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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Physiol.</journal-id>
<journal-title>Frontiers in Physiology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Physiol.</abbrev-journal-title>
<issn pub-type="epub">1664-042X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fphys.2015.00190</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physiology</subject>
<subj-group>
<subject>General Commentary</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Commentary: Pi&#x000E9;ron&#x00027;s law is not just an artifact of the response mechanism</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name><surname>Medina</surname> <given-names>Jos&#x000E9; M.</given-names></name>
<xref ref-type="author-notes" rid="fn001"><sup>&#x0002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/11464/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>D&#x000ED;az</surname> <given-names>Jos&#x000E9; A.</given-names></name>
<uri xlink:href="http://loop.frontiersin.org/people/106072/overview"/>
</contrib>
</contrib-group>
<aff><institution>Departamento de &#x000D3;ptica, Facultad de Ciencias, Edificio Mecenas, Universidad de Granada</institution> <country>Granada, Spain</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Paolo Allegrini, Consiglio Nazionale delle Ricerche, Italy</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Willy Wong, University of Toronto, Canada; Gerardo Aquino, Imperial College London, UK</p></fn>
<fn fn-type="corresp" id="fn001"><p>&#x0002A;Correspondence: Jos&#x000E9; M. Medina, <email>jmedinaru&#x00040;cofis.es</email></p></fn>
<fn fn-type="other" id="fn002"><p>This article was submitted to Fractal Physiology, a section of the journal Frontiers in Physiology</p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>30</day>
<month>06</month>
<year>2015</year>
</pub-date>
<pub-date pub-type="collection">
<year>2015</year>
</pub-date>
<volume>6</volume>
<elocation-id>190</elocation-id>
<history>
<date date-type="received">
<day>15</day>
<month>04</month>
<year>2015</year>
</date>
<date date-type="accepted">
<day>16</day>
<month>06</month>
<year>2015</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2015 Medina and D&#x000ED;az.</copyright-statement>
<copyright-year>2015</copyright-year>
<copyright-holder>Medina and D&#x000ED;az</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) or licensor 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>
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<related-article id="RA1" related-article-type="commentary-article" journal-id="J Math Psychol" journal-id-type="nlm-ta" vol="62" page="22" xlink:href="10.1016/j.jmp.2014.09.006" ext-link-type="doi">A commentary on <article-title>Pi&#x000E9;ron&#x00027;s law is not just an artifact of the response mechanism</article-title> by Donkin, C., and van Maanen, L. (2014). J. Math. Psychol. 62&#x02013;63, 22&#x02013;32. doi: <object-id>10.1016/j.jmp.2014.09.006</object-id></related-article>
<kwd-group>
<kwd>human reaction time</kwd>
<kwd>power laws</kwd>
<kwd>decision making</kwd>
<kwd>information entropy</kwd>
<kwd>statistical physics</kwd>
<kwd>fractals</kwd>
</kwd-group>
<counts>
<fig-count count="1"/>
<table-count count="0"/>
<equation-count count="4"/>
<ref-count count="37"/>
<page-count count="4"/>
<word-count count="2500"/>
</counts>
</article-meta>
</front>
<body>
<p>It has long been known that the mean human reaction/response time (RT), <italic>t<sub>RT</sub></italic>, decreases as the stimulus strength or intensity <italic>S</italic> increases (Cattell, <xref ref-type="bibr" rid="B3">1886</xref>), reaching an asymptotic value or plateau, <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub>, at very high <italic>S</italic>-values in all sensory modalities. A well-established power law, namely, Pi&#x000E9;ron&#x00027;s law, describes mathematically that empirical relationship (Pi&#x000E9;ron, <xref ref-type="bibr" rid="B27">1914</xref>; Luce, <xref ref-type="bibr" rid="B12">1986</xref>):
<disp-formula id="E1"><label>(1)</label><mml:math id="M1"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>t</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:msub><mml:mi>T</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:mi>k</mml:mi><mml:msup><mml:mi>S</mml:mi><mml:mrow><mml:mo>&#x02212;</mml:mo><mml:mi>p</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:math></disp-formula>
where <italic>k</italic> and <italic>p</italic> are coefficients; the latter being a fractional exponent that controls the <italic>RT</italic> decay. Donkin and van Maanen has investigated the origin of Pi&#x000E9;ron&#x00027;s law based on a version of the Linear Ballistic Accumulator model. They concluded that Pi&#x000E9;ron&#x00027;s law is not due only to a decision making process. Various types of models have been proposed for describing the foundations of Pi&#x000E9;ron&#x00027;s law (Link, <xref ref-type="bibr" rid="B11">1992</xref>; Baird, <xref ref-type="bibr" rid="B1">1997</xref>; Stafford and Gurney, <xref ref-type="bibr" rid="B32">2004</xref>; Hsu, <xref ref-type="bibr" rid="B8">2005</xref>; Palmer et al., <xref ref-type="bibr" rid="B24">2005</xref>; Stafford et al., <xref ref-type="bibr" rid="B33">2011</xref>; Servant et al., <xref ref-type="bibr" rid="B31">2014</xref>; Verdonck and Tuerlinckx, <xref ref-type="bibr" rid="B36">2014</xref>). The model proposed by Donkin and van Maanen belongs to an influential class of models in mathematical psychology, i.e., sequential sampling models. In general, these models of Pi&#x000E9;ron&#x00027;s law assume the existence of an internal variable threshold. From the stimulus onset, there is an accumulation of noisy &#x0201C;sensory information&#x0201D; or &#x0201C;evidence&#x0201D; until a response criterion is reached. However, the concept of information is not properly defined within the context of information theory and plays no role. A decisional stage is usually implemented in the form of random walk, diffusion, and accumulator models. Despite these models mimic the functional form of Pi&#x000E9;ron&#x00027;s law, it is not clear whether they are able to explain the internal structure of <italic>k</italic> and <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub> in Equation (1) and to provide more detailed predictions based on threshold mechanisms. For instance, all these models often postulate that the asymptotic term <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub> is nearly invariant and includes non-decision components (e.g., the motor execution time) that do not hold a chronological order. However, <italic>k</italic> and <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub> span a range of experimental values and depend on early sensory processing (Pins and Bonnet, <xref ref-type="bibr" rid="B28">1997</xref>; Plainis and Murray, <xref ref-type="bibr" rid="B29">2000</xref>; Murray and Plainis, <xref ref-type="bibr" rid="B19">2003</xref>).</p>
<p>There is an information-theoretic approach, which is rarely mentioned in the literature of Pi&#x000E9;ron&#x00027;s law, that derives Equation (1) from an optimal information process in sensory perception. In this framework, the first stage of RTs always corresponds to an efficient stimulus encoder. Only after this initial stage there is a <italic>bona fide</italic> accumulation of information over time, &#x00394;<italic>H</italic> &#x0003E; 0 (e.g., measured in bits), that is related with power law behavior at the threshold, &#x003B2;S<sup>p</sup><sub>0</sub>. <italic>S</italic><sub>0</sub>, and &#x003B2; indicate an internal threshold and a normalization coefficient, respectively. Pi&#x000E9;ron&#x00027;s law results from a temporal sequence of events that differentiates those components near the threshold <italic>S</italic><sub>0</sub> from those at suprathreshold conditions (S &#x0003E; S<sub>0</sub>). The coefficient <italic>k</italic> follows a power law (Norwich et al., <xref ref-type="bibr" rid="B22">1989</xref>; Norwich, <xref ref-type="bibr" rid="B21">1993</xref>):
<disp-formula id="E2"><label>(2)</label><mml:math id="M2"><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>t</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:msub><mml:mi>T</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:msub><mml:msubsup><mml:mi>S</mml:mi><mml:mn>0</mml:mn><mml:mi>p</mml:mi></mml:msubsup></mml:mrow></mml:math></disp-formula></p>
<p>The asymptotic term <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub> only contains the initial encoding time <italic>t</italic><sub>0</sub> and &#x003B2;S<sup>p</sup><sub>0</sub>, and it obeys a similar power law (Medina, <xref ref-type="bibr" rid="B14a">2012</xref>):
<disp-formula id="E3"><label>(3)</label><mml:math id="M3"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mrow><mml:mi>R</mml:mi><mml:msub><mml:mi>T</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>t</mml:mi><mml:mn>0</mml:mn></mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mi>&#x003B2;</mml:mi><mml:msubsup><mml:mi>S</mml:mi><mml:mn>0</mml:mn><mml:mi>p</mml:mi></mml:msubsup></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula></p>
<p>Equation (2) corroborates that the coefficient <italic>k</italic> has a direct link with a threshold mechanism in human vision (Plainis and Murray, <xref ref-type="bibr" rid="B29">2000</xref>; Murray and Plainis, <xref ref-type="bibr" rid="B19">2003</xref>; Medina and Diaz, <xref ref-type="bibr" rid="B16">2005</xref>, <xref ref-type="bibr" rid="B17">2006</xref>).</p>
<p>There is a chronological order that cannot be violated, namely, <italic>t</italic><sub>RT</sub> &#x0003E; t<sub>RT<sub>0</sub></sub> &#x0003E; t<sub>0</sub> &#x0003E; 0. This is a direct consequence of &#x00394;<italic>H</italic> and involves the principle of causality over time, which states that the effect cannot be before the cause. The formation of a threshold at <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub> cannot precede the stimulus encoding at <italic>t</italic><sub>0</sub>, and those processes at suprathreshold conditions at <italic>t<sub>RT</sub></italic> cannot precede those at <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub> either (Medina et al., <xref ref-type="bibr" rid="B18">2014</xref>). Further, Pi&#x000E9;ron&#x00027;s law is shape-invariant under rescaling (Chater and Brown, <xref ref-type="bibr" rid="B4">1999</xref>) in a fractal-like process. In the rate domain (1/RT), Pi&#x000E9;ron&#x00027;s law has a direct link with the Naka-Rushton equation in neurophysiology (Naka and Rushton, <xref ref-type="bibr" rid="B20">1966</xref>; Carandini and Heeger, <xref ref-type="bibr" rid="B2">2012</xref>). Let, <italic>R</italic> &#x0003D; 1/<italic>t<sub>RT</sub></italic>, and <italic>R<sub>M</sub></italic> &#x0003D; 1/<italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub>, from Equations (1) and (2) (Medina, <xref ref-type="bibr" rid="B14">2009</xref>):
<disp-formula id="E4"><label>(4)</label><mml:math id="M4"><mml:mrow><mml:mi>R</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>R</mml:mi><mml:mi>M</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:msup><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mfrac><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow><mml:mi>S</mml:mi></mml:mfrac></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mi>p</mml:mi></mml:msup></mml:mrow></mml:mfrac></mml:mrow></mml:math></disp-formula></p>
<p>Equations (2) and (3) show that threshold impairment in <italic>S</italic><sub>0</sub> leads to longer RTs and consequently, it modifies Pi&#x000E9;ron&#x00027;s law in Equation (1). We exemplify the non-trivial effects of anomalous power law behavior &#x003B2;S<sup>p</sup><sub>0</sub> in Pi&#x000E9;ron&#x00027;s law in two different scenarios. <italic>&#x003B2;</italic>, <italic>S</italic><sub>0</sub>, and <italic>p</italic> could vary based on several experimental factors. Similar examples follow in the same way. In the first example, we illustrate Pi&#x000E9;ron&#x00027;s law in amblyopia. Amblyopia (usually called &#x0201C;lazy eye&#x0201D;) affects approximately 3% of human population and is a combination of visual deficits that impairs binocular vision from physiological alterations during early development (Ciuffreda et al., <xref ref-type="bibr" rid="B5">1991</xref>; Howard, <xref ref-type="bibr" rid="B7">2002</xref>). Figure <xref ref-type="fig" rid="F1">1A</xref> simulates the typical variation of the reciprocal of <italic>S</italic><sub>0</sub> for spatial sine-wave gratings in normal and amblyopic vision. Threshold values <italic>S</italic><sub>0</sub> are higher in the amblyopic eye at high spatial frequencies (Ciuffreda et al., <xref ref-type="bibr" rid="B5">1991</xref>). This deficit is the principal responsible for higher &#x003B2;S<sup>p</sup><sub>0</sub>, <italic>k</italic>, and <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub> values in Equation (1) and consequently, for longer RTs in amblyopic vision (Figure <xref ref-type="fig" rid="F1">1B</xref>) (Pianta and Kalloniatis, <xref ref-type="bibr" rid="B26">1998</xref>). In the rate domain (Equation 4), amblyopic vision is limited because it gives saturated responses sooner (Figure <xref ref-type="fig" rid="F1">1C</xref>).</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p><bold>Examples of Pi&#x000E9;ron&#x00027;s law</bold>. <bold>(A)</bold> Double logarithmic plot of the contrast sensitivity function (1/threshold) as a function of the spatial frequency for sine-wave gratings. Points labeled as &#x0201C;1&#x0201D; and &#x0201C;2&#x0201D; indicate two threshold values at the same spatial frequency that correspond to normal and amblyopic vision, respectively (Ciuffreda et al., <xref ref-type="bibr" rid="B5">1991</xref>). In both cases the adapting conditions were the same and fixed. <bold>(B)</bold> Linear plot of Pi&#x000E9;ron&#x00027;s law as a function of the stimulus strength <italic>S</italic>. Vertical dash and dash-dot lines represent those threshold values labeled as &#x0201C;1&#x0201D; and &#x0201C;2&#x0201D; in <bold>(A)</bold>, respectively. Solid lines labeled as &#x0201C;1&#x0201D; and &#x0201C;2&#x0201D; show the corresponding Pi&#x000E9;ron&#x00027;s law in normal and amblyopic vision, respectively (Pianta and Kalloniatis, <xref ref-type="bibr" rid="B26">1998</xref>). Simulation parameters in normal vision: <italic>t</italic><sub>0</sub> &#x0003D; 44, &#x003B2; &#x0003D; 294.39, <italic>S</italic><sub>0</sub> &#x0003D; 0.52, <italic>p</italic> &#x0003D; 0.5. Amblyopic eye: <italic>t</italic><sub>0</sub> &#x0003D; 44, &#x003B2; &#x0003D; 439.35, <italic>S</italic><sub>0</sub> &#x0003D; 0.71, <italic>p</italic> &#x0003D; 1.4. <bold>(C)</bold> Linear plot of Pi&#x000E9;ron&#x00027;s law in the rate domain (1/RT). Solid lines labeled as &#x0201C;1&#x0201D; and &#x0201C;2&#x0201D; follow the same as in <bold>(B)</bold>. <bold>(D)</bold> Double logarithmic plot of the Weber fraction (&#x00394;<italic>S/S</italic>) as a function of intensity <italic>S</italic>. Vertical dash line separates the Rose-de Vries regime at low <italic>S</italic>-values from Weber&#x00027;s law. <bold>(E)</bold> Linear plot of Pi&#x000E9;ron&#x00027;s law as a function of the stimulus strength <italic>S</italic>. The adapting conditions now vary. The power law &#x003B2;S<sup>p</sup><sub>0</sub> is mapped onto a Weber fraction-type power law (&#x00394;<italic>S/S</italic>)<italic><sup>p</sup></italic> (Medina, <xref ref-type="bibr" rid="B15">2011</xref>) and was varied from Weber&#x00027;s law to the terminal rise in <bold>(D)</bold>. Simulation parameters: <italic>t</italic><sub>0</sub> &#x0003D; 150, &#x003B2; &#x0003D; 1, <italic>p</italic> &#x0003D; 0.33. <bold>(F)</bold> Linear plot of Pi&#x000E9;ron&#x00027;s law in the rate domain. (a.u.) &#x0003D; arbitrary units.</p></caption>
<graphic xlink:href="fphys-06-00190-g0001.tif"/>
</fig>
<p>The second example illustrates the van der Mollen-Keuss effect in RTs. The van der Mollen-Keuss effect imposes a limitation to Pi&#x000E9;ron&#x00027;s law by producing a U-shaped function at very high <italic>S</italic>-values (van der Molen and Orlebeke, <xref ref-type="bibr" rid="B35">1980</xref>; Ja&#x0015B;kowski and W&#x00142;odarczyk, <xref ref-type="bibr" rid="B9">2006</xref>; Marino and Munoz, <xref ref-type="bibr" rid="B13">2009</xref>). &#x003B2;S<sup>p</sup><sub>0</sub> also depends on the sensory adaptation level (Plainis and Murray, <xref ref-type="bibr" rid="B29">2000</xref>; Murray and Plainis, <xref ref-type="bibr" rid="B19">2003</xref>; Medina, <xref ref-type="bibr" rid="B15">2011</xref>). Figure <xref ref-type="fig" rid="F1">1D</xref> simulates the differential threshold relative to the background or Weber fraction (&#x00394;<italic>S/S</italic>) as a function of the intensity <italic>S</italic>. The minimum value corresponds to Weber&#x00027;s law. There is a terminal rise at very high intensities. By interpreting the &#x003B2;S<sup>p</sup><sub>0</sub> as a Weber fraction, the terminal rise in Weber&#x00027;s law which is observed in many modalities gives rise to an abrupt increment in both <italic>k</italic>, and <italic>t</italic><sub><italic>RT</italic><sub>0</sub></sub> in Equation (1) for high intensities. The van der Mollen-Keuss effect can therefore be explained theoretically as a consecuence of an entropy-based approach together with Weber&#x00027;s law (Figure <xref ref-type="fig" rid="F1">1E</xref>). In the rate domain (Equation 4), the reciprocal of RT shows an inverted U-shaped function (Figure <xref ref-type="fig" rid="F1">1F</xref>). This suggests a correlation with specific neural activity (Peirce, <xref ref-type="bibr" rid="B25">2007</xref>). Outside the framework of Pi&#x000E9;ron&#x00027;s law, a more ellaborate approach to the Weber fraction and Weber&#x00027;s law has been developed using the same information-theoretic formalism (Norwich, <xref ref-type="bibr" rid="B21">1993</xref>; Norwich and Wong, <xref ref-type="bibr" rid="B23">1997</xref>).</p>
<p>Donkin and van Maanen fitted three different experimental data sets to test the validity of their assumptions (Donkin and van Maanen, <xref ref-type="bibr" rid="B6">2014</xref>). Good fits to experimental data are neccesary but insufficient to support theoretical models with free parameters. Power laws in complex systems are better supported by models that constraint possible results and predict how experiments agree with such constraints (Roberts and Pashler, <xref ref-type="bibr" rid="B30">2000</xref>; Kello et al., <xref ref-type="bibr" rid="B10">2010</xref>; Stumpf and Porter, <xref ref-type="bibr" rid="B34">2012</xref>). Hence, we have introduced a poweful approach for analyzing the relationship between an internal variable sensory threshold and Pi&#x000E9;ron&#x00027;s law by using information theory and power law scaling.</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>
</body>
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