate the network interconnectivity by estimating the normalized Jensen&#x02013;Shannon distance between the BP probabilities across different nodes, quantifying the non-linear dynamics of the EEG signals. We choose thereafter to compute the closeness centrality because it is a helpful measure to estimate the level of efficiency and convenience that gauges how quick the transmission of data would be through a given node all the available nodes [<xref ref-type="bibr" rid="B67">67</xref>&#x02013;<xref ref-type="bibr" rid="B72">72</xref>]. Our methodology enables us to characterize the &#x0201C;closeness centrality properties&#x0201D; of various nodes inside the EEG rhythms, considering the causality of the signal and gathering the rising dynamical properties of the diverse oscillation patterns of the brain while performing distinctive visuomotor or imagery tasks. That is to say in the current paper, we analyze EEG network organization through the closeness centrality to study how to discriminate imagined and non-imagined tasks for the different rhythmic oscillations, showing that the alpha 1 bands allow us to discriminate between both assignments. Thus, we determine that the current approach combining the BP estimation with the Jensen-Shannon distance and the closeness centrality is a viable option for classification of hand realized and imagined signals.</p>
<p>It has been found that alpha frequency oscillations posses an important role in inhibitory control actions managing access of data of a cognition procedure and working memory [<xref ref-type="bibr" rid="B75">75</xref>&#x02013;<xref ref-type="bibr" rid="B77">77</xref>]. Our findings show that several nodes within the gamma 1 band have an overall higher amount of closeness centrality during the imagined task in comparison to realized tasks. These higher amounts of centrality are located within the pre-motor, motor, and visual cortex areas. Thus, we can conclude that the imagined cognitive processes coincide with higher alpha 1 levels of closeness centrality of the different nodes. Our discoveries underscore the significance of the alpha band while taking part in cognitive tasks. That is in concurrence with strong proof that EEG alpha power is especially susceptible to different imagination-related requests, and that is happening due to creativity interventions [<xref ref-type="bibr" rid="B78">78</xref>]. We suggest that increased levels of centrality of several nodes for alpha 1 levels during the imaginative tasks might be important neurocognitive processes related to the internal attention required to perform mental imagery tasks.</p>
<p>As far as we can tell, there is still no ideal way to deal with the construction of a brain computer interphase (BCI) based on motor imagined tasks (MI-BCI, [<xref ref-type="bibr" rid="B79">79</xref>]). Specifically, features extraction and determination of relevant patterns and biomarkers for developing a successful MI-BCI are still under debate. Thus, it is extremely useful to investigate new methodologies that can offer a better understanding of how motor imagined patterns and connectivity differs from the non-imagined/realized activities. Recently, new research has investigated the possibility of taking measures that were originally developed in graph theory for data classification as they could provide important information about the connectivity [<xref ref-type="bibr" rid="B80">80</xref>]. In particular, a recent study has shown that graph metrics can be used for EEG-BCIs based on hand motor imagery graphs, as they are a feasible option for classification of hand motor imagined signals [<xref ref-type="bibr" rid="B81">81</xref>]. A recent study showed that the activity of the globulous pallidus is significantly reduced during imagined locomotion in patients with Parkinson disease when compared to healthy subjects [<xref ref-type="bibr" rid="B82">82</xref>]. Importantly the authors showed, using fMRI measures, that Parkinson disease patients displayed larger beta weights in the visuomotor zone amid envisioned turning contrasted with forward or in reverse while controls did not, and that overground marching speed is associated with beta weights amid imagined marching in a few locomotor areas in patients with Parkinson disease and not in controls [<xref ref-type="bibr" rid="B82">82</xref>]. The early detection and diagnosis based on extracting features of the neuronal networks EEG topology thought imagined tasks can be of ultimate help for understanding brain functions and neuronal diseases. When one performs a network analysis, markers of closeness centrality allow us to find the most relevant vertices within a graph. Applications means identifying the most important structure of the neuronal network, therefore the main relevance of the nodes&#x00027; centrality is identifying the different networks that might be related with neural diseases. The detection of those differences between realized and imagined features is a relevant highlight of the EEG topology that can be of assistance for inferring the brain functions. Moreover, we plan future related work to perform estimations of wavelet phase coherence to obtain the connectivity matrices for the different oscillations bands and to estimate the betweenness centrality across them to identify possible nodes that might mediate communication with the other nodes for the different imagined/realized tasks as performed in Makarov et al. [<xref ref-type="bibr" rid="B83">83</xref>]. We suggest that the current tool that combines a subtle information theoretical approach, representing the causality of the signal together with a quantification of the levels of centrality for the different nodes, can be very useful for early detection of neuronal diseases.</p>
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<sec sec-type="data-availability" id="s7">
<title>Data Availability</title>
<p>The datasets EEGMIDB for this study can be found in the physionet database. (<ext-link ext-link-type="uri" xlink:href="https://archive.physionet.org/pn4/eegmmidb/">https://archive.physionet.org/pn4/eegmmidb/</ext-link>).</p>
</sec>
<sec id="s8">
<title>Author Contributions</title>
<p>Authors contributed equally in the design of this research as well as in the writing of this paper. All authors have read and approved the final manuscript.</p>
<sec>
<title>Conflict of Interest Statement</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
</sec>
</body>
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<sec sec-type="supplementary-material" id="s9">
<title>Supplementary Material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fphy.2019.00115/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fphy.2019.00115/full#supplementary-material</ext-link></p>
<supplementary-material xlink:href="Data_Sheet_1.PDF" id="SM1" mimetype="application/pdf" xmlns:xlink="http://www.w3.org/1999/xlink"/>
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<fn-group>
<fn fn-type="financial-disclosure"><p><bold>Funding.</bold> We gratefully acknowledge PIP 11220130100327CO (2014/2016) CONICET, Argentina (FM) and Universidad Nacional de La Plata, Argentina (project 11/X812).</p></fn>
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