<?xml version="1.0" encoding="UTF-8" standalone="no"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing DTD v2.3 20070202//EN" "journalpublishing.dtd">
<article xml:lang="EN" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" article-type="research-article">
<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Neurosci.</journal-id>
<journal-title>Frontiers in Neuroscience</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Neurosci.</abbrev-journal-title>
<issn pub-type="epub">1662-453X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fnins.2021.761826</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Neuroscience</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Theoretical Relationship Between Two Measures of Spike Synchrony: Correlation Index and Vector Strength</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Kessler</surname> <given-names>Dominik</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/1439317/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Carr</surname> <given-names>Catherine E.</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/3474/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Kretzberg</surname> <given-names>Jutta</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/17427/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Ashida</surname> <given-names>Go</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</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/15273/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Computational Neuroscience, Department of Neuroscience, Faculty VI, University of Oldenburg</institution>, <addr-line>Oldenburg</addr-line>, <country>Germany</country></aff>
<aff id="aff2"><sup>2</sup><institution>Department of Biology, University of Maryland</institution>, <addr-line>College Park, MD</addr-line>, <country>United States</country></aff>
<aff id="aff3"><sup>3</sup><institution>Cluster of Excellence Hearing4all, Department of Neuroscience, Faculty VI, University of Oldenburg</institution>, <addr-line>Oldenburg</addr-line>, <country>Germany</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Enrique A. Lopez-Poveda, University of Salamanca, Spain</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Peter Heil, Leibniz Institute for Neurobiology, Germany; Satyabrata Parida, University of Pittsburgh, United States</p></fn>
<corresp id="c001">&#x0002A;Correspondence: Go Ashida <email>go.ashida&#x00040;uni-oldenburg.de</email></corresp>
<fn fn-type="other" id="fn001"><p>This article was submitted to Auditory Cognitive Neuroscience, a section of the journal Frontiers in Neuroscience</p></fn></author-notes>
<pub-date pub-type="epub">
<day>20</day>
<month>12</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>15</volume>
<elocation-id>761826</elocation-id>
<history>
<date date-type="received">
<day>20</day>
<month>08</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>09</day>
<month>11</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x000A9; 2021 Kessler, Carr, Kretzberg and Ashida.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Kessler, Carr, Kretzberg and Ashida</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>Information processing in the nervous system critically relies on temporally precise spiking activity. In the auditory system, various degrees of phase-locking can be observed from the auditory nerve to cortical neurons. The classical metric for quantifying phase-locking is the vector strength (VS), which captures the periodicity in neuronal spiking. More recently, another metric, called the correlation index (CI), was proposed to quantify the temporally reproducible response characteristics of a neuron. The CI is defined as the peak value of a normalized shuffled autocorrelogram (SAC). Both VS and CI have been used to investigate how temporal information is processed and propagated along the auditory pathways. While previous analyses of physiological data in cats suggested covariation of these two metrics, general characterization of their connection has never been performed. In the present study, we derive a rigorous relationship between VS and CI. To model phase-locking, we assume Poissonian spike trains with a temporally changing intensity function following a <italic>von Mises</italic> distribution. We demonstrate that VS and CI are mutually related via the so-called concentration parameter that determines the degree of phase-locking. We confirm that these theoretical results are largely consistent with physiological data recorded in the auditory brainstem of various animals. In addition, we generate artificial phase-locked spike sequences, for which recording and analysis parameters can be systematically manipulated. Our analysis results suggest that mismatches between empirical data and the theoretical prediction can often be explained with deviations from the <italic>von Mises</italic> distribution, including skewed or multimodal period histograms. Furthermore, temporal relations of spike trains across trials can contribute to higher CI values than predicted mathematically based on the VS. We find that, for most applications, a SAC bin width of 50 ms seems to be a favorable choice, leading to an estimated error below 2.5% for physiologically plausible conditions. Overall, our results provide general relations between the two measures of phase-locking and will aid future analyses of different physiological datasets that are characterized with these metrics.</p></abstract>
<kwd-group>
<kwd>phase-locking</kwd>
<kwd>circular statistics</kwd>
<kwd>temporal coding</kwd>
<kwd>auditory brainstem</kwd>
<kwd>autocorrelogram</kwd>
<kwd>spike train analysis</kwd>
<kwd>periodic signals</kwd>
<kwd>frequency-following response</kwd>
</kwd-group>
<counts>
<fig-count count="8"/>
<table-count count="0"/>
<equation-count count="9"/>
<ref-count count="72"/>
<page-count count="14"/>
<word-count count="10071"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="s1">
<title>1. Introduction</title>
<p>Temporal coding is found virtually everywhere in the brain, underlying numerous sensory, cognitive, and motor functions of the nervous system (Paton and Buonomano, <xref ref-type="bibr" rid="B50">2018</xref>). Well-timed neuronal spiking is essential for vision (Rucci et al., <xref ref-type="bibr" rid="B56">2018</xref>), audition (Grothe et al., <xref ref-type="bibr" rid="B28">2010</xref>; Heil and Peterson, <xref ref-type="bibr" rid="B31">2015</xref>; Yin et al., <xref ref-type="bibr" rid="B70">2019</xref>), balance (Cullen, <xref ref-type="bibr" rid="B18">2012</xref>), olfaction (Gire et al., <xref ref-type="bibr" rid="B26">2013</xref>), gustation (Hallock and Di Lorenzo, <xref ref-type="bibr" rid="B29">2006</xref>), touch (Saal et al., <xref ref-type="bibr" rid="B58">2016</xref>), electrosensation (Carr and Friedman, <xref ref-type="bibr" rid="B13">1999</xref>; Baker et al., <xref ref-type="bibr" rid="B8">2013</xref>), as well as spinal pattern generation (Catela et al., <xref ref-type="bibr" rid="B16">2015</xref>), motor control (Lehman and Bartussek, <xref ref-type="bibr" rid="B46">2017</xref>; Sober et al., <xref ref-type="bibr" rid="B61">2018</xref>), cerebellar motor learning (De Zeeuw et al., <xref ref-type="bibr" rid="B20">2011</xref>), and memory formation and consolidation (Dragoi, <xref ref-type="bibr" rid="B21">2020</xref>). Loss of temporal precision in neural activity is related to cognitive and behavioral deficits (Balci et al., <xref ref-type="bibr" rid="B9">2009</xref>). When action potentials of a neuron occur preferentially at a certain phase of a periodic stimulus, such a neuronal spiking pattern is called &#x0201C;phase-locked&#x0201D; (see Carr and Friedman, <xref ref-type="bibr" rid="B13">1999</xref>; Ashida et al., <xref ref-type="bibr" rid="B6">2010</xref>, for typical examples). In the auditory system, phase-locking to tonal stimuli plays a fundamental role, for example, in detecting the location of a sound source (Grothe et al., <xref ref-type="bibr" rid="B28">2010</xref>; Ashida, <xref ref-type="bibr" rid="B2">2015</xref>; Yin et al., <xref ref-type="bibr" rid="B70">2019</xref>).</p>
<p>Phase-locking of a spike train (<xref ref-type="fig" rid="F1">Figure 1A</xref>) can be captured in a phase histogram (<xref ref-type="fig" rid="F1">Figure 1C</xref>) that visualizes the spiking rate at each phase of the periodic reference signal (see <xref ref-type="fig" rid="F1">Figure 1B</xref> for the schematic construction of a phase histogram). In order to quantify the degree of phase-locking, a metric called the &#x0201C;vector strength&#x0201D; (VS: Goldberg and Brown, <xref ref-type="bibr" rid="B27">1969</xref>; Fisher, <xref ref-type="bibr" rid="B23">1993</xref>; van Hemmen, <xref ref-type="bibr" rid="B66">2013</xref>) has been widely used (for examples, see Joris et al., <xref ref-type="bibr" rid="B39">2004</xref>; Ashida et al., <xref ref-type="bibr" rid="B6">2010</xref>; Heil and Peterson, <xref ref-type="bibr" rid="B31">2015</xref>, <xref ref-type="bibr" rid="B32">2017</xref>). Here, each spike is converted into a vector on a unit circle with a corresponding phase; all these phase vectors are summed up to a mean spike vector, whose length is the value of VS. Mathematically, VS (sometimes called &#x0201C;synchronization index&#x0201D; or &#x0201C;synchronization coefficient&#x0201D;) is equal to the absolute value of the Fourier component of the spike train at the reference signal frequency (<italic>f</italic>) normalized by the total number of spikes (Johnson, <xref ref-type="bibr" rid="B35">1974</xref>; Ashida et al., <xref ref-type="bibr" rid="B6">2010</xref>). By definition (detailed in Materials and Methods), the value of VS is between zero and one: from no to perfect periodicity at <italic>f</italic>. Certain types of neurons in the cochlear nucleus, for instance, exhibit enhanced phase-locking compared to their peripheral auditory nerve inputs, which is manifested in an increase of VS (Joris et al., <xref ref-type="bibr" rid="B37">1994</xref>; K&#x000F6;ppl, <xref ref-type="bibr" rid="B42">1997</xref>; Wei et al., <xref ref-type="bibr" rid="B69">2017</xref>).</p>
<fig id="F1" position="float">
<label>Figure 1</label>
<caption><p>Characterization of phase-locked spiking response. <bold>(A)</bold> Exemplary phase-locked spike trains recorded in a nucleus magnocellularis (NM) neuron of an American alligator. The raster plot shows the occurrence of spikes for 51 (out of 63) repetitions of a 100 ms pure tone stimulus at the unit&#x00027;s CF (1200 Hz). Sound stimulation starts at 0 ms. <bold>(B)</bold> Schematic drawing for the construction of a phase histogram. For each recorded spike, the corresponding phase at the reference frequency is calculated. Then, a histogram is constructed to show the number of spikes for each phase bin. A steep peak indicates strong phase-locking, whereas a flat phase histogram reflects a lack thereof. <bold>(C)</bold> Phase histogram for the response in <bold>(A)</bold> with its vector strength (VS) value. <bold>(D)</bold> Schematic drawing for the construction of a normalized shuffled autocorrelogram (SAC). Each spike timing within one spike train (here, exemplary trial 1) is compared to the spike timings of all other trains (here, trial 2 and 3) by measuring pairwise temporal distances of the spikes (colored arrows). This procedure is repeated for every recorded spike train. All resulting temporal distances, also called delays, are binned into a histogram and normalized to a dimensionless entity with an average of one. The correlation index (CI) corresponds to the value of the SAC at delay zero. <bold>(E)</bold> SAC for the response in <bold>(A)</bold> with its CI value.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fnins-15-761826-g0001.tif"/>
</fig>
<p>In addition to VS, another metric called the &#x0201C;correlation index&#x0201D; (CI: Joris et al., <xref ref-type="bibr" rid="B38">2006</xref>) was more recently introduced to quantify neuronal synchrony. The value of CI is defined as the height of the central peak of a normalized shuffled autocorrelogram (SAC; <xref ref-type="fig" rid="F1">Figure 1E</xref>), whose construction is depicted in <xref ref-type="fig" rid="F1">Figure 1D</xref> (a more detailed description is given in Materials and Methods). If a set of spike trains has no temporally reproducible spiking pattern across trials, its CI value equals one. A large CI value indicates highly reproducible spiking responses over repeated trials (Joris et al., <xref ref-type="bibr" rid="B38">2006</xref>). In contrast to VS, which is narrowband (i.e., only the spectral component at frequency <italic>f</italic> is considered), CI is generally broadband, as it is a collective measure of multiple frequency components (Parida et al., <xref ref-type="bibr" rid="B49">2021</xref>). SACs and CIs can be applied to both periodic and aperiodic signals and were used for characterizing the temporal coding properties of auditory nerve (AN) fibers (Dreyer and Delgutte, <xref ref-type="bibr" rid="B22">2006</xref>; Heinz and Swaminathan, <xref ref-type="bibr" rid="B33">2009</xref>; Huet et al., <xref ref-type="bibr" rid="B34">2018</xref>; Heeringa et al., <xref ref-type="bibr" rid="B30">2019</xref>), various neurons in the cochlear nuclei recorded <italic>in vivo</italic> (Gai and Carney, <xref ref-type="bibr" rid="B24">2008</xref>; Steinberg and Pe&#x000F1;a, <xref ref-type="bibr" rid="B62">2011</xref>; Recio-Spinoso, <xref ref-type="bibr" rid="B54">2012</xref>; Keine et al., <xref ref-type="bibr" rid="B40">2016</xref>) and <italic>in vitro</italic> (Street and Manis, <xref ref-type="bibr" rid="B63">2007</xref>; Kreeger et al., <xref ref-type="bibr" rid="B44">2012</xref>), and neurons in the auditory midbrain (Shackleton et al., <xref ref-type="bibr" rid="B59">2009</xref>; Zheng and Escab&#x000ED;, <xref ref-type="bibr" rid="B72">2013</xref>).</p>
<p>While both VS and CI represent the degree of synchronized neuronal spiking activity, it is not known how these two measures are related to each other. Previous analyses of physiological data suggested that they should covary according to some monotonic, non-linear relationship (Dreyer and Delgutte, <xref ref-type="bibr" rid="B22">2006</xref>; Joris et al., <xref ref-type="bibr" rid="B38">2006</xref>). Parida and colleagues mathematically related peristimulus time histograms (PSTHs) to VS and CI under very general conditions (Parida et al., <xref ref-type="bibr" rid="B49">2021</xref>). In the present study, we derive a mathematically rigorous relationship between VS and CI under certain assumptions for phase-locking. Our theoretical results will be validated with spike train data that were either recorded from different types of auditory neurons or simulated with available auditory neuron models. These results provide a foundation for comparing past and future experimental data quantified with these measures of phase-locking.</p></sec>
<sec sec-type="materials and methods" id="s2">
<title>2. Materials and Methods</title>
<p>In this section, we summarize our theoretical formulations and describe the methods for validating our mathematical results. A full derivation of the equations is provided in <xref ref-type="supplementary-material" rid="SM1">Supplementary Materials</xref>.</p>
<sec>
<title>2.1. Mathematical Analysis</title>
<sec>
<title>2.1.1. <italic>Von Mises</italic> Distribution</title>
<p>A key assumption for our mathematical formulation and the modeling of phase-locked spike trains is that the neuron fires action potentials according to an underlying <italic>von Mises</italic> distribution (Fisher, <xref ref-type="bibr" rid="B23">1993</xref>). Such an assumption has been adopted in previous modeling studies of auditory neurons for half a century (e.g., Siebert, <xref ref-type="bibr" rid="B60">1970</xref>; Colburn, <xref ref-type="bibr" rid="B17">1973</xref>; Johnson, <xref ref-type="bibr" rid="B35">1974</xref>; Ashida and Carr, <xref ref-type="bibr" rid="B3">2010</xref>). A more recent study confirmed that most phase histograms of cat auditory nerve fibers can be reasonably described by the <italic>von Mises</italic> distribution (Peterson and Heil, <xref ref-type="bibr" rid="B52">2020</xref>). Here, we consider a <italic>von Mises</italic> density function <italic>p</italic><sub>&#x003BA;, <italic>f</italic></sub>, whose period is <italic>T</italic> &#x0003D; 1/<italic>f</italic>, with <italic>f</italic> being the stimulus (or reference) frequency, as</p>
<disp-formula id="E1"><label>(1)</label><mml:math id="M1"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi><mml:mo>,</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:msub><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:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>&#x000B7;</mml:mo><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow></mml:mfrac><mml:mo class="qopname">exp</mml:mo><mml:mstyle mathsize="1.19em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mi>&#x003BA;</mml:mi><mml:mo class="qopname">cos</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:mi>&#x003BC;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mstyle mathsize="1.19em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>where &#x003BC; is the mean direction (or the preferred spiking phase) and &#x003BA;&#x02265;0 is the concentration parameter. Generally, a large &#x003BA; corresponds to a high degree of phase-locking (numerical examples are shown in <xref ref-type="fig" rid="F2">Figures 2A1&#x02013;C3</xref>). <inline-formula><mml:math id="M2"><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi></mml:mrow></mml:mfrac><mml:msubsup><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mo>-</mml:mo><mml:mi>&#x003C0;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003C0;</mml:mi></mml:mrow></mml:msubsup><mml:mo class="qopname">exp</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi><mml:mo class="qopname">cos</mml:mo><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:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mtext>d</mml:mtext><mml:mi>x</mml:mi></mml:math></inline-formula> is the modified Bessel function of order zero, which serves as the normalization constant for <italic>p</italic><sub>&#x003BA;, <italic>f</italic></sub>, such that <inline-formula><mml:math id="M3"><mml:msubsup><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msubsup><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi><mml:mo>,</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:msub><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:mtext>d</mml:mtext><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:math></inline-formula>. Without loss of generality, we set &#x003BC; &#x0003D; 0 for the rest of this paper.</p>
<fig id="F2" position="float">
<label>Figure 2</label>
<caption><p>Relationship between vector strength (VS) and correlation index (CI). <bold>(A1,B1,C1)</bold> Phase-locked spike trains simulated with an inhomogeneous Poisson process whose periodic intensity function is <italic>von Mises</italic> distributed. The raster plots show the spike occurrences for three different phase-locking strengths, namely &#x003BA; &#x0003D; 0.65 <bold>(A1)</bold>, &#x003BA; &#x0003D; 1.56 <bold>(B1)</bold> and &#x003BA; &#x0003D; 5.85 <bold>(C1)</bold>. <bold>(A2,B2,C2)</bold> Corresponding phase histograms for the simulated spike trains in <bold>(A1&#x02013;C1)</bold>. The resulting empirical VS is shown, together with its back-calculated &#x003BA; and estimated CI value. <bold>(A3,B3,C3)</bold> SACs for the spike trains in <bold>(A1&#x02013;C1)</bold> with corresponding empirical CI values. In <bold>(A1&#x02013;C1)</bold>, only 51 trials are shown for clarity, while 400 trials of 150 ms trains were used for <bold>(A2&#x02013;C2)</bold> and <bold>(A3&#x02013;C3)</bold>. <bold>(D)</bold> Value of VS as a function of &#x003BA; for the <italic>von Mises</italic> distribution. <bold>(E)</bold> Value of CI as a function of &#x003BA; for the <italic>von Mises</italic> distribution. <bold>(F)</bold> Relation between VS and CI for varied concentration parameters &#x003BA; of the underlying <italic>von Mises</italic> distribution.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fnins-15-761826-g0002.tif"/>
</fig>
<p>For generating phase-locked spike trains, we used an inhomogeneous Poisson process with a periodic time-varying intensity function</p>
<disp-formula id="E2"><label>(2)</label><mml:math id="M4"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mo>&#x003BB;</mml:mo><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:mi>T</mml:mi><mml:mover accent="true"><mml:mrow><mml:mo>&#x003BB;</mml:mo></mml:mrow><mml:mo>&#x00304;</mml:mo></mml:mover><mml:mo>&#x000B7;</mml:mo><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi><mml:mo>,</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:msub><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:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>where <italic>T</italic> is the length of the stimulus period, and <inline-formula><mml:math id="M5"><mml:mover accent="true"><mml:mrow><mml:mi>&#x003BB;</mml:mi></mml:mrow><mml:mo>&#x00304;</mml:mo></mml:mover></mml:math></inline-formula> the mean spike rate of the neuron (see Ashida et al., <xref ref-type="bibr" rid="B6">2010</xref>). In the following analyses, VS, SAC, and CI do not depend on <inline-formula><mml:math id="M6"><mml:mover accent="true"><mml:mrow><mml:mi>&#x003BB;</mml:mi></mml:mrow><mml:mo>&#x00304;</mml:mo></mml:mover></mml:math></inline-formula>. We note that the presented results are asymptotically true with sufficiently many spikes collected. When only few spikes are considered, the results would be biased (Kutil, <xref ref-type="bibr" rid="B45">2012</xref>). Furthermore, phase histograms of real neurons do not necessarily follow the <italic>von Mises</italic> distribution because of refractory periods and harmonic distortions (e.g., Avissar et al., <xref ref-type="bibr" rid="B7">2013</xref>; Peterson and Heil, <xref ref-type="bibr" rid="B51">2019</xref>). We will revisit this point in the Discussion.</p></sec>
<sec>
<title>2.1.2. Vector Strength</title>
<p>As reviewed in Ashida et al. (<xref ref-type="bibr" rid="B6">2010</xref>), the vector strength of a neuronal spike train in response to a periodic signal with frequency <italic>f</italic> is calculated as the length of the mean phase vector (X, Y) of all collected spikes (Goldberg and Brown, <xref ref-type="bibr" rid="B27">1969</xref>), namely <inline-formula><mml:math id="M7"><mml:mstyle class="text"><mml:mtext class="textrm" mathvariant="normal">VS</mml:mtext></mml:mstyle><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msup><mml:mrow><mml:mstyle class="text"><mml:mtext class="textrm" mathvariant="normal">X</mml:mtext></mml:mstyle></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>&#x0002B;</mml:mo><mml:msup><mml:mrow><mml:mstyle class="text"><mml:mtext class="textrm" mathvariant="normal">Y</mml:mtext></mml:mstyle></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:msqrt></mml:math></inline-formula> with <inline-formula><mml:math id="M8"><mml:mstyle class="text"><mml:mtext class="textrm" mathvariant="normal">X</mml:mtext></mml:mstyle><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:mfrac><mml:msubsup><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:msubsup><mml:mo class="qopname">sin</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:msub><mml:mrow><mml:mi>t</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:math></inline-formula> and <inline-formula><mml:math id="M9"><mml:mstyle class="text"><mml:mtext class="textrm" mathvariant="normal">Y</mml:mtext></mml:mstyle><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:mfrac><mml:msubsup><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:msubsup><mml:mo class="qopname">cos</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:msub><mml:mrow><mml:mi>t</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:math></inline-formula>, where <italic>t</italic><sub><italic>j</italic></sub> denotes the timing of the <italic>j</italic>-th spike and <italic>N</italic> is the total number of spikes. For our theoretical analyses, we used the continuous extension of the definition of vector strength (see Ashida et al., <xref ref-type="bibr" rid="B6">2010</xref>, <xref ref-type="bibr" rid="B4">2013</xref>), according to which VS was computed as a function of &#x003BA; by</p>
<disp-formula id="E3"><label>(3)</label><mml:math id="M10"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mtext class="textrm" mathvariant="normal">VS</mml:mtext><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>&#x000B7;</mml:mo><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow></mml:mfrac><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:mo class="qopname">exp</mml:mo><mml:mstyle mathsize="1.19em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mi>&#x003BA;</mml:mi><mml:mo class="qopname">cos</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mstyle mathsize="1.19em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mo class="qopname">cos</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mtext>d</mml:mtext><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</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 <inline-formula><mml:math id="M11"><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi></mml:mrow></mml:mfrac><mml:msubsup><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mo>-</mml:mo><mml:mi>&#x003C0;</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003C0;</mml:mi></mml:mrow></mml:msubsup><mml:mo class="qopname">exp</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi><mml:mo class="qopname">cos</mml:mo><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:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo class="qopname">cos</mml:mo><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:mtext>d</mml:mtext><mml:mi>x</mml:mi></mml:math></inline-formula> is the modified Bessel function of order one. VS monotonically increases with &#x003BA; (<xref ref-type="fig" rid="F2">Figure 2D</xref>).</p></sec>
<sec>
<title>2.1.3. Normalized Shuffled Autocorrelogram and Correlation Index</title>
<p>SACs are obtained by measuring all pairwise spike intervals across all non-identical spike trains (see <xref ref-type="fig" rid="F1">Figure 1D</xref>). The peak value of the normalized SAC at delay zero is the CI, which captures the degree of reproducibility in spike trains for repeated stimuli. Assuming that spike trains to repeated stimulus presentations are independent and identically <italic>von Mises</italic> distributed, we can derive a formula for SAC, which is only dependent on the concentration parameter &#x003BA; and the time delay <italic>s</italic> (see <xref ref-type="supplementary-material" rid="SM1">Supplementary Material</xref> for detailed derivations). Namely,</p>
<disp-formula id="E4"><label>(4)</label><mml:math id="M12"><mml:mtable class="eqnarray" columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mtext class="textrm" mathvariant="normal">SAC</mml:mtext></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow></mml:msub><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:mo>=</mml:mo><mml:mi>T</mml:mi><mml:mo>&#x000B7;</mml:mo><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi><mml:mo>,</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:msub><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>&#x000B7;</mml:mo><mml:msub><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi><mml:mo>,</mml:mo><mml:mi>f</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:mi>s</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mtext>d</mml:mtext><mml:mi>t</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi><mml:mo>&#x000B7;</mml:mo><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:msup><mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:mo class="qopname">exp</mml:mo><mml:mstyle mathsize="1.61em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mi>&#x003BA;</mml:mi><mml:mstyle mathsize="1.19em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mo class="qopname">cos</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>&#x0002B;</mml:mo><mml:mo class="qopname">cos</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:mi>s</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mstyle mathsize="1.19em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mstyle mathsize="1.61em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mtext>d</mml:mtext><mml:mi>t</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:msup><mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac><mml:mo>&#x000B7;</mml:mo><mml:mfrac><mml:mrow><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:mfrac><mml:mstyle displaystyle="true"><mml:msubsup><mml:mrow><mml:mo>&#x0222B;</mml:mo></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:msubsup></mml:mstyle><mml:mo class="qopname">exp</mml:mo><mml:mstyle mathsize="1.61em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mn>2</mml:mn><mml:mi>&#x003BA;</mml:mi><mml:mo class="qopname">cos</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:mi>s</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>&#x000B7;</mml:mo><mml:mo class="qopname">cos</mml:mo><mml:mstyle mathsize="1.61em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mn>2</mml:mn><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:mstyle mathsize="1.61em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mi>t</mml:mi><mml:mo>-</mml:mo><mml:mfrac><mml:mrow><mml:mi>s</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:mfrac><mml:mstyle mathsize="1.61em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mstyle mathsize="1.61em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mstyle mathsize="1.61em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mtext>d</mml:mtext><mml:mi>t</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003BA;</mml:mi><mml:mo class="qopname">cos</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003C0;</mml:mi><mml:mi>f</mml:mi><mml:mi>s</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:msup><mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>For its center peak at delay <italic>s</italic> &#x0003D; 0, we find</p>
<disp-formula id="E6"><label>(5)</label><mml:math id="M14"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:mtext class="textrm" mathvariant="normal">CI</mml:mtext><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mtext class="textrm" mathvariant="normal">SAC</mml:mtext></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>0</mml:mn></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:msup><mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac><mml:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>CI increases monotonically as a function of &#x003BA; (<xref ref-type="fig" rid="F2">Figure 2E</xref>). Knowing the relationship between the concentration parameter &#x003BA; with VS and CI, we can now relate VS and CI via &#x003BA; (<xref ref-type="fig" rid="F2">Figure 2F</xref>). We note that there is no closed formula that directly relates VS and CI without using &#x003BA;. Therefore, to estimate the value of CI from the value of VS, for example, Equation (3) is solved for &#x003BA;, and the obtained value of &#x003BA; is then substituted into Equation (5).</p></sec>
<sec>
<title>2.1.4. Effects of Data Length <bold><italic>D</italic></bold> and SAC Bin Width <bold><italic>&#x003C9;</italic></bold></title>
<p>To evaluate the scattering of the data around the theoretical VS-CI curve, we examined the effect of the data length <italic>D</italic> and the bin width &#x003C9; on the SAC and CI value. Here we refer to the &#x0201C;data length&#x0201D; as the time length of each single spike train used for the calculation of SAC. Assuming that it is equally likely for a unit to fire during each stimulus phase, the data length <italic>D</italic> introduces a linear decay to the side peaks of the SAC with delay <italic>s</italic>, which can be combined with the SAC in Equation (4) by the multiplicative factor</p>
<disp-formula id="E7"><label>(6)</label><mml:math id="M77"><mml:mrow><mml:msub><mml:mi>&#x003B6;</mml:mi><mml:mi>D</mml:mi></mml:msub><mml:mo stretchy='false'>(</mml:mo><mml:mi>s</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mo>=</mml:mo><mml:mrow><mml:mo>{</mml:mo><mml:mtable columnalign='left'><mml:mtr><mml:mtd><mml:mn>1</mml:mn><mml:mo>&#x02212;</mml:mo><mml:mo>&#x0007C;</mml:mo><mml:mfrac><mml:mi>s</mml:mi><mml:mi>D</mml:mi></mml:mfrac><mml:mo>&#x0007C;</mml:mo><mml:mo>,</mml:mo><mml:mtext>&#x000A0;&#x000A0;</mml:mtext><mml:mo>&#x0007C;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x0007C;</mml:mo><mml:mo>&#x0003C;</mml:mo><mml:mi>D</mml:mi></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mtext>&#x000A0;&#x000A0;&#x000A0;&#x000A0;&#x000A0;&#x000A0;&#x000A0;&#x000A0;&#x000A0;</mml:mtext><mml:mn>0</mml:mn><mml:mtext>&#x000A0;&#x000A0;&#x000A0;&#x000A0;</mml:mtext><mml:mo>,</mml:mo><mml:mtext>&#x000A0;&#x000A0;</mml:mtext><mml:mo>&#x0007C;</mml:mo><mml:mi>s</mml:mi><mml:mo>&#x0007C;</mml:mo><mml:mo>&#x02265;</mml:mo><mml:mi>D</mml:mi></mml:mtd></mml:mtr></mml:mtable></mml:mrow><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
<p>such that</p>
<disp-formula id="E8"><mml:math id="M16"><mml:mtable columnalign="left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mtext class="textrm" mathvariant="normal">SAC</mml:mtext></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi><mml:mo>,</mml:mo><mml:mi>D</mml:mi></mml:mrow></mml:msub><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:mo>=</mml:mo><mml:msub><mml:mrow><mml:mtext class="textrm" mathvariant="normal">SAC</mml:mtext></mml:mrow><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow></mml:msub><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:mo>&#x000B7;</mml:mo><mml:msub><mml:mrow><mml:mi>&#x003B6;</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi></mml:mrow></mml:msub><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:mo>.</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>This equation indicates that CI is not affected by the data length <italic>D</italic>, as it is the value of SAC at <italic>s</italic> &#x0003D; 0.</p>
<p>The derivation of the CI in Equation (5) implicitly assumed a sufficiently small &#x003C9;. Therefore, by design, the value of the <italic>von Mises</italic> density <italic>p</italic><sub>&#x003BA;, <italic>f</italic></sub> does not change within each bin. This is different when introducing binning of a finite size, which leads to a bias in the calculation of CI. The effect of binning can be formulated as the convolution of <italic>p</italic><sub>&#x003BA;, <italic>f</italic></sub> with a rectangular window function. This effectively induces the averaging of function values in each bin. Thus, CI becomes a function of &#x003C9;, &#x003BA; and <italic>f</italic> (see <xref ref-type="supplementary-material" rid="SM1">Supplementary Material</xref> for detailed derivation):</p>
<disp-formula id="E9"><label>(7)</label><mml:math id="M17"><mml:mtable class="eqnarray" columnalign="right center left"><mml:mtr><mml:mtd><mml:msub><mml:mrow><mml:mtext class="textrm" mathvariant="normal">CI</mml:mtext></mml:mrow><mml:mrow><mml:mi>&#x003C9;</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mo>&#x0002B;</mml:mo><mml:mn>2</mml:mn><mml:mstyle displaystyle="true"><mml:munderover accentunder="false" accent="false"><mml:mrow><mml:mo>&#x02211;</mml:mo></mml:mrow><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mrow><mml:mi>&#x0221E;</mml:mi></mml:mrow></mml:munderover></mml:mstyle><mml:mstyle displaystyle="true"><mml:munder class="msub"><mml:mrow><mml:mstyle displaystyle="true"><mml:munder accentunder="false"><mml:mrow><mml:mstyle mathsize="2.03em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mfrac><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mi>n</mml:mi></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow></mml:mfrac><mml:msup><mml:mrow><mml:mstyle mathsize="2.03em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>&#x0FE38;</mml:mo></mml:munder></mml:mstyle></mml:mrow><mml:mrow><mml:mtable style="text-align:axis;" equalrows="false" columnlines="none none none none none none none none none" equalcolumns="false" class="array"><mml:mtr><mml:mtd><mml:mtext class="textrm" mathvariant="normal">strength of</mml:mtext></mml:mtd></mml:mtr><mml:mtr><mml:mtd><mml:mtext class="textrm" mathvariant="normal">n-th harmonic</mml:mtext></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:munder></mml:mstyle><mml:mstyle displaystyle="true"><mml:munder class="msub"><mml:mrow><mml:mstyle displaystyle="true"><mml:munder accentunder="false"><mml:mrow><mml:mstyle mathsize="2.03em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle><mml:mfrac><mml:mrow><mml:mo class="qopname">sin</mml:mo><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003C0;</mml:mi><mml:mi>n</mml:mi><mml:mi>f</mml:mi><mml:mi>&#x003C9;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mi>&#x003C0;</mml:mi><mml:mi>n</mml:mi><mml:mi>f</mml:mi><mml:mi>&#x003C9;</mml:mi></mml:mrow></mml:mfrac><mml:mstyle mathsize="2.03em"><mml:mrow><mml:mtext>&#x0200a;</mml:mtext></mml:mrow></mml:mstyle></mml:mrow><mml:mo>&#x0FE38;</mml:mo></mml:munder></mml:mstyle></mml:mrow><mml:mrow><mml:mtable style="text-align:axis;" equalrows="false" columnlines="none none none none none none none none none" equalcolumns="false" class="array"><mml:mtr><mml:mtd><mml:mtext class="textrm" mathvariant="normal">decay factor</mml:mtext></mml:mtd></mml:mtr></mml:mtable></mml:mrow></mml:munder></mml:mstyle><mml:mo>,</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
<p>For large bin widths &#x003C9;, the CI value decays toward 1, as the second term of Equation (7) monotonically decreases with &#x003C9;. For sufficiently small &#x003C9;, the decay factor is (close to) 1, since sin(&#x003C0;<italic>nf&#x003C9;</italic>)&#x02248;&#x003C0;<italic>nf&#x003C9;</italic>, thus leading to very small bias.</p></sec></sec>
<sec>
<title>2.2. Data Analysis</title>
<p>To validate our theoretical findings, we analyzed spike trains from three different sources: (1) simulated spike trains with an inhomogeneous Poisson process, (2) simulated auditory nerve (AN) and globular bushy cell (GBC) data, and (3) spike timing data recorded from auditory neurons <italic>in vivo</italic>. To calculate the SACs and CI values, custom-written Matlab scripts were used that followed the procedure described in Joris et al. (<xref ref-type="bibr" rid="B38">2006</xref>). Unless otherwise stated, we used &#x003C9; &#x0003D; 50 &#x003BC;s for the SAC bin width.</p>
<sec>
<title>2.2.1. Spike Train Generation</title>
<p>Phase-locked spike trains were generated using an inhomogeneous Poisson process with the time-dependent intensity function in Equation (2). This simple model does not include refractory periods (see Discussion for the possible effects of refractory periods on VS and CI). A total of 46 units were generated with target VS values evenly spaced between 0.05 and 0.95 (with a step of 0.02), for which the value of &#x003BA; was back-calculated using Equation (3). The frequency <italic>f</italic> was fixed to 500 Hz. For each &#x003BA;, 150 ms long spike trains were generated 400 times. The average firing rate was set to 200 spikes/s and the time resolution for spike generation was 2 &#x003BC;s (i.e., &#x003C9;/dt &#x0003D; 25). <xref ref-type="fig" rid="F2">Figures 2A1&#x02013;C1</xref> shows exemplary rasters of simulated spike trains with target VS values of 0.31, 0.61 and 0.91. Their corresponding phase histograms (<xref ref-type="fig" rid="F2">Figures 2A2&#x02013;C2</xref>) and SACs (<xref ref-type="fig" rid="F2">Figures 2A3&#x02013;C3</xref>) are shown below the rasters.</p></sec>
<sec>
<title>2.2.2. AN/GBC Model Data</title>
<p>To simulate AN fiber responses, an auditory periphery model (Bruce et al., <xref ref-type="bibr" rid="B10">2018</xref>) was used, which was shown to replicate physiological spiking patterns of AN in cats. To simulate tone-driven spiking patterns of GBCs, an adaptive coincidence counting model was used, which was fed with the simulated AN output (Ashida et al., <xref ref-type="bibr" rid="B5">2019</xref>). AN fiber spike trains were generated for tonal waveforms with frequencies ranging from 200 to 3,000 Hz in steps of 100 Hz at sound pressure levels of 40 and 70 dB SPL. The spontaneous spike rate of the AN model was set to 70 spikes/s, so that we could reuse the simulated spike trains of this high spontaneous rate AN fiber model as inputs to the GBC model. The characteristic frequency of the model was always the same as the stimulus frequency. The simulated time length of each trial was 190 ms and the sound stimulation started at 25 ms with a 5 ms cosine ramp. Sampling frequency was 100 kHz (dt &#x0003D; 10&#x003BC;s). For each combination of sound frequency and level, 8000 repetitions were generated. The first 400 trials were used for further AN data analyses. The entire 8000 repetitions served as inputs to simulated GBCs. Assuming that each GBC received inputs from 20 AN units (Ashida et al., <xref ref-type="bibr" rid="B5">2019</xref>), we had 400 trials for each GBC simulation. For both AN and GBC, the resulting spike trains were analyzed over a 150 ms window, excluding the first 15 ms onset response to avoid possible effects of spike rate adaptation on VS and CI.</p></sec>
<sec>
<title>2.2.3. <italic>In vivo</italic> Recordings From Auditory Brainstem Neurons</title>
<p>Similarly to Ashida and Carr (<xref ref-type="bibr" rid="B3">2010</xref>), we re-analyzed our previous <italic>in vivo</italic> recording data from nucleus magnocellularis (NM) and nucleus laminaris (NL) neurons in birds and reptiles. Corresponding experimental procedures were described in Carr et al. (<xref ref-type="bibr" rid="B15">2009</xref>) for alligators, in K&#x000F6;ppl and Carr (<xref ref-type="bibr" rid="B43">2008</xref>) for chickens, and in Carr and K&#x000F6;ppl (<xref ref-type="bibr" rid="B14">2004</xref>) for barn owls. To induce phase-locked spiking responses, NM and NL neurons in these animals were driven with repeated tonal stimulation at their best (or characteristic) frequencies. In total, we re-analyzed 142 units (57 from alligators, 34 from chickens, and 51 from owls). Stimulus duration was 50 or 100 ms, except for two units with 200 and 400 ms stimulation. Stimulus presentation was repeated 50&#x02013;400 times. To eliminate the effect of the stimulus onset, we excluded the initial 15 ms of the spiking response for each stimulus presentation. Units with a total number of collected spikes fewer than 400 or with an average driven firing rate lower than 30 spikes/s were excluded from further analyses, leaving us with 125 units. From the spike timing data of each of these units, we calculated VS and CI according to the methods described above. In addition to our own data, we adopted the empirical VS-CI plot of Joris et al. (<xref ref-type="bibr" rid="B38">2006</xref>) for comparison, in which <italic>in vivo</italic> recording data from trapezoid body (TB) fibers in cats were presented.</p></sec>
<sec>
<title>2.2.4. Data Length <bold><italic>D</italic></bold> and SAC Bin Width <bold>&#x003C9;</bold> Analysis</title>
<p>To test the effect of the data length <italic>D</italic> on the SAC and CI, we simulated 2,000 Poissonian spike trains of one unit responding to a 100 ms long 500 Hz pure tone stimulus with a temporal resolution of 2 &#x003BC;s. The target VS value was 0.8 and the mean firing rate <inline-formula><mml:math id="M18"><mml:mover accent="true"><mml:mrow><mml:mi>&#x003BB;</mml:mi></mml:mrow><mml:mo>&#x00304;</mml:mo></mml:mover></mml:math></inline-formula> was set at 200 spikes/s. We calculated the SAC for spikes in the time interval between 30 and 80 ms after the stimulus onset with the bin width &#x003C9; &#x0003D; 50 &#x003BC;s, such that &#x003C9;/dt &#x0003D; 25. The simulation results were then compared with our theoretical findings in Equation (6).</p>
<p>To evaluate the effect of the SAC bin width &#x003C9;, we created 400,000 trials of inhomogeneous Poissonian spike trains, each of which was 100 ms long, locked at 500 Hz with an average rate of 200 spikes/s and a target VS of 0.6. To calculate the mean and standard deviation of SAC and CI, we divided them into 1000 repetitions, each containing 400 trials. The temporal resolution of the spike trains was dt &#x0003D; 2&#x003BC;s. In total, 88 different bin width values ranging from &#x003C9;= 2 to 2,000 &#x003BC;s were used. As shown in Results (section 3.4), deviation from the theoretical value critically depends on the value of &#x003C9;/dt. Therefore, we divided the values of &#x003C9; into the four groups &#x0201C;odd&#x0201D; (N &#x0003D; 23), &#x0201C;even&#x0201D; (N &#x0003D; 23), &#x0201C;non-integer&#x0201D; (N &#x0003D; 32), and &#x0201C;large&#x0201D; (N &#x0003D; 10), according to the value of the ratio &#x003C9;/dt. The group &#x0201C;large&#x0201D; contains all bin widths with &#x003C9;/dt&#x02265;550. For each repetition and each bin width &#x003C9;, SAC and CI were computed and compared with the theoretical CI decay in Equation (7).</p></sec></sec></sec>
<sec sec-type="results" id="s3">
<title>3. Results</title>
<p>The main goal of the present study is to establish a clear relationship between VS and CI. After a brief mathematical description of their relationship, we test the validity of our theoretical formulation with published auditory neuron models and physiologically recorded <italic>in vivo</italic> data. Finally, we investigate potential causes for deviations between theoretical and empirical results.</p>
<sec>
<title>3.1. Mathematical Formulation of the Relation Between VS and CI</title>
<p>In order to relate VS and CI by mathematical expressions, we assumed that phase-locked spike times can be described by the arrival times of an inhomogeneous Poisson process with a periodic, time-dependent intensity function &#x003BB;(<italic>t</italic>) that was based on the <italic>von Mises</italic> distribution (Equation 2). This function captures the periodic spike rate change at frequency <italic>f</italic>, the degree of phase-locking quantified with the concentration parameter &#x003BA;, and the mean discharge rate <inline-formula><mml:math id="M19"><mml:mover accent="true"><mml:mrow><mml:mi>&#x003BB;</mml:mi></mml:mrow><mml:mo>&#x00304;</mml:mo></mml:mover></mml:math></inline-formula> of the neuronal response. A large value of &#x003BA; generally corresponds to prominent phase-locking, which is indicated in the vertical alignment of spikes in raster plots (compare <xref ref-type="fig" rid="F2">Figures 2A1&#x02013;C1</xref>). Temporal fidelity and reproducibility of spike timings can be visualized with phase histograms (<xref ref-type="fig" rid="F2">Figures 2A2&#x02013;C2</xref>) or SACs (<xref ref-type="fig" rid="F2">Figures 2A3&#x02013;C3</xref>).</p>
<p>As summarized in Materials and Methods and detailed in <xref ref-type="supplementary-material" rid="SM1">Supplementary Material</xref>, we obtained the formulae VS(&#x003BA;) &#x0003D; <italic>I</italic><sub>1</sub>(&#x003BA;)/<italic>I</italic><sub>0</sub>(&#x003BA;) (Equation 3) and <inline-formula><mml:math id="M20"><mml:mstyle class="text"><mml:mtext class="textrm" mathvariant="normal">CI</mml:mtext></mml:mstyle><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow><mml:mo>/</mml:mo><mml:msub><mml:mrow><mml:mi>I</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:msup><mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>&#x003BA;</mml:mi></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> (Equation 5). Here, both metrics depend only on the concentration parameter &#x003BA; of the <italic>von Mises</italic> distribution (<xref ref-type="fig" rid="F2">Figures 2D,E</xref>). Since both VS and CI are monotonic functions of &#x003BA;, we can connect VS and CI using their one-to-one relationship with &#x003BA; (<xref ref-type="fig" rid="F2">Figure 2F</xref>). CI is a monotonically increasing function of VS (and vice versa), and VS &#x0003D; 0 corresponds to CI &#x0003D; 1. Next, we compare these results to simulated and <italic>in vivo</italic> data.</p></sec>
<sec>
<title>3.2. Validation of Theoretical Results</title>
<sec>
<title>3.2.1. Simulated Data</title>
<p>In order to validate the theoretical relationship between VS and CI, we simulated spike trains for varied degrees of phase-locking (three examples are shown in <xref ref-type="fig" rid="F2">Figures 2A1&#x02013;C3</xref>) using an inhomogeneous Poisson process as described in the Materials and Methods section. From these sequences, we computed VS and CI values, and compared them with the theoretical prediction shown in <xref ref-type="fig" rid="F2">Figure 2F</xref>. When the underlying spiking distribution is <italic>von Mises</italic>, the theoretical findings match the empirical calculations of simulated data (<xref ref-type="fig" rid="F3">Figure 3A</xref>). Hence, the validity of our analytical results is confirmed with sufficiently long trials containing sufficiently many spikes.</p>
<fig id="F3" position="float">
<label>Figure 3</label>
<caption><p>Validation of the theoretical relation between VS and CI. In each panel, the theoretical VS-CI relationship is shown with a black solid curve, while simulated or recorded data are shown by different types of symbols. The gray dotted lines indicate 0.7 &#x000D7; (theoretical CI) and 1.4 &#x000D7; (theoretical CI) for each value of VS. <bold>(A)</bold> VS and CI values for numerically calculated <italic>von Mises</italic> distributions. Results from 46 simulated units that are locked at 500 Hz with target VS values ranging from 0.05 to 0.95 (in steps of 0.02) are shown. <bold>(B)</bold> Simulated auditory nerve (AN) and globular bushy cell (GBC) responses with 58 units each. The stimulus frequency was fixed to the unit&#x00027;s CF that ranged from 200 to 2,000 Hz, each tested at 40 and 70 dB SPL. <bold>(C)</bold> VS-CI relationship from 125 auditory brainstem neurons of three animal species. <bold>(D)</bold> VS-CI relationship in 564 tonal responses of cat TB fibers. Data points were adapted from Joris et al. (<xref ref-type="bibr" rid="B38">2006</xref>) with permission. Arrows in <bold>(B,C)</bold> indicate the examples used in <xref ref-type="fig" rid="F4">Figure 4</xref>.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fnins-15-761826-g0003.tif"/>
</fig></sec>
<sec>
<title>3.2.2. AN/GBC Model Data</title>
<p>We generated spike data using AN and GBC models driven by tonal stimulation of frequencies from 200 to 2,000 Hz at 40 and 70 dB SPL and determined VS and CI of these simulated traces. Overall, their trend closely follows the mathematical prediction (<xref ref-type="fig" rid="F3">Figure 3B</xref>). There are a few instances, however, that notably deviated from the theoretical curve. These instances indicate either higher CI or lower VS than what is estimated from the theoretical relationship (e.g., arrows in <xref ref-type="fig" rid="F3">Figure 3B</xref>). We will examine this discrepancy in section 3.3.</p></sec>
<sec>
<title>3.2.3. <italic>In vivo</italic> Data</title>
<p>Finally, we analyzed auditory brainstem neuron data from three different species and two different neuron types. The animals were presented with pure tone stimuli at the unit&#x00027;s presumed CF. The empirical data points generally followed the trend of the theoretical curve (<xref ref-type="fig" rid="F3">Figure 3C</xref>). However, considerable scattering of the VS-CI points around the theoretical prediction is evident. Most of the deviating data points appear to the right of the theoretical line, indicating a degraded VS, an increased CI, or both. The same holds true for cat TB data originally collected by Joris et al. (<xref ref-type="bibr" rid="B38">2006</xref>) (<xref ref-type="fig" rid="F3">Figure 3D</xref>). While most data points fall into a reasonable range around the mathematical reference, there are some units with potentially reduced VS or increased CI. In summary, both simulated and empirical data were consistent with our theoretical relations between VS and CI. Possible reasons for the deviation include violations of the mathematical assumptions and systematic calculation errors of the empirical VS and CI values, which we further investigate in the following two subsections.</p></sec></sec>
<sec>
<title>3.3. Violation of the Mathematical Assumptions</title>
<p>Deviation from the theoretical relationship between VS and CI can happen, when the underlying spiking pattern does not obey the <italic>von Mises</italic> distribution function. Example rasters are shown in <xref ref-type="fig" rid="F4">Figures 4A1&#x02013;E1</xref>. The phase histograms of such units include skewed (<xref ref-type="fig" rid="F4">Figures 4A2,B2</xref>) or bimodal (<xref ref-type="fig" rid="F4">Figures 4C2,D2</xref>) phase distributions. Similar phase histograms were also observed in, e.g., cat AN fiber recordings, primarily due to harmonic distortions originating from the auditory periphery (see Peterson and Heil, <xref ref-type="bibr" rid="B51">2019</xref>, and references therein). In one of the alligator NL neurons (<xref ref-type="fig" rid="F4">Figure 4D1</xref>), both the spike rate and the spike timing depend on interaural time differences, leading to a bimodal phase histogram (<xref ref-type="fig" rid="F4">Figure 4D2</xref>).</p>
<fig id="F4" position="float">
<label>Figure 4</label>
<caption><p>Violation of the theoretical assumptions for the VS-CI relationship. Each column shows the response of a unit whose CI value deviates from the theoretical value estimated from its VS. Corresponding data points are indicated by arrows in <xref ref-type="fig" rid="F3">Figures 3B,C</xref>. <bold>(A1&#x02013;E1)</bold> Raster plots. The sound stimulus starts at time zero. <bold>(A2&#x02013;E2)</bold> Phase histograms with VS values, from which the value of &#x003BA; was back-calculated and then the value of CI was estimated. <bold>(A3&#x02013;E3)</bold> SACs with CI values. Note the difference between the estimated CI in <bold>(A2&#x02013;E2)</bold> and actual CI in <bold>(A3&#x02013;E3)</bold>. To the alligator NL units, pure tone stimuli were presented binaurally with an interaural time difference ranging from &#x02013;2,000 to &#x0002B;2,000 &#x003BC;s in a step of 250 &#x003BC;s, repeated three times <bold>(D1&#x02013;D3)</bold>; or from &#x02013;1,000 to &#x0002B;1,000 &#x003BC;s in a step of 100 &#x003BC;s, repeated 5 times <bold>(E1&#x02013;E3)</bold>; only 51 repetitions are shown in <bold>(E1)</bold>, but all repetitions are used for <bold>(E2,E3)</bold>.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fnins-15-761826-g0004.tif"/>
</fig>
<p>Such violations of the theoretical assumption of a symmetrical, unimodal <italic>von Mises</italic> distribution result in SACs that are also skewed (<xref ref-type="fig" rid="F4">Figures 4A3,B3</xref>) or with multiple side peaks (<xref ref-type="fig" rid="F4">Figures 4C3,D3</xref>). Consistent with the observations by Joris et al. (<xref ref-type="bibr" rid="B38">2006</xref>), we find that units with these types of phase histograms show a reduced VS. The CI, on the other hand, seems more robust to such changes, as the SAC can capture temporal structures that are not frequency specific (Parida et al., <xref ref-type="bibr" rid="B49">2021</xref>). In other words, CI can be large when there is trial-to-trial reproducibility in the spiking responses even without periodic patterns. In the cases presented here, low frequency units (typically below 500 Hz) predominantly showed such phase histograms, which often present more than one peak in one stimulus cycle (i.e., peak splitting).</p>
<p>In addition to these relatively apparent examples, the value of CI can be higher than the theoretical prediction, when there is some hidden temporal structure between trials. Such an example is shown in <xref ref-type="fig" rid="F4">Figure 4E1</xref>. In this case, the neuron was stimulated binaurally with a time difference between the two ears that was systematically varied across trials. The spike rate of this neuron varies according to the interaural time difference (ITD: <xref ref-type="fig" rid="F5">Figure 5A</xref>), which is a representative response of an NL neuron (Carr et al., <xref ref-type="bibr" rid="B15">2009</xref>). In contrast to the previous example (<xref ref-type="fig" rid="F4">Figures 4D1,D2</xref>), the stimulus-dependent variation of spiking pattern in this neuron is hardly noticeable in the phase histogram (<xref ref-type="fig" rid="F4">Figure 4E2</xref>). The CI value of this neuron, however, was substantially higher than the naive expectation from the VS (<xref ref-type="fig" rid="F4">Figure 4E3</xref>). In order to investigate how such a large CI value was achieved, we generated artificial spike trains with the same phase histogram as this neuron (<xref ref-type="fig" rid="F5">Figure 5B</xref>). In contrast to the ITD dependence of the actual NL neuron (<xref ref-type="fig" rid="F4">Figures 4E1</xref>, <xref ref-type="fig" rid="F5">5A</xref>), the simulated spike trains contained no additional structures in their repeated trials. For delays between &#x02013;10 and &#x0002B;10 ms, the empirical SAC (<xref ref-type="fig" rid="F5">Figure 5C</xref>, blue) presents higher peaks than the simulated SAC (<xref ref-type="fig" rid="F5">Figure 5C</xref>, red), indicating that spikes of this alligator NL unit were more likely to occur at the same or neighboring cycles than an inhomogeneous Poisson process having the same phase histogram. For larger delays, however, empirical spike coincidences drop below the simulated data. In sum, the deviation of the empirical CI from the theoretically expected value suggested an additional temporal structure in the spike trains of this NL unit and the comparison of empirical and simulated SACs revealed increased spike coincidences across trials.</p>
<fig id="F5" position="float">
<label>Figure 5</label>
<caption><p>Comparison of empirical and simulated data. <bold>(A)</bold> ITD-tuning curve of the 700 Hz alligator NL unit used for <xref ref-type="fig" rid="F4">Figures 4E1&#x02013;E3</xref>. Error bars represent standard deviations (5 repetitions for each ITD). <bold>(B)</bold> Phase histograms and <bold>(C)</bold> SACs of the same NL unit (blue) and simulated spike train (red) that was generated with an inhomogeneous Poisson process whose intensity function is modeled with the empirical phase histogram without any additionally assumed trial-to-trial relations.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fnins-15-761826-g0005.tif"/>
</fig></sec>
<sec>
<title>3.4. Data Length and Bin Width Analysis for the SAC and CI</title>
<p>The choice of parameters for CI calculation can lead to an additional deviation from the theoretical prediction. We investigated the effects of the data length <italic>D</italic> and the SAC bin width &#x003C9; on CI by deriving Equations 6 and 7. The limited data length <italic>D</italic> of spike trains linearly scales down the heights of the side peaks in the SAC (<xref ref-type="fig" rid="F6">Figure 6A</xref>) with a multiplicative factor 1&#x02212;|<italic>s</italic>/<italic>D</italic>|. This decay of SAC reflects the fact that spike coincidences are not counted for spikes that could occur before the beginning or after the end of the time interval used for the calculation of SAC. Therefore, the decay of SAC is stronger for smaller <italic>D</italic> (<xref ref-type="fig" rid="F6">Figure 6B</xref>). The value of CI, or the SAC peak at <italic>s</italic> &#x0003D; 0, is nevertheless unaffected by the data length <italic>D</italic>. We also note that the value of VS is generally unaffected by <italic>D</italic>, as long as a sufficient number of spikes is collected.</p>
<fig id="F6" position="float">
<label>Figure 6</label>
<caption><p>Effects of limited data length on the heights of the side peaks of the SAC. <bold>(A)</bold> (Black) Theoretical SAC for a spike train of an infinite length for a 500 Hz stimulation. (Blue) SAC for a 50 ms long interval of a simulated spike train with theoretical decay of SAC peak heights (dotted blue). (Green) SAC for a 40 ms long interval of a simulated spike train with theoretical decay of SAC peak heights (dotted green). The concentration parameter &#x003BA; was 2.8713 corresponding to a VS of 0.8. <bold>(B)</bold> More examples for different data lengths of 30 (red) and 20 (orange) ms.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fnins-15-761826-g0006.tif"/>
</fig>
<p>The calculation of VS is affected by the recording time resolution (Ashida and Carr, <xref ref-type="bibr" rid="B3">2010</xref>). Similarly, CI is impacted by the SAC bin width &#x003C9;. For experimental data of cat AN and TB fibers, Joris et al. (<xref ref-type="bibr" rid="B38">2006</xref>) had already shown a decay of CI with increasing bin widths &#x003C9;, which was theoretically confirmed in our calculation (Equation 7). The true CI is underestimated for large &#x003C9; and decays toward 1 for &#x003C9;&#x0226B;100 &#x003BC;s for this 500 Hz example (<xref ref-type="fig" rid="F7">Figure 7A</xref>), because a large &#x003C9; effectively works as a low-pass filter by averaging out the spike rate in each bin. Since the decay factor in Equation (7) is a function of the product &#x003C9;<italic>f</italic>, the decay of CI starts at different values of &#x003C9;, depending on the frequency <italic>f</italic>. The decaying part of the curve in <xref ref-type="fig" rid="F7">Figure 7A</xref> will shift to the left (smaller &#x003C9;) if the frequency is increased. This frequency dependence is further investigated below.</p>
<fig id="F7" position="float">
<label>Figure 7</label>
<caption><p>Effects of the SAC bin width &#x003C9; on CI. <bold>(A)</bold> CI values for 88 different SAC bin widths. Spike trains simulated with a <italic>von Mises</italic> distribution (frequency = 500 Hz; concentration &#x003BA; = 1.5157; target VS = 0.60; mean spike rate = 200 spikes/s; time step dt = 0.002 ms; duration = 100 ms; and 400 repetitions) were used. The amount of error or bias in CI depends on the ratio between the spike sampling time step dt and the SAC bin width &#x003C9;, namely &#x003C9;/dt, being either <bold>(B)</bold> odd integer, <bold>(D)</bold> even integer or <bold>(F)</bold> non-integer. The gray dotted line represents the estimated CI (= 1.8120) based on the underlying &#x003BA; value. The dark blue line shows the mean CI values with error bars indicating the standard deviation for the simulated spike trains. The theoretical decay of CI with large &#x003C9; is illustrated by the cyan curve (see Equation 7). <bold>(C,E,G)</bold> Schematic illustrations for the effects of the SAC bin width &#x003C9;. <bold>(C)</bold> For an odd integer ratio &#x003C9;/dt, each bin has the same number of time points. <bold>(E)</bold> When &#x003C9;/dt is an even integer, the number of time points in each bin may or may not be equal depending on the rounding algorithm. <bold>(G)</bold> For a non-integer &#x003C9;/dt, the number of time points differs between two neighboring bins.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fnins-15-761826-g0007.tif"/>
</fig>
<p>Using a small bin width &#x003C9;, however, is not always optimal for error reduction. If &#x003C9; is too small, the SAC becomes more variable leading to strong deviations from the theoretical CI value (&#x003C9; &#x0003C;50 &#x003BC;s in <xref ref-type="fig" rid="F7">Figure 7A</xref>). For small &#x003C9;, three different cases should be considered, depending on the value of the ratio between the SAC time bin and spike timing resolution dt. When the value of &#x003C9;/dt is an odd integer, the simulated data closely follow the theoretical value (<xref ref-type="fig" rid="F7">Figure 7B</xref>). In this case, the number of data points in each SAC bin is constant (<xref ref-type="fig" rid="F7">Figure 7C</xref>). When the value of &#x003C9;/dt is an even integer, however, the calculation of CI can be erroneous (<xref ref-type="fig" rid="F7">Figure 7D</xref>), because the time points that are located on the border of two neighboring SAC time bins are pushed into one of the bins possibly in an uneven way, depending on the rounding algorithm used in the specific analysis program (<xref ref-type="fig" rid="F7">Figure 7E</xref>). We note that this rounding issue might appear differently, if the CI bin were not centered at 0 &#x003BC;s. Finally, if the quotient &#x003C9;/dt is not an integer, the error can be large (<xref ref-type="fig" rid="F7">Figure 7F</xref>), because the number of time points can vary between SAC bins (<xref ref-type="fig" rid="F7">Figure 7G</xref>).</p>
<p>Based on these theoretical considerations, we aim to derive a recommendation for the choice of reasonable SAC bin widths. In addition to &#x003C9;, the error in CI depends both on the frequency <italic>f</italic> and the concentration parameter &#x003BA; that controls the degree of phase-locking (Equation 7). For a given frequency, more prominent phase-locking, reflected in large &#x003BA; values, leads to a more pronounced CI decay (<xref ref-type="fig" rid="F8">Figure 8A</xref>) because the strength of the n-th harmonic (see Equation 7) monotonically increases with &#x003BA;. This observation allows us to estimate upper CI error bounds by only considering the maximal value of &#x003BA; that is physiologically plausible at each frequency. Using published data in cats (Joris et al., <xref ref-type="bibr" rid="B37">1994</xref>), we obtained an empirical approximation for the maximum values of VS at each frequency (<xref ref-type="fig" rid="F8">Figure 8B</xref>, blue line) and calculated the corresponding &#x003BA;<sub>max</sub> (<xref ref-type="fig" rid="F8">Figure 8C</xref>). The values of &#x003BA;<sub>max</sub> for AN fibers also matched the estimation by Peterson and Heil (<xref ref-type="bibr" rid="B51">2019</xref>, see their Figure 9). Our results suggest that a bin width of &#x003C9; &#x0003D; 50 &#x003BC;s keeps the relative error below 2.5 % for frequencies in the range of 200 and 5,000 Hz (<xref ref-type="fig" rid="F8">Figure 8D</xref>). The error is largest for frequencies between 2,000 and 3,000 Hz.</p>
<fig id="F8" position="float">
<label>Figure 8</label>
<caption><p>Estimation of the binning error in CI calculation depending on the bin size &#x003C9;, frequency <italic>f</italic>, and concentration parameter &#x003BA;. <bold>(A)</bold> Theoretical CI decay (see Equation 7) for four different frequencies and seven different &#x003BA; values. CI ratio was calculated as CI<sub>&#x003C9;</sub>/CI. <bold>(B)</bold> Empirical VS values measured in cats and their maximum values approximated by a function <inline-formula><mml:math id="M21"><mml:msub><mml:mrow><mml:mstyle class="text"><mml:mtext class="textrm" mathvariant="normal">VS</mml:mtext></mml:mstyle></mml:mrow><mml:mrow><mml:mstyle class="text"><mml:mtext class="textrm" mathvariant="normal">max</mml:mtext></mml:mstyle></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mo class="qopname">min</mml:mo><mml:mrow><mml:mo>{</mml:mo><mml:mrow><mml:mn>0</mml:mn><mml:mo>.</mml:mo><mml:mn>986</mml:mn><mml:mo>,</mml:mo><mml:mn>1</mml:mn><mml:mo>-</mml:mo><mml:msup><mml:mrow><mml:mrow><mml:mo stretchy="false">(</mml:mo><mml:mrow><mml:mi>f</mml:mi><mml:mo>/</mml:mo><mml:mn>5700</mml:mn></mml:mrow><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>.</mml:mo><mml:mn>5</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>}</mml:mo></mml:mrow></mml:math></inline-formula>. Symbols show cat TB fiber recordings (Joris et al., <xref ref-type="bibr" rid="B37">1994</xref>). Diamonds: phase-locked units; open triangles: presumed GBCs with primary-like-with-notch PSTHs; filled triangles: histologically confirmed GBCs. Dashed green line indicates the maximal VS values for cat AN fibers (Johnson, <xref ref-type="bibr" rid="B36">1980</xref>). Figure adapted from Ashida et al. (<xref ref-type="bibr" rid="B5">2019</xref>). <bold>(C)</bold> Estimation of &#x003BA;<sub>max</sub> from VS<sub>max</sub> in <bold>(B)</bold> calculated with Equation (3). <bold>(D)</bold> Upper CI error bounds for different bin widths calculated with the estimated &#x003BA;<sub>max</sub> shown in <bold>(C)</bold>. Relative errors were computed as (CI&#x02212;CI<sub>&#x003C9;</sub>)/CI. The gray dotted horizontal line highlights the relative error of 2.5 %.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fnins-15-761826-g0008.tif"/>
</fig>
<p>In summary, the SAC bin width &#x003C9; should be chosen to be equal to or smaller than 50 &#x003BC;s to avoid a substantial underestimation of CI. Furthermore, the amount of error in CI calculation depends on the ratio between the bin width &#x003C9; and the spike sampling time step dt. The bias is smallest in the odd integer case (<xref ref-type="fig" rid="F7">Figures 7B,C</xref>) and highest in the non-integer case (<xref ref-type="fig" rid="F7">Figures 7F,G</xref>).</p></sec></sec>
<sec sec-type="discussion" id="s4">
<title>4. Discussion</title>
<p>In the era of large-scale recording and simulation, the ability to compare data has become a fundamental issue in various scientific fields, including biology (Cao et al., <xref ref-type="bibr" rid="B12">2005</xref>; Vogt, <xref ref-type="bibr" rid="B68">2009</xref>; Mallott et al., <xref ref-type="bibr" rid="B47">2019</xref>) and neuroscience (Mulugeta et al., <xref ref-type="bibr" rid="B48">2018</xref>; Bzdok et al., <xref ref-type="bibr" rid="B11">2019</xref>). A number of practical suggestions have been made and implemented toward effective integration of multiple datasets (e.g., Poldrack and Gorgolewski, <xref ref-type="bibr" rid="B53">2014</xref>; Zehl et al., <xref ref-type="bibr" rid="B71">2016</xref>; Tratwal et al., <xref ref-type="bibr" rid="B64">2020</xref>). These ongoing efforts, however, do not necessarily guarantee that neurophysiological data that were published decades ago can be compared with more recent data quantified with different methods. As reviewed in the Introduction, VS has served as a practical measure of phase-locking, since it was introduced more than half a century ago (Goldberg and Brown, <xref ref-type="bibr" rid="B27">1969</xref>). More recently, the use of CI has been increasingly common, since SACs and CIs can be defined for a wider variety of stimuli than VS, including non-periodic acoustic stimulation (Joris et al., <xref ref-type="bibr" rid="B38">2006</xref>). To facilitate comparisons between phase-locked spiking data quantified with VS and those with CI, the present study established a mathematical relationship between these measures (<xref ref-type="fig" rid="F2">Figure 2F</xref>). Our mathematical formulation assumed a <italic>von Mises</italic> distribution characterized with the concentration parameter &#x003BA; that systematically affects both VS and CI (<xref ref-type="fig" rid="F2">Figures 2D,E</xref>).</p>
<p>Our theoretical predictions generally agreed with measured (<xref ref-type="fig" rid="F3">Figures 3C,D</xref>) or simulated (<xref ref-type="fig" rid="F3">Figures 3A,B</xref>) spiking data of several different auditory neurons, even though spike timings in real neurons do not necessarily follow the <italic>von Mises</italic> distribution (Peterson and Heil, <xref ref-type="bibr" rid="B51">2019</xref>). Real neurons and modeled AN fibers, for example, have refractory periods, while <italic>von Mises</italic> distributed spike trains do not. Recordings of auditory nerve fibers showed that refractoriness can affect VS especially at low frequencies (below 800 Hz; Avissar et al., <xref ref-type="bibr" rid="B7">2013</xref>; Peterson and Heil, <xref ref-type="bibr" rid="B51">2019</xref>). Furthermore, spiking timing of auditory nerve fibers and cochlear nucleus neurons are generally more regular than pure Poissonian spike trains (Rothman et al., <xref ref-type="bibr" rid="B55">1993</xref>; Heil and Peterson, <xref ref-type="bibr" rid="B32">2017</xref>). The AN and GBC models we used (Bruce et al., <xref ref-type="bibr" rid="B10">2018</xref>; Ashida et al., <xref ref-type="bibr" rid="B5">2019</xref>) include refractory periods and show more regular spiking than the Poisson process. Nevertheless, our simulation results with these models showed a good agreement with the curve for the <italic>von Mises</italic> distribution (<xref ref-type="fig" rid="F3">Figure 3B</xref>), suggesting that the violations of these mathematical assumptions may only have limited effects on the theoretical VS-CI relationship. More systematic analyses on the effects of refractoriness and regularity on SAC would be a topic of future studies.</p>
<p>Deviations of data points from the theoretical curve may originate from a skewed (<xref ref-type="fig" rid="F4">Figures 4A2,B2</xref>) or bimodal (<xref ref-type="fig" rid="F4">Figures 4C2,D2</xref>) phase distribution (Peterson and Heil, <xref ref-type="bibr" rid="B51">2019</xref>). In auditory nerve recordings <italic>in vivo</italic>, such bimodal distributions were observed, for example, with low-frequency, high-intensity acoustic stimulation (Johnson, <xref ref-type="bibr" rid="B36">1980</xref>; Wei et al., <xref ref-type="bibr" rid="B69">2017</xref>) which induces considerable harmonic distortions in the peripheral response (Peterson and Heil, <xref ref-type="bibr" rid="B51">2019</xref>, also see references therein for more examples). In addition to these relatively apparent cases, the value of CI can be higher than what is expected from VS, even if the phase distribution resembles a <italic>von Mises</italic> distribution. In our example (<xref ref-type="fig" rid="F4">Figure 4E2</xref>), spikes across trials were more likely to occur in the same or neighboring stimulus cycles than naively expected from the period histogram that only retains the phase information of spikes in each period (<xref ref-type="fig" rid="F5">Figures 5B,C</xref>). These results indicate that the applicability of our theoretical results is limited to unimodal (<italic>von-Mises</italic>-like) phase distributions without additional trial-to-trial coincidences due to variations of the stimulus parameters. A more appropriate fitting of skewed or bimodal phase distribution would require modifications of the fitting function by, e.g., summing multiple unimodal distributions or introducing additional shape parameters to create asymmetry (Gatto and Jammalamadaka, <xref ref-type="bibr" rid="B25">2007</xref>; Umbach and Jammalamadaka, <xref ref-type="bibr" rid="B65">2009</xref>; Abe and Pewsey, <xref ref-type="bibr" rid="B1">2011</xref>; Kim and SenGupta, <xref ref-type="bibr" rid="B41">2013</xref>). In the cat auditory nerve, for example, additional one or two distortion components would be necessary to account for the observed spiking patterns (Peterson and Heil, <xref ref-type="bibr" rid="B51">2019</xref>).</p>
<p>In addition to the violation of theoretical assumptions, multiple sources of errors can affect the calculation of CI. While the length <italic>D</italic> of each trial would not affect the value of CI (<xref ref-type="fig" rid="F6">Figure 6</xref>), the size of the SAC time bin &#x003C9; can constitute a major error source (<xref ref-type="fig" rid="F7">Figure 7</xref>). If &#x003C9; is too large, the resulting CI value becomes smaller than the theoretical estimation, because the SAC peak is reduced by averaging within the time bin. A similar effect was shown for the calculation of VS (Ashida and Carr, <xref ref-type="bibr" rid="B3">2010</xref>). For small &#x003C9;, the calculation of CI can be error-prone, especially when the number of data points is not uniform across SAC bins (<xref ref-type="fig" rid="F7">Figures 7D,F</xref>). In other words, the size of SAC bins should be selected in a way that the number of time steps in each bin becomes constant (<xref ref-type="fig" rid="F7">Figures 7B,C</xref>). Considering these factors, we support the selection of &#x003C9; &#x0003D; 50 &#x003BC;s (or some similar value), which was used by the original study of Joris et al. (<xref ref-type="bibr" rid="B38">2006</xref>), provided that the recording time step is sufficiently small (e.g., 10 &#x003BC;s or less). In our <italic>in vivo</italic> recording data, however, the spike times were usually sampled at a lower rate (48 kHz, corresponding to a 20.8 &#x003BC;s time step) due to technical restrictions. Hence, the discrepancy between the theoretical prediction and empirical data (<xref ref-type="fig" rid="F3">Figure 3C</xref>) could be (at least partly) due to the effect of the SAC bin size. Furthermore, the number of repeated trials needs to be large enough to have sufficiently many spike coincidences in each SAC time bin. Otherwise, the empirical CI value may differ from the theoretical prediction, which is exemplified by larger error bars for small &#x003C9; (<xref ref-type="fig" rid="F7">Figure 7B</xref>). Moreover, for an estimation of CI from VS, even a small error in VS may result in a large error of CI, especially for VS&#x0003E;0.95. This is because the value of VS is bounded by one, while the value of CI can be infinitely large (<xref ref-type="fig" rid="F2">Figure 2F</xref>).</p>
<p>Comparisons of multiple measures may reveal hidden structures of spike trains. As demonstrated in <xref ref-type="fig" rid="F5">Figures 5B,C</xref>, a comparison of the VS-CI relationship with the theoretical prediction may help us discover additional spiking patterns that may not be found with a period histogram or SAC alone. While CI contains broadband spectral information, VS is a measure at a specific frequency (Parida et al., <xref ref-type="bibr" rid="B49">2021</xref>). Expanding the concept of VS is possible by introducing multiple reference frequencies (van Hemmen and Vollmayr, <xref ref-type="bibr" rid="B67">2013</xref>). For spectrally rich acoustic stimuli, such as natural sounds, locking to more than one frequencies may have to be considered (Joris et al., <xref ref-type="bibr" rid="B39">2004</xref>). Even though the use of natural stimuli is increasing common in neuroscience, response patterns to simple stimuli still provide fundamental information about the functionality of the sensory system (e.g., Rust and Movshon, <xref ref-type="bibr" rid="B57">2005</xref>). It is not always clear, however, how neuronal responses to simple stimuli can be related with those to complex stimuli. Future investigation on the relationship between CI and frequency-dependent VS under physiologically reasonable mathematical conditions might be useful to bridge between fundamental spiking patterns of auditory neurons and responses to broadband acoustic stimulation.</p>
<p>A number of measures have been developed to quantify the degree of correlation between spike trains, including SACs and its variations (reviewed in Cutts and Eglen, <xref ref-type="bibr" rid="B19">2014</xref>). Nevertheless, quantitative relationships between these measures are not always clear. Gai and Carney (<xref ref-type="bibr" rid="B24">2008</xref>) compared CI, the Victor-Purpura spike distance metric, and mutual information to quantify time-locked spiking patterns recorded in the cochlear nucleus. Our theoretical method used in this study may also be applied to temporal measures other than VS and CI. Such an analysis would not only reveal the mathematical relations behind these measures but also provide practical information on which measure to use for quantifying temporal information processing in the nervous system.</p></sec>
<sec sec-type="data-availability" id="s5">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="supplementary-material" rid="SM1">Supplementary Material</xref>, further inquiries can be directed to the corresponding author. Matlab program code for some of the simulations and analyses in this study is available online at <ext-link ext-link-type="uri" xlink:href="https://github.com/pinkbox-models/CI-VS-2021">https://github.com/pinkbox-models/CI-VS-2021</ext-link>.</p></sec>
<sec id="s6">
<title>Ethics Statement</title>
<p>Ethical review and approval was not required for the animal study because only existing data collected in previously published studies were re-analyzed.</p></sec>
<sec id="s7">
<title>Author Contributions</title>
<p>DK and GA: conceptualization, formal analysis, numerical simulation, data analysis, interpretation, visualization, and drafting manuscript. CC and GA: physiological data collection. CC and JK: resources. CC, JK, and GA: funding acquisition. JK and GA: project administration and supervision. DK, CC, JK, and GA: reviewing and editing manuscript and approving submission. All authors contributed to the article and approved the submitted version.</p></sec>
<sec sec-type="funding-information" id="s8">
<title>Funding</title>
<p>This work was supported by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany&#x00027;s Excellence Strategy EXC2177/1 (Project ID 390895286), Associate Junior Fellowship from the Hanse-Wissenschaftskolleg (GA), and NIH/NIDCD Grant R01DC019341 (CC).</p>
</sec>
<sec sec-type="COI-statement" id="conf1">
<title>Conflict of Interest</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 sec-type="disclaimer" id="s9">
<title>Publisher&#x00027;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p></sec> </body>
<back>
<ack><p>We thank the members of the Computational Neuroscience Group in Oldenburg, especially Ann-Katrin Tzschaschel, for active discussions.</p>
</ack><sec sec-type="supplementary-material" id="s10">
<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/fnins.2021.761826/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fnins.2021.761826/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"/></sec>
<ref-list>
<title>References</title>
<ref id="B1">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Abe</surname> <given-names>T.</given-names></name> <name><surname>Pewsey</surname> <given-names>A.</given-names></name></person-group> (<year>2011</year>). <article-title>Sine-skewed circular distributions</article-title>. <source>Stat. Pap</source>. <volume>52</volume>, <fpage>683</fpage>&#x02013;<lpage>707</lpage>. <pub-id pub-id-type="doi">10.1007/s00362-009-0277-x</pub-id></citation>
</ref>
<ref id="B2">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Ashida</surname> <given-names>G..</given-names></name></person-group> (<year>2015</year>). <article-title>Barn owl and sound localization</article-title>. <source>Acoust. Sci. Tech</source>. <volume>36</volume>, <fpage>275</fpage>&#x02013;<lpage>285</lpage>. <pub-id pub-id-type="doi">10.1250/ast.36.275</pub-id></citation>
</ref>
<ref id="B3">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Ashida</surname> <given-names>G.</given-names></name> <name><surname>Carr</surname> <given-names>C. E.</given-names></name></person-group> (<year>2010</year>). <article-title>Effect of sampling frequency on the measurement of phase-locked action potentials</article-title>. <source>Front. Neurosci</source>. <volume>4</volume>:<fpage>172</fpage>. <pub-id pub-id-type="doi">10.3389/fnins.2010.00172</pub-id><pub-id pub-id-type="pmid">20953249</pub-id></citation></ref>
<ref id="B4">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Ashida</surname> <given-names>G.</given-names></name> <name><surname>Funabiki</surname> <given-names>K.</given-names></name> <name><surname>Carr</surname> <given-names>C. E.</given-names></name></person-group> (<year>2013</year>). <article-title>Theoretical foundations of the sound analog membrane potential that underlies coincidence detection in the barn owl</article-title>. <source>Front. Comput. Neurosci</source> <volume>7</volume>:<fpage>151</fpage>. <pub-id pub-id-type="doi">10.3389/fncom.2013.00151</pub-id><pub-id pub-id-type="pmid">24265616</pub-id></citation></ref>
<ref id="B5">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Ashida</surname> <given-names>G.</given-names></name> <name><surname>Heinermann</surname> <given-names>H. T.</given-names></name> <name><surname>Kretzberg</surname> <given-names>J.</given-names></name></person-group> (<year>2019</year>). <article-title>Neuronal population model of globular bushy cells covering unit-to-unit variability</article-title>. <source>PLoS Comput. Biol</source>. <volume>15</volume>:<fpage>e1007563</fpage>. <pub-id pub-id-type="doi">10.1371/journal.pcbi.1007563</pub-id><pub-id pub-id-type="pmid">31881018</pub-id></citation></ref>
<ref id="B6">
<citation citation-type="book"><person-group person-group-type="author"><name><surname>Ashida</surname> <given-names>G.</given-names></name> <name><surname>Wagner</surname> <given-names>H.</given-names></name> <name><surname>Carr</surname> <given-names>C. E.</given-names></name></person-group> (<year>2010</year>). <article-title>&#x0201C;Processing of phase-locked spikes and periodic signals,&#x0201D;</article-title> in <source>Analysis of Parallel Spike Trains</source>, eds S. Gr&#x000FC;n and S. Rotter (<publisher-loc>New York, NY</publisher-loc>: <publisher-name>Springer</publisher-name>), <fpage>59</fpage>&#x02013;<lpage>74</lpage>.</citation>
</ref>
<ref id="B7">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Avissar</surname> <given-names>M.</given-names></name> <name><surname>Wittig</surname> <given-names>J. H.</given-names></name> <name><surname>Saunders</surname> <given-names>J. C.</given-names></name> <name><surname>Parsons</surname> <given-names>T. D.</given-names></name></person-group> (<year>2013</year>). <article-title>Refractoriness enhances temporal coding by auditory nerve fibers</article-title>. <source>J. Neurosci</source>. <volume>33</volume>, <fpage>7681</fpage>&#x02013;<lpage>7690</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.3405-12.2013</pub-id><pub-id pub-id-type="pmid">23637161</pub-id></citation></ref>
<ref id="B8">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Baker</surname> <given-names>C. A.</given-names></name> <name><surname>Kohashi</surname> <given-names>T.</given-names></name> <name><surname>Lyons-Warren</surname> <given-names>A. M.</given-names></name> <name><surname>Ma</surname> <given-names>X.</given-names></name> <name><surname>Carlson</surname> <given-names>B. A.</given-names></name> <name><surname>Krahe</surname> <given-names>R.</given-names></name> <etal/></person-group>. (<year>2013</year>). <article-title>Multiplexed temporal coding of electric communication signals in mormyrid fishes</article-title>. <source>J. Exp. Biol</source>. <volume>216</volume>, <fpage>2365</fpage>&#x02013;<lpage>2379</lpage>. <pub-id pub-id-type="doi">10.1242/jeb.082289</pub-id><pub-id pub-id-type="pmid">23761462</pub-id></citation></ref>
<ref id="B9">
<citation citation-type="book"><person-group person-group-type="author"><name><surname>Balci</surname> <given-names>F.</given-names></name> <name><surname>Brunner</surname> <given-names>D.</given-names></name> <name><surname>Meck</surname> <given-names>W. H.</given-names></name> <name><surname>Moore</surname> <given-names>H.</given-names></name></person-group> (<year>2009</year>). <article-title>&#x0201C;Timing deficits in aging and neuropathology,&#x0201D;</article-title> in <source>Animal Models of Human Cognitive Aging</source>, eds J. L. Bizon and A. Woods (<publisher-loc>New York, NY</publisher-loc>: <publisher-name>Springer</publisher-name>), <fpage>161</fpage>&#x02013;<lpage>201</lpage>.</citation>
</ref>
<ref id="B10">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Bruce</surname> <given-names>I. C.</given-names></name> <name><surname>Erfani</surname> <given-names>Y.</given-names></name> <name><surname>Zilany</surname> <given-names>M. S. A.</given-names></name></person-group> (<year>2018</year>). <article-title>A phenomenological model of the synapse between the inner hair cell and auditory nerve: implications of limited neurotransmitter release sites</article-title>. <source>Hear. Res</source>. <volume>360</volume>, <fpage>40</fpage>&#x02013;<lpage>54</lpage>. <pub-id pub-id-type="doi">10.1016/j.heares.2017.12.016</pub-id><pub-id pub-id-type="pmid">29395616</pub-id></citation></ref>
<ref id="B11">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Bzdok</surname> <given-names>D.</given-names></name> <name><surname>Nichols</surname> <given-names>T. E.</given-names></name> <name><surname>Smith</surname> <given-names>S. M.</given-names></name></person-group> (<year>2019</year>). <article-title>Towards algorithmic analytics for large-scale datasets</article-title>. <source>Nat. Mach. Intell</source>. <volume>1</volume>, <fpage>296</fpage>&#x02013;<lpage>306</lpage>. <pub-id pub-id-type="doi">10.1038/s42256-019-0069-5</pub-id><pub-id pub-id-type="pmid">31701088</pub-id></citation></ref>
<ref id="B12">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Cao</surname> <given-names>Y.</given-names></name> <name><surname>Hawkins</surname> <given-names>C. P.</given-names></name> <name><surname>Storey</surname> <given-names>A. W.</given-names></name></person-group> (<year>2005</year>). <article-title>A method for measuring the comparability of different sampling methods used in biological surveys: implications for data integration and synthesis</article-title>. <source>Freshw. Biol</source>. <volume>50</volume>, <fpage>1105</fpage>&#x02013;<lpage>1115</lpage>. <pub-id pub-id-type="doi">10.1111/j.1365-2427.2005.01377.x</pub-id></citation>
</ref>
<ref id="B13">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Carr</surname> <given-names>C. E.</given-names></name> <name><surname>Friedman</surname> <given-names>M. A.</given-names></name></person-group> (<year>1999</year>). <article-title>Evolution of time coding systems</article-title>. <source>Neural Comput</source>. <volume>11</volume>, <fpage>1</fpage>&#x02013;<lpage>20</lpage>. <pub-id pub-id-type="doi">10.1162/089976699300016773</pub-id><pub-id pub-id-type="pmid">9950719</pub-id></citation></ref>
<ref id="B14">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Carr</surname> <given-names>C. E.</given-names></name> <name><surname>K&#x000F6;ppl</surname> <given-names>C.</given-names></name></person-group> (<year>2004</year>). <article-title>Coding interaural time differences at low best frequencies in the barn owl</article-title>. <source>J. Physiol</source>. <volume>98</volume>, <fpage>99</fpage>&#x02013;<lpage>112</lpage>. <pub-id pub-id-type="doi">10.1016/j.jphysparis.2004.03.003</pub-id><pub-id pub-id-type="pmid">15477025</pub-id></citation></ref>
<ref id="B15">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Carr</surname> <given-names>C. E.</given-names></name> <name><surname>Soares</surname> <given-names>D.</given-names></name> <name><surname>Smolders</surname> <given-names>J.</given-names></name> <name><surname>Simon</surname> <given-names>J. Z.</given-names></name></person-group> (<year>2009</year>). <article-title>Detection of interaural time differences in the alligator</article-title>. <source>J. Neurosci</source>. <volume>29</volume>, <fpage>7978</fpage>&#x02013;<lpage>7990</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.6154-08.2009</pub-id><pub-id pub-id-type="pmid">19553438</pub-id></citation></ref>
<ref id="B16">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Catela</surname> <given-names>C.</given-names></name> <name><surname>Shin</surname> <given-names>M. M.</given-names></name> <name><surname>Dasen</surname> <given-names>J. S.</given-names></name></person-group> (<year>2015</year>). <article-title>Assembly and function of spinal circuits for motor control</article-title>. <source>Annu. Rev. Cell. Dev. Biol</source>. <volume>31</volume>, <fpage>669</fpage>&#x02013;<lpage>698</lpage>. <pub-id pub-id-type="doi">10.1146/annurev-cellbio-100814-125155</pub-id><pub-id pub-id-type="pmid">26393773</pub-id></citation></ref>
<ref id="B17">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Colburn</surname> <given-names>H. S..</given-names></name></person-group> (<year>1973</year>). <article-title>Theory of binaural interaction based on auditory-nerve data. I. General strategy and preliminary results on interaural discrimination</article-title>. <source>J. Acoust. Soc. Am</source>. <volume>54</volume>, <fpage>1458</fpage>&#x02013;<lpage>1470</lpage>. <pub-id pub-id-type="doi">10.1121/1.1914445</pub-id><pub-id pub-id-type="pmid">4780800</pub-id></citation></ref>
<ref id="B18">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Cullen</surname> <given-names>K. E..</given-names></name></person-group> (<year>2012</year>). <article-title>The vestibular system: multimodal integration and encoding of self-motion for motor control</article-title>. <source>Trends Neurosci</source>. <volume>35</volume>, <fpage>185</fpage>&#x02013;<lpage>196</lpage>. <pub-id pub-id-type="doi">10.1016/j.tins.2011.12.001</pub-id><pub-id pub-id-type="pmid">22245372</pub-id></citation></ref>
<ref id="B19">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Cutts</surname> <given-names>C. S.</given-names></name> <name><surname>Eglen</surname> <given-names>S. J.</given-names></name></person-group> (<year>2014</year>). <article-title>Detecting pairwise correlations in spike trains: an objective comparison of methods and application to the study of retinal waves</article-title>. <source>J. Neurosci</source>. <volume>34</volume>, <fpage>14288</fpage>&#x02013;<lpage>14303</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.2767-14.2014</pub-id><pub-id pub-id-type="pmid">25339742</pub-id></citation></ref>
<ref id="B20">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>De Zeeuw</surname> <given-names>C. I.</given-names></name> <name><surname>Hoebeek</surname> <given-names>F. E.</given-names></name> <name><surname>Bosman</surname> <given-names>L. W. J.</given-names></name> <name><surname>Schonewille</surname> <given-names>M.</given-names></name> <name><surname>Witter</surname> <given-names>L.</given-names></name> <name><surname>Koekkoek</surname> <given-names>S. K.</given-names></name></person-group> (<year>2011</year>). <article-title>Spatiotemporal patterns in the cerebellum</article-title>. <source>Nat. Rev. Neurosci</source>. <volume>12</volume>, <fpage>327</fpage>&#x02013;<lpage>344</lpage>. <pub-id pub-id-type="doi">10.1038/nrn3011</pub-id><pub-id pub-id-type="pmid">21544091</pub-id></citation></ref>
<ref id="B21">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Dragoi</surname> <given-names>G..</given-names></name></person-group> (<year>2020</year>). <article-title>Cell assemblies, sequences and temporal coding in the hippocampus</article-title>. <source>Curr. Opin. Neurobiol</source>. <volume>64</volume>, <fpage>111</fpage>&#x02013;<lpage>118</lpage>. <pub-id pub-id-type="doi">10.1016/j.conb.2020.03.003</pub-id><pub-id pub-id-type="pmid">32375084</pub-id></citation></ref>
<ref id="B22">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Dreyer</surname> <given-names>A.</given-names></name> <name><surname>Delgutte</surname> <given-names>B.</given-names></name></person-group> (<year>2006</year>). <article-title>Phase locking of auditory-nerve fibers to the envelopes of high-frequency sounds: implications for sound localization</article-title>. <source>J. Neurophysiol</source>. <volume>96</volume>, <fpage>2327</fpage>&#x02013;<lpage>2341</lpage>. <pub-id pub-id-type="doi">10.1152/jn.00326.2006</pub-id><pub-id pub-id-type="pmid">16807349</pub-id></citation></ref>
<ref id="B23">
<citation citation-type="book"><person-group person-group-type="author"><name><surname>Fisher</surname> <given-names>N. I..</given-names></name></person-group> (<year>1993</year>). <source>Statistical Analysis of Circular Data</source>. <publisher-loc>Cambridge, UK</publisher-loc>: <publisher-name>Cambridge University Press</publisher-name>.</citation>
</ref>
<ref id="B24">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Gai</surname> <given-names>Y.</given-names></name> <name><surname>Carney</surname> <given-names>L. H.</given-names></name></person-group> (<year>2008</year>). <article-title>Statistical analyses of temporal information in auditory brainstem responses to tones in noise: correlation index and spike-distance metric</article-title>. <source>J. Assoc. Res. Otolaryngol</source>. <volume>9</volume>, <fpage>373</fpage>&#x02013;<lpage>387</lpage>. <pub-id pub-id-type="doi">10.1007/s10162-008-0129-8</pub-id><pub-id pub-id-type="pmid">18535861</pub-id></citation></ref>
<ref id="B25">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Gatto</surname> <given-names>R.</given-names></name> <name><surname>Jammalamadaka</surname> <given-names>S. R.</given-names></name></person-group> (<year>2007</year>). <article-title>The generalized von Mises distribution</article-title>. <source>Stat. Methodol</source>. <volume>4</volume>, <fpage>341</fpage>&#x02013;<lpage>353</lpage>. <pub-id pub-id-type="doi">10.1016/j.stamet.2006.11.003</pub-id></citation>
</ref>
<ref id="B26">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Gire</surname> <given-names>D. H.</given-names></name> <name><surname>Restrepo</surname> <given-names>D.</given-names></name> <name><surname>Sejnowski</surname> <given-names>T. J.</given-names></name> <name><surname>Greer</surname> <given-names>C.</given-names></name> <name><surname>De Carlos</surname> <given-names>J. A.</given-names></name> <name><surname>Lopez-Mascaraque</surname> <given-names>L.</given-names></name></person-group> (<year>2013</year>). <article-title>Temporal processing in the olfactory system: can we see a smell?</article-title> <source>Neuron</source> <volume>78</volume>, <fpage>416</fpage>&#x02013;<lpage>432</lpage>. <pub-id pub-id-type="doi">10.1016/j.neuron.2013.04.033</pub-id><pub-id pub-id-type="pmid">23664611</pub-id></citation></ref>
<ref id="B27">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Goldberg</surname> <given-names>J. M.</given-names></name> <name><surname>Brown</surname> <given-names>P. B.</given-names></name></person-group> (<year>1969</year>). <article-title>Response of binaural neurons of dog superior olivary complex to dichotic tonal stimuli: some physiological mechanisms of sound localization</article-title>. <source>J. Neurophysiol</source>. <volume>32</volume>, <fpage>613</fpage>&#x02013;<lpage>636</lpage>. <pub-id pub-id-type="doi">10.1152/jn.1969.32.4.613</pub-id><pub-id pub-id-type="pmid">5810617</pub-id></citation></ref>
<ref id="B28">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Grothe</surname> <given-names>B.</given-names></name> <name><surname>Pecka</surname> <given-names>M.</given-names></name> <name><surname>McAlpine</surname> <given-names>D.</given-names></name></person-group> (<year>2010</year>). <article-title>Mechanisms of sound localization in mammals</article-title>. <source>Physiol. Rev</source>. <volume>90</volume>, <fpage>983</fpage>&#x02013;<lpage>1012</lpage>. <pub-id pub-id-type="doi">10.1152/physrev.00026.2009</pub-id><pub-id pub-id-type="pmid">20664077</pub-id></citation></ref>
<ref id="B29">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Hallock</surname> <given-names>R. M.</given-names></name> <name><surname>Di Lorenzo</surname> <given-names>P. M.</given-names></name></person-group> (<year>2006</year>). <article-title>Temporal coding in the gustatory system</article-title>. <source>Neurosci. Biobehav. Rev</source>. <volume>30</volume>, <fpage>1145</fpage>&#x02013;<lpage>1160</lpage>. <pub-id pub-id-type="doi">10.1016/j.neubiorev.2006.07.005</pub-id><pub-id pub-id-type="pmid">16979239</pub-id></citation></ref>
<ref id="B30">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Heeringa</surname> <given-names>A. N.</given-names></name> <name><surname>Zhang</surname> <given-names>L.</given-names></name> <name><surname>Ashida</surname> <given-names>G.</given-names></name> <name><surname>Beutelmann</surname> <given-names>R.</given-names></name> <name><surname>Steenken</surname> <given-names>F.</given-names></name> <name><surname>K&#x000F6;ppl</surname> <given-names>C.</given-names></name></person-group> (<year>2019</year>). <article-title>Temporal coding of single auditory nerve fibers is not degraded in aging gerbils</article-title>. <source>J. Neurosci</source>. <volume>40</volume>, <fpage>343</fpage>&#x02013;<lpage>354</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.2784-18.2019</pub-id><pub-id pub-id-type="pmid">31719164</pub-id></citation></ref>
<ref id="B31">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Heil</surname> <given-names>P.</given-names></name> <name><surname>Peterson</surname> <given-names>A. J.</given-names></name></person-group> (<year>2015</year>). <article-title>Basic response properties of auditory nerve fibers: a review</article-title>. <source>Cell. Tissue Res</source>. <volume>361</volume>, <fpage>129</fpage>&#x02013;<lpage>158</lpage>. <pub-id pub-id-type="doi">10.1007/s00441-015-2177-9</pub-id><pub-id pub-id-type="pmid">25920587</pub-id></citation></ref>
<ref id="B32">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Heil</surname> <given-names>P.</given-names></name> <name><surname>Peterson</surname> <given-names>A. J.</given-names></name></person-group> (<year>2017</year>). <article-title>Spike timing in auditory-nerve fibers during spontaneous activity and phase locking</article-title>. <source>Synapse</source> <volume>71</volume>, <fpage>5</fpage>&#x02013;<lpage>36</lpage>. <pub-id pub-id-type="doi">10.1002/syn.21925</pub-id><pub-id pub-id-type="pmid">27466786</pub-id></citation></ref>
<ref id="B33">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Heinz</surname> <given-names>M. G.</given-names></name> <name><surname>Swaminathan</surname> <given-names>J.</given-names></name></person-group> (<year>2009</year>). <article-title>Quantifying envelope and fine-structure coding in auditory nerve responses to chimaeric speech</article-title>. <source>J. Assoc. Res. Otolaryngol</source>. <volume>10</volume>, <fpage>407</fpage>&#x02013;<lpage>423</lpage>. <pub-id pub-id-type="doi">10.1007/s10162-009-0169-8</pub-id><pub-id pub-id-type="pmid">19365691</pub-id></citation></ref>
<ref id="B34">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Huet</surname> <given-names>A.</given-names></name> <name><surname>Desmadryl</surname> <given-names>G.</given-names></name> <name><surname>Justal</surname> <given-names>T.</given-names></name> <name><surname>Nouvian</surname> <given-names>R.</given-names></name> <name><surname>Puel</surname> <given-names>J.-L.</given-names></name> <name><surname>Bourien</surname> <given-names>J.</given-names></name></person-group> (<year>2018</year>). <article-title>The interplay between spike-time and spike-rate modes in the auditory nerve encodes tone-in-noise threshold</article-title>. <source>J. Neurosci</source>. <volume>38</volume>, <fpage>5727</fpage>&#x02013;<lpage>5738</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.3103-17.2018</pub-id><pub-id pub-id-type="pmid">29793977</pub-id></citation></ref>
<ref id="B35">
<citation citation-type="thesis"><person-group person-group-type="author"><name><surname>Johnson</surname> <given-names>D. H..</given-names></name></person-group> (<year>1974</year>). <source>The response of single auditory-nerve fibers in the cat to single tones: synchrony and average discharge rate</source> (<publisher-loc>Ph.D. thesis</publisher-loc>), Massachusetts Institute of Technology, Cambridge, MA. Available online at: <ext-link ext-link-type="uri" xlink:href="http://hdl.handle.net/1721.1/61806">http://hdl.handle.net/1721.1/61806</ext-link></citation>
</ref>
<ref id="B36">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Johnson</surname> <given-names>D. H..</given-names></name></person-group> (<year>1980</year>). <article-title>The relationship between spike rate and synchrony in responses of auditory&#x02013;nerve fibers to single tones</article-title>. <source>J. Acoust. Soc. Am</source>. <volume>68</volume>, <fpage>1115</fpage>&#x02013;<lpage>1122</lpage>. <pub-id pub-id-type="doi">10.1121/1.384982</pub-id><pub-id pub-id-type="pmid">7419827</pub-id></citation></ref>
<ref id="B37">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Joris</surname> <given-names>P. X.</given-names></name> <name><surname>Carney</surname> <given-names>L. H.</given-names></name> <name><surname>Smith</surname> <given-names>P. H.</given-names></name> <name><surname>Yin</surname> <given-names>T. C.</given-names></name></person-group> (<year>1994</year>). <article-title>Enhancement of neural synchronization in the anteroventral cochlear nucleus. I. Responses to tones at the characteristic frequency</article-title>. <source>J. Neurophysiol</source>. <volume>71</volume>, <fpage>1022</fpage>&#x02013;<lpage>1036</lpage>. <pub-id pub-id-type="doi">10.1152/jn.1994.71.3.1022</pub-id><pub-id pub-id-type="pmid">8201399</pub-id></citation></ref>
<ref id="B38">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Joris</surname> <given-names>P. X.</given-names></name> <name><surname>Louage</surname> <given-names>D. H.</given-names></name> <name><surname>Cardoen</surname> <given-names>L.</given-names></name> <name><surname>van der Heijden</surname> <given-names>M.</given-names></name></person-group> (<year>2006</year>). <article-title>Correlation index: a new metric to quantify temporal coding</article-title>. <source>Hear. Res</source>. 216&#x02013;<volume>217</volume>, <fpage>19</fpage>&#x02013;<lpage>30</lpage>. <pub-id pub-id-type="doi">10.1016/j.heares.2006.03.010</pub-id><pub-id pub-id-type="pmid">16644160</pub-id></citation></ref>
<ref id="B39">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Joris</surname> <given-names>P. X.</given-names></name> <name><surname>Schreiner</surname> <given-names>C. E.</given-names></name> <name><surname>Rees</surname> <given-names>A.</given-names></name></person-group> (<year>2004</year>). <article-title>Neural processing of amplitude-modulated sounds</article-title>. <source>Physiol. Rev</source>. <volume>84</volume>, <fpage>541</fpage>&#x02013;<lpage>577</lpage>. <pub-id pub-id-type="doi">10.1152/physrev.00029.2003</pub-id><pub-id pub-id-type="pmid">15044682</pub-id></citation></ref>
<ref id="B40">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Keine</surname> <given-names>C.</given-names></name> <name><surname>R&#x000FC;bsamen</surname> <given-names>R.</given-names></name> <name><surname>Englitz</surname> <given-names>B.</given-names></name></person-group> (<year>2016</year>). <article-title>Inhibition in the auditory brainstem enhances signal representation and regulates gain in complex acoustic environments</article-title>. <source>Elife</source> <volume>5</volume>:<fpage>e19295</fpage>. <pub-id pub-id-type="doi">10.7554/eLife.19295</pub-id><pub-id pub-id-type="pmid">27855778</pub-id></citation></ref>
<ref id="B41">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Kim</surname> <given-names>S.</given-names></name> <name><surname>SenGupta</surname> <given-names>A.</given-names></name></person-group> (<year>2013</year>). <article-title>A three-parameter generalized von Mises distribution</article-title>. <source>Stat. Pap</source>. <volume>54</volume>, <fpage>685</fpage>&#x02013;<lpage>693</lpage>. <pub-id pub-id-type="doi">10.1007/s00362-012-0454-1</pub-id></citation>
</ref>
<ref id="B42">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>K&#x000F6;ppl</surname> <given-names>C..</given-names></name></person-group> (<year>1997</year>). <article-title>Phase locking to high frequencies in the auditory nerve and cochlear nucleus magnocellularis of the barn owl, Tyto alba</article-title>. <source>J. Neurosci</source>. <volume>17</volume>, <fpage>3312</fpage>&#x02013;<lpage>3321</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.17-09-03312.1997</pub-id><pub-id pub-id-type="pmid">9096164</pub-id></citation></ref>
<ref id="B43">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>K&#x000F6;ppl</surname> <given-names>C.</given-names></name> <name><surname>Carr</surname> <given-names>C. E.</given-names></name></person-group> (<year>2008</year>). <article-title>Maps of interaural time difference in the chicken&#x00027;s brainstem nucleus laminaris</article-title>. <source>Biol. Cybern</source>. <volume>98</volume>, <fpage>541</fpage>&#x02013;<lpage>559</lpage>. <pub-id pub-id-type="doi">10.1007/s00422-008-0220-6</pub-id><pub-id pub-id-type="pmid">18491165</pub-id></citation></ref>
<ref id="B44">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Kreeger</surname> <given-names>L. J.</given-names></name> <name><surname>Arshed</surname> <given-names>A.</given-names></name> <name><surname>MacLeod</surname> <given-names>K. M.</given-names></name></person-group> (<year>2012</year>). Intrinsic firing properties in the avian auditory brain stem allow both integration and encoding of temporally modulated noisy inputs <italic>in vitro</italic>. <italic>J. Neurophysiol</italic>. <volume>108</volume>, <fpage>2794</fpage>&#x02013;<lpage>2809</lpage>. <pub-id pub-id-type="doi">10.1152/jn.00092.2012</pub-id><pub-id pub-id-type="pmid">22914650</pub-id></citation></ref>
<ref id="B45">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Kutil</surname> <given-names>R..</given-names></name></person-group> (<year>2012</year>). <article-title>Biased and unbiased estimation of the circular mean resultant length and its variance</article-title>. <source>Statistics</source> <volume>46</volume>, <fpage>549</fpage>&#x02013;<lpage>561</lpage>. <pub-id pub-id-type="doi">10.1080/02331888.2010.543463</pub-id></citation>
</ref>
<ref id="B46">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Lehman</surname> <given-names>F. O.</given-names></name> <name><surname>Bartussek</surname> <given-names>J.</given-names></name></person-group> (<year>2017</year>). <article-title>Neural control and precision of flight muscle activation in Drosophila</article-title>. <source>J. Comp. Physiol. A Neuroethol</source>. <volume>203</volume>, <fpage>1</fpage>&#x02013;<lpage>14</lpage>. <pub-id pub-id-type="doi">10.1007/s00359-016-1133-9</pub-id><pub-id pub-id-type="pmid">27942807</pub-id></citation></ref>
<ref id="B47">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Mallott</surname> <given-names>E. K.</given-names></name> <name><surname>Malhi</surname> <given-names>R. S.</given-names></name> <name><surname>Amato</surname> <given-names>K. R.</given-names></name></person-group> (<year>2019</year>). <article-title>Assessing the comparability of different dna extraction and amplification methods in gut microbial community profiling</article-title>. <source>Access Microbiol</source>. <volume>1</volume>:<fpage>e000060</fpage>. <pub-id pub-id-type="doi">10.1099/acmi.0.000060</pub-id><pub-id pub-id-type="pmid">32974545</pub-id></citation></ref>
<ref id="B48">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Mulugeta</surname> <given-names>L.</given-names></name> <name><surname>Drach</surname> <given-names>A.</given-names></name> <name><surname>Erdemir</surname> <given-names>A.</given-names></name> <name><surname>Hunt</surname> <given-names>C. A.</given-names></name> <name><surname>Horner</surname> <given-names>M.</given-names></name> <name><surname>Ku</surname> <given-names>J. P.</given-names></name> <etal/></person-group>. (<year>2018</year>). <article-title>Credibility, replicability, and reproducibility in simulation for biomedicine and clinical applications in neuroscience</article-title>. <source>Front. Neuroinform</source>. <volume>12</volume>:<fpage>18</fpage>. <pub-id pub-id-type="doi">10.3389/fninf.2018.00018</pub-id><pub-id pub-id-type="pmid">29713272</pub-id></citation></ref>
<ref id="B49">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Parida</surname> <given-names>S.</given-names></name> <name><surname>Bharadwaj</surname> <given-names>H.</given-names></name> <name><surname>Heinz</surname> <given-names>M. G.</given-names></name></person-group> (<year>2021</year>). <article-title>Spectrally specific temporal analyses of spike-train responses to complex sounds: A unifying framework</article-title>. <source>PLoS Comput. Biol</source>. <volume>17</volume>:<fpage>e1008155</fpage>. <pub-id pub-id-type="doi">10.1371/journal.pcbi.1008155</pub-id><pub-id pub-id-type="pmid">33617548</pub-id></citation></ref>
<ref id="B50">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Paton</surname> <given-names>J. J.</given-names></name> <name><surname>Buonomano</surname> <given-names>D. V.</given-names></name></person-group> (<year>2018</year>). <article-title>The neural basis of timing: Distributed mechanisms for diverse functions</article-title>. <source>Neuron</source> <volume>98</volume>, <fpage>687</fpage>&#x02013;<lpage>705</lpage>. <pub-id pub-id-type="doi">10.1016/j.neuron.2018.03.045</pub-id><pub-id pub-id-type="pmid">29772201</pub-id></citation></ref>
<ref id="B51">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Peterson</surname> <given-names>A. J.</given-names></name> <name><surname>Heil</surname> <given-names>P.</given-names></name></person-group> (<year>2019</year>). <article-title>Phase locking of auditory-nerve fibers reveals stereotyped distortions and an exponential transfer function with a level-dependent slope</article-title>. <source>J. Neurosci</source>. <volume>39</volume>, <fpage>4077</fpage>&#x02013;<lpage>4099</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.1801-18.2019</pub-id><pub-id pub-id-type="pmid">30867259</pub-id></citation></ref>
<ref id="B52">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Peterson</surname> <given-names>A. J.</given-names></name> <name><surname>Heil</surname> <given-names>P.</given-names></name></person-group> (<year>2020</year>). <article-title>Phase locking of auditory-nerve fibers: the role of lowpass filtering by hair cells</article-title>. <source>J. Neurosci</source>. <volume>40</volume>, <fpage>4700</fpage>&#x02013;<lpage>4714</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.2269-19.2020</pub-id><pub-id pub-id-type="pmid">32376778</pub-id></citation></ref>
<ref id="B53">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Poldrack</surname> <given-names>R.</given-names></name> <name><surname>Gorgolewski</surname> <given-names>K.</given-names></name></person-group> (<year>2014</year>). <article-title>Making big data open: data sharing in neuroimaging</article-title>. <source>Nat. Neurosci</source>. <volume>17</volume>, <fpage>1510</fpage>&#x02013;<lpage>1517</lpage>. <pub-id pub-id-type="doi">10.1038/nn.3818</pub-id><pub-id pub-id-type="pmid">25349916</pub-id></citation></ref>
<ref id="B54">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Recio-Spinoso</surname> <given-names>A..</given-names></name></person-group> (<year>2012</year>). <article-title>Enhancement and distortion in the temporal representation of sounds in the ventral cochlear nucleus of chinchillas and cats</article-title>. <source>PLoS ONE</source> <volume>7</volume>:<fpage>e44286</fpage>. <pub-id pub-id-type="doi">10.1371/journal.pone.0044286</pub-id><pub-id pub-id-type="pmid">23028514</pub-id></citation></ref>
<ref id="B55">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Rothman</surname> <given-names>J. S.</given-names></name> <name><surname>Young</surname> <given-names>E. D.</given-names></name> <name><surname>Manis</surname> <given-names>P. B.</given-names></name></person-group> (<year>1993</year>). <article-title>Convergence of auditory nerve fibers onto bushy cells in the ventral cochlear nucleus: implications of a computational model</article-title>. <source>J. Neurophysiol</source>. <volume>70</volume>, <fpage>2562</fpage>&#x02013;<lpage>2583</lpage>. <pub-id pub-id-type="doi">10.1152/jn.1993.70.6.2562</pub-id><pub-id pub-id-type="pmid">8120599</pub-id></citation></ref>
<ref id="B56">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Rucci</surname> <given-names>M.</given-names></name> <name><surname>Ahissar</surname> <given-names>E.</given-names></name> <name><surname>Burr</surname> <given-names>D.</given-names></name></person-group> (<year>2018</year>). <article-title>Temporal coding of visual space</article-title>. <source>Trends Cogn. Sci</source>. <volume>22</volume>, <fpage>883</fpage>&#x02013;<lpage>895</lpage>. <pub-id pub-id-type="doi">10.1016/j.tics.2018.07.009</pub-id><pub-id pub-id-type="pmid">30266148</pub-id></citation></ref>
<ref id="B57">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Rust</surname> <given-names>N. C.</given-names></name> <name><surname>Movshon</surname> <given-names>J. A.</given-names></name></person-group> (<year>2005</year>). <article-title>In praise of artifice</article-title>. <source>Nat. Neurosci</source>. <volume>8</volume>, <fpage>1647</fpage>&#x02013;<lpage>1650</lpage>. <pub-id pub-id-type="doi">10.1038/nn1606</pub-id><pub-id pub-id-type="pmid">16306892</pub-id></citation></ref>
<ref id="B58">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Saal</surname> <given-names>H. P.</given-names></name> <name><surname>Wang</surname> <given-names>X.</given-names></name> <name><surname>Bensmaia</surname> <given-names>S. J.</given-names></name></person-group> (<year>2016</year>). <article-title>Importance of spike timing in touch: an analogy with hearing?</article-title> <source>Curr. Opin Neurobiol</source>. <volume>40</volume>, <fpage>142</fpage>&#x02013;<lpage>149</lpage>. <pub-id pub-id-type="doi">10.1016/j.conb.2016.07.013</pub-id><pub-id pub-id-type="pmid">27504741</pub-id></citation></ref>
<ref id="B59">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Shackleton</surname> <given-names>T. M.</given-names></name> <name><surname>Liu</surname> <given-names>L.</given-names></name> <name><surname>Palmer</surname> <given-names>A. R.</given-names></name></person-group> (<year>2009</year>). <article-title>Responses to diotic, dichotic, and alternating phase harmonic stimuli in the inferior colliculus of guinea pigs</article-title>. <source>J. Assoc. Res. Otolaryngol</source>. <volume>10</volume>, <fpage>76</fpage>&#x02013;<lpage>90</lpage>. <pub-id pub-id-type="doi">10.1007/s10162-008-0149-4</pub-id><pub-id pub-id-type="pmid">19089495</pub-id></citation></ref>
<ref id="B60">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Siebert</surname> <given-names>W. M..</given-names></name></person-group> (<year>1970</year>). <article-title>Frequency discrimination in the auditory system: place or periodicity mechanisms?</article-title> <source>Proc. IEEE</source> <volume>58</volume>, <fpage>723</fpage>&#x02013;<lpage>730</lpage>. <pub-id pub-id-type="doi">10.1109/PROC.1970.7727</pub-id><pub-id pub-id-type="pmid">27295638</pub-id></citation></ref>
<ref id="B61">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Sober</surname> <given-names>S. J.</given-names></name> <name><surname>Sponberg</surname> <given-names>S.</given-names></name> <name><surname>Nemenman</surname> <given-names>I.</given-names></name> <name><surname>Ting</surname> <given-names>L. H.</given-names></name></person-group> (<year>2018</year>). <article-title>Millisecond spike timing codes for motor control</article-title>. <source>Trends Neurosci</source>. <volume>41</volume>, <fpage>644</fpage>&#x02013;<lpage>648</lpage>. <pub-id pub-id-type="doi">10.1016/j.tins.2018.08.010</pub-id><pub-id pub-id-type="pmid">30274598</pub-id></citation></ref>
<ref id="B62">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Steinberg</surname> <given-names>L. J.</given-names></name> <name><surname>Pe&#x000F1;a</surname> <given-names>J. L.</given-names></name></person-group> (<year>2011</year>). <article-title>Difference in response reliability predicted by spectrotemporal tuning in the cochlear nuclei of barn owls</article-title>. <source>J. Neurosci</source>. <volume>31</volume>, <fpage>3234</fpage>&#x02013;<lpage>3242</lpage>. <pub-id pub-id-type="doi">10.1523/JNEUROSCI.5422-10.2011</pub-id><pub-id pub-id-type="pmid">21368035</pub-id></citation></ref>
<ref id="B63">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Street</surname> <given-names>S. E.</given-names></name> <name><surname>Manis</surname> <given-names>P. B.</given-names></name></person-group> (<year>2007</year>). <article-title>Action potential timing precision in dorsal cochlear nucleus pyramidal cells</article-title>. <source>J. Neurophysiol</source>. <volume>97</volume>, <fpage>4162</fpage>&#x02013;<lpage>4172</lpage>. <pub-id pub-id-type="doi">10.1152/jn.00469.2006</pub-id><pub-id pub-id-type="pmid">17442767</pub-id></citation></ref>
<ref id="B64">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Tratwal</surname> <given-names>J.</given-names></name> <name><surname>Labella</surname> <given-names>R.</given-names></name> <name><surname>Bravenboer</surname> <given-names>N.</given-names></name> <name><surname>Kerckhofs</surname> <given-names>G.</given-names></name> <name><surname>Douni</surname> <given-names>E.</given-names></name> <name><surname>Scheller</surname> <given-names>E. L.</given-names></name> <etal/></person-group>. (<year>2020</year>). <article-title>Reporting guidelines, review of methodological standards, and challenges toward harmonization in bone marrow adiposity research. Report of the methodologies working group of the international bone marrow adiposity society</article-title>. <source>Front. Endocrinol</source>. <volume>11</volume>:<fpage>65</fpage>. <pub-id pub-id-type="doi">10.3389/fendo.2020.00065</pub-id><pub-id pub-id-type="pmid">32180758</pub-id></citation></ref>
<ref id="B65">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Umbach</surname> <given-names>D.</given-names></name> <name><surname>Jammalamadaka</surname> <given-names>S. R.</given-names></name></person-group> (<year>2009</year>). <article-title>Building asymmetry into circular distributions</article-title>. <source>Stat. Probab. Lett</source>. <volume>79</volume>, <fpage>659</fpage>&#x02013;<lpage>663</lpage>. <pub-id pub-id-type="doi">10.1016/j.spl.2008.10.022</pub-id></citation>
</ref>
<ref id="B66">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>van Hemmen</surname> <given-names>J. L..</given-names></name></person-group> (<year>2013</year>). <article-title>Vector strength after Goldberg, Brown, and von Mises: biological and mathematical perspectives</article-title>. <source>Biol. Cybern</source>. <volume>107</volume>, <fpage>385</fpage>&#x02013;<lpage>396</lpage>. <pub-id pub-id-type="doi">10.1007/s00422-013-0561-7</pub-id><pub-id pub-id-type="pmid">23982848</pub-id></citation></ref>
<ref id="B67">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>van Hemmen</surname> <given-names>J. L.</given-names></name> <name><surname>Vollmayr</surname> <given-names>A. N.</given-names></name></person-group> (<year>2013</year>). <article-title>Resonating vector strength: what happens when we vary the &#x0201C;probing&#x0201D; frequency while keeping the spike times fixed</article-title>. <source>Biol. Cybern</source>. <volume>107</volume>, <fpage>491</fpage>&#x02013;<lpage>494</lpage>. <pub-id pub-id-type="doi">10.1007/s00422-013-0560-8</pub-id><pub-id pub-id-type="pmid">23982849</pub-id></citation></ref>
<ref id="B68">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Vogt</surname> <given-names>L..</given-names></name></person-group> (<year>2009</year>). <article-title>The future role of bio-ontologies for developing a general data standard in biology: chance and challenge for zoo-morphology</article-title>. <source>Zoomorphology</source> <volume>128</volume>, <fpage>201</fpage>&#x02013;<lpage>217</lpage>. <pub-id pub-id-type="doi">10.1007/s00435-008-0081-5</pub-id></citation>
</ref>
<ref id="B69">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Wei</surname> <given-names>L.</given-names></name> <name><surname>Karino</surname> <given-names>S.</given-names></name> <name><surname>Verschooten</surname> <given-names>E.</given-names></name> <name><surname>Joris</surname> <given-names>P. X.</given-names></name></person-group> (<year>2017</year>). <article-title>Enhancement of phase-locking in rodents. I. An axonal recording study in gerbil</article-title>. <source>J. Neurophysiol</source>. <volume>118</volume>, <fpage>2009</fpage>&#x02013;<lpage>2023</lpage>. <pub-id pub-id-type="doi">10.1152/jn.00194.2016</pub-id><pub-id pub-id-type="pmid">28701535</pub-id></citation></ref>
<ref id="B70">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Yin</surname> <given-names>T.</given-names></name> <name><surname>Smith</surname> <given-names>P.</given-names></name> <name><surname>Joris</surname> <given-names>P. X.</given-names></name></person-group> (<year>2019</year>). <article-title>Neural mechanisms of binaural processing in the auditory brainstem</article-title>. <source>Compr. Physiol</source>. <volume>9</volume>, <fpage>1503</fpage>&#x02013;<lpage>1575</lpage>. <pub-id pub-id-type="doi">10.1002/cphy.c180036</pub-id><pub-id pub-id-type="pmid">31688966</pub-id></citation></ref>
<ref id="B71">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Zehl</surname> <given-names>L.</given-names></name> <name><surname>Jaillet</surname> <given-names>F.</given-names></name> <name><surname>Stoewer</surname> <given-names>A.</given-names></name> <name><surname>Grewe</surname> <given-names>J.</given-names></name> <name><surname>Sobolev</surname> <given-names>A.</given-names></name> <name><surname>Wachtler</surname> <given-names>T.</given-names></name> <etal/></person-group>. (<year>2016</year>). <article-title>Handling metadata in a neurophysiology laboratory</article-title>. <source>Front. Neuroinform</source>. <volume>10</volume>:<fpage>26</fpage>. <pub-id pub-id-type="doi">10.3389/fninf.2016.00026</pub-id><pub-id pub-id-type="pmid">27486397</pub-id></citation></ref>
<ref id="B72">
<citation citation-type="journal"><person-group person-group-type="author"><name><surname>Zheng</surname> <given-names>Y.</given-names></name> <name><surname>Escab&#x000ED;</surname> <given-names>M. A.</given-names></name></person-group> (<year>2013</year>). <article-title>Proportional spike-timing precision and firing reliability underlie efficient temporal processing of periodicity and envelope shape cues</article-title>. <source>J. Neurophysiol</source>. <volume>110</volume>, <fpage>587</fpage>&#x02013;<lpage>606</lpage>. <pub-id pub-id-type="doi">10.1152/jn.01080.2010</pub-id><pub-id pub-id-type="pmid">23636724</pub-id></citation></ref>
</ref-list> 
</back>
</article> 