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<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Physiol.</journal-id>
<journal-title>Frontiers in Physiology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Physiol.</abbrev-journal-title>
<issn pub-type="epub">1664-042X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
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<article-meta>
<article-id pub-id-type="publisher-id">1474568</article-id>
<article-id pub-id-type="doi">10.3389/fphys.2024.1474568</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physiology</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Left atrial spatial entropy: a novel tool for electrophysiological substrate characterization in atrial fibrillation</article-title>
<alt-title alt-title-type="left-running-head">Gigli et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fphys.2024.1474568">10.3389/fphys.2024.1474568</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Gigli</surname>
<given-names>Lorenzo</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
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<contrib contrib-type="author" corresp="yes">
<name>
<surname>Preda</surname>
<given-names>Alberto</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
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<contrib contrib-type="author">
<name>
<surname>Coluzzi</surname>
<given-names>Davide</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
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</contrib>
<contrib contrib-type="author">
<name>
<surname>Sartore</surname>
<given-names>Marta</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
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<contrib contrib-type="author">
<name>
<surname>Vila</surname>
<given-names>Muhamed</given-names>
</name>
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<sup>3</sup>
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<contrib contrib-type="author">
<name>
<surname>Carbonaro</surname>
<given-names>Marco</given-names>
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<sup>1</sup>
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<contrib contrib-type="author">
<name>
<surname>Baroni</surname>
<given-names>Matteo</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
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<contrib contrib-type="author">
<name>
<surname>Varrenti</surname>
<given-names>Marisa</given-names>
</name>
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<sup>1</sup>
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<contrib contrib-type="author">
<name>
<surname>Vargiu</surname>
<given-names>Sara</given-names>
</name>
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<sup>1</sup>
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<contrib contrib-type="author">
<name>
<surname>Guarracini</surname>
<given-names>Fabrizio</given-names>
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<sup>1</sup>
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<contrib contrib-type="author">
<name>
<surname>Frontera</surname>
<given-names>Antonio</given-names>
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<sup>1</sup>
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<contrib contrib-type="author">
<name>
<surname>Pannone</surname>
<given-names>Luigi</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
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<contrib contrib-type="author">
<name>
<surname>Chierchia</surname>
<given-names>Gian Battista</given-names>
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<sup>2</sup>
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<contrib contrib-type="author">
<name>
<surname>De Asmundis</surname>
<given-names>Carlo</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
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<contrib contrib-type="author">
<name>
<surname>Mazzone</surname>
<given-names>Patrizio</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
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<contrib contrib-type="author">
<name>
<surname>Sassi</surname>
<given-names>Roberto</given-names>
</name>
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<sup>3</sup>
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<aff id="aff1">
<sup>1</sup>
<institution>De Gasperis Cardio Center</institution>, <institution>Electrophysiology Unit</institution>, <institution>Niguarda Hospital</institution>, <addr-line>Milan</addr-line>, <country>Italy</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Heart Rhythm Management Centre</institution>, <institution>Postgraduate Program in Cardiac Electrophysiology and Pacing</institution>, <institution>Universitair Ziekenhuis Brussel &#x2013; Vrije Universiteit Brussel</institution>, <addr-line>Brussels</addr-line>, <country>Belgium</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Department of Computer Science</institution>, <institution>University of Milan</institution>, <addr-line>Milan</addr-line>, <country>Italy</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/9466/overview">Lukas R. C. Dekker</ext-link>, Catharina Hospital, Netherlands</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/282710/overview">Marianna Meo</ext-link>, Boston Scientific, Netherlands</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/2020925/overview">Sridharan Rajamani</ext-link>, Janssen Pharmaceutical Companies of Johnson and Johnson, United States</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Alberto Preda, <email>alberto.preda@ospedaleniguarda.it</email>
</corresp>
</author-notes>
<pub-date pub-type="epub">
<day>27</day>
<month>11</month>
<year>2024</year>
</pub-date>
<pub-date pub-type="collection">
<year>2024</year>
</pub-date>
<volume>15</volume>
<elocation-id>1474568</elocation-id>
<history>
<date date-type="received">
<day>01</day>
<month>08</month>
<year>2024</year>
</date>
<date date-type="accepted">
<day>31</day>
<month>10</month>
<year>2024</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2024 Gigli, Preda, Coluzzi, Sartore, Vila, Carbonaro, Baroni, Varrenti, Vargiu, Guarracini, Frontera, Pannone, Chierchia, De Asmundis, Mazzone and Sassi.</copyright-statement>
<copyright-year>2024</copyright-year>
<copyright-holder>Gigli, Preda, Coluzzi, Sartore, Vila, Carbonaro, Baroni, Varrenti, Vargiu, Guarracini, Frontera, Pannone, Chierchia, De Asmundis, Mazzone and Sassi</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>
<sec>
<title>Background</title>
<p>Electrical remodeling has been linked to the progression and recurrence of atrial fibrillation (AF) after catheter ablation (CA). Substrate mapping based solely on a voltage amplitude electrogram (EGM) does not provide a comprehensive understanding of the left atrial (LA) disease. The aim of this study is to assess left atrial spatial entropy (LASE) from voltage maps routinely obtained during AF ablation to further characterize the LA substrate.</p>
</sec>
<sec>
<title>Materials and Methods</title>
<p>High-density electroanatomic maps (EAMs) of 27 patients with paroxysmal or persistent AF undergoing routine CA were prospectively collected. Computational post-processing was performed on the voltage maps. Using the Shannon entropy model, the probability distribution of the amplitude range values associated with each point of the map was used to measure LASE. Finally, correlations between LASE and clinical and electrophysiological characteristics of AF were explored.</p>
</sec>
<sec>
<title>Results</title>
<p>LASE differentiated between patients with paroxysmal and persistent AF (6.45 &#xb1; 0.41 vs. 5.87 &#xb1; 0.53; <italic>p</italic> &#x3d; 0.028) and patients with normal and abnormal LA substrate (6.42 &#xb1; 0.42 vs. 5.87 &#xb1; 0.56; <italic>p</italic> &#x3d; 0.043), independent of the basal rhythm during EM acquisition (6.33 &#xb1; 0.41 vs. 6.11 &#xb1; 0.63; <italic>p</italic> &#x3d; 0.619). Accordance between LASE and EAMs was assessed by ROC analysis (AUC: 0.81; C.I.: 0.62&#x2013;0.99; Youden index: 6.06; sensitivity: 80%; and specificity: 80%). Patients with the lowest LASE reported AF recurrence at the follow-up.</p>
</sec>
<sec>
<title>Conclusion</title>
<p>LASE may play a role in the further characterization of the LA substrate and the type of AF, independent of basal rhythm.</p>
</sec>
</abstract>
<abstract abstract-type="graphical">
<title>Graphical Abstract</title>
<p>
<graphic xlink:href="FPHYS_fphys-2024-1474568_wc_abs.tif" position="anchor"/>
</p>
</abstract>
<kwd-group>
<kwd>atrial fibrillation</kwd>
<kwd>left atrial spatial entropy</kwd>
<kwd>catheter ablation</kwd>
<kwd>substrate characterization</kwd>
<kwd>mapping technologies</kwd>
</kwd-group>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Cardiac Electrophysiology</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Atrial fibrillation (AF) is the most common arrhythmia worldwide, associated with increased morbidity and mortality (<xref ref-type="bibr" rid="B5">Chugh et al., 2014</xref>). Sinus rhythm (SR) maintenance is the main target of AF treatment, and catheter ablation (CA) is currently the gold standard used to prevent arrhythmia recurrence (<xref ref-type="bibr" rid="B1">Arbelo et al., 2014</xref>). Continuous technological advances in the characterization of anatomical and electrical substrates, as well as in ablation methods, have allowed us to better understand AF mechanisms and improve outcomes (<xref ref-type="bibr" rid="B24">Parameswaran et al., 2021</xref>). However, the prediction of further events after CA is still a matter of debate (<xref ref-type="bibr" rid="B2">Berruezo et al., 2007</xref>; <xref ref-type="bibr" rid="B15">Li et al., 2023</xref>; <xref ref-type="bibr" rid="B17">Marcon et al., 2023</xref>). During bipolar mapping, the identification of low-voltage areas (LVAs) using universally accepted thresholds is considered proof of cardiomyocyte disease and left atrial (LA) fibrosis (<xref ref-type="bibr" rid="B29">Rodr&#xed;guez-Ma&#xf1;ero et al., 2018</xref>), which is associated with the advanced stage of AF and, consequently, a higher risk of recurrence (<xref ref-type="bibr" rid="B37">Vlachos et al., 2017</xref>). However, voltage mapping, based on electrogram (EGM) acquisition, has some well-known limitations, mainly due to the variability in signal morphology according to the wavefront direction with respect to the electrode position (<xref ref-type="bibr" rid="B6">de Bakker, 2019</xref>), electrode length, interelectrode spacing, and tissue contact (<xref ref-type="bibr" rid="B39">Yamaguchi et al., 2019</xref>). Finally, the heart rhythm highly influences EGM acquisition and, thus, its interpretation (<xref ref-type="bibr" rid="B12">Jadidi et al., 2016</xref>).</p>
<p>Entropy was introduced in thermodynamics as a measure of randomness and &#x201c;disorder&#x201d; in a molecular system. Its application has since expanded across numerous scientific domains, including information theory, data mining, and mathematical linguistics (<xref ref-type="bibr" rid="B33">Shaw and Charles, 1983</xref>). In the medical field, entropy was largely used to evaluate the state of consciousness (<xref ref-type="bibr" rid="B18">Mateos et al., 2018</xref>) and analyze the homogeneity of the heart tissue and its relationship with cardiac events (<xref ref-type="bibr" rid="B38">Wu and Chrispin, 2022</xref>).</p>
<p>In particular, the measurement of entropy from a distribution of signals (called &#x201c;Shannon entropy&#x201d;) and its links to the probability theory, as described in the information theory, was applied to cardiac electrophysiology to differentiate complex fractionated atrial electrograms (CFAEs) in patients with AF from background noise (<xref ref-type="bibr" rid="B22">Ng et al., 2010</xref>) and distinguish bipolar EGMs recorded at pivot points of rotors from EGMs detected in peripheral regions (<xref ref-type="bibr" rid="B8">Ganesan et al., 2013</xref>). <xref ref-type="bibr" rid="B11">Hwang et al. (2016)</xref> highlighted the potential use of Shannon entropy to evaluate the nature of rotors in 2D and 3D <italic>in silico</italic> models of persistent AF. To date, despite its potential relevance in this field, no studies have applied and evaluated entropy directly computed from EGM-based voltage maps across diverse cohorts of AF patients.</p>
<p>The aim of this study is thus to quantify left atrial spatial entropy (LASE) for further characterizing LA tissue in paroxysmal AF (paAF) and persistent AF (peAF) patients. We applied the Shannon entropy model to process a whole mass of data from voltage maps routinely collected during AF ablation.</p>
</sec>
<sec sec-type="materials|methods" id="s2">
<title>2 Materials and methods</title>
<sec id="s2-1">
<title>2.1 Study design</title>
<p>The data from 27 consecutive patients with either paAF or peAF admitted to the electrophysiology unit of Niguarda Hospital, Milan, Italy, in January 2022, who underwent CA of AF, were prospectively collected and analyzed. The study was conducted in collaboration with the department of Computer Science of the University of Milan, Italy. Inclusion criteria were as follows: patients aged &#x3e;18 years with paAF or peAF who had a first indication for AF ablation. Exclusion criteria were as follows: the presence of LA appendage thrombus at pre-operatory imaging, previous ablations of any type, and the need for additional ablations (i.e., cavotricuspid isthmus isolation). Baseline clinical characteristics were recorded through digital medical reports. Electroanatomic maps of LA were obtained using the CARTO 3 electroanatomic mapping system (Biosense Webster, Diamond Bar, CA, United States). For each patient undergoing AF ablation, a bipolar, high-density map of the LA was obtained. The resulting data, comprising the spatial position of the catheters, electrical signals, and vertices and triangles of the LA mesh, were extracted, exported, and analyzed offline. After discharge, patients were followed up with 24-hour Holter monitoring and clinical examinations performed at 3, 6, and 12 months. The primary endpoint was to compare the LASE with the AF-type and LA electroanatomical map (EAM).</p>
<p>The study was approved by the Ethics Committee of Niguarda Hospital in compliance with the Declaration of Helsinki. All patients provided informed consent before the procedure.</p>
</sec>
<sec id="s2-2">
<title>2.2 Mapping and ablation procedure</title>
<p>All procedures were performed under general anesthesia by an electrophysiologist experienced in AF ablation, assisted by at least one additional electrophysiologist or fellow. The whole CA methodology has been previously described in the work by <xref ref-type="bibr" rid="B25">Pratola et al. (2008)</xref>. A deflectable decapolar catheter (Bard Dynamic) (Boston Scientific, Marlborough, MA, United States) was positioned in the coronary sinus. A single trans-septal puncture was performed with the standard electrophysiological approach. After a trans-septal puncture, intravenous heparin was administered to maintain an activated clotting time of &#x3e;300 s. Real-time 3D LA maps were reconstructed using the PentaRay mapping catheter (Biosense Webster, Diamond Bar, CA, United States) with a minimum of 2,000 anatomical points acquired. The maps were acquired independently in the presence of SR or AF, and the normal LA substrate was distinguished from the abnormal LA substrate according to universally accepted voltage thresholds, setting low and high band pass thresholds at &#x3c;0.05 mV and &#x3e;0.5 mV, respectively (<xref ref-type="bibr" rid="B37">Vlachos et al., 2017</xref>). In particular, the LVA was defined by &#x2265; 5 adjacent points of &#x3c;0.5 mV acquired during SR and using a multipolar HD catheter. The accuracy of point acquisition was evaluated through the Tissue Proximity Index (TPI) algorithm using the CARTO 3 system to limit low-contact artifacts. Furthermore, multiple local remaps with a minimum density of &#x2265;10 points were performed to reduce wavefront direction distortion. The entire mapped LA was generally as defined abnormal by &#x3e;1 LVAs adjacent or localized in different LA regions. In addition, to reduce the acquisition of false positive LVAs due to inadequate contact with the wall, all EAMs were acquired using the activated Tissue Proximity Indicator (TPI) tool of PentaRay. Anatomic reconstruction of the LA, including the LA&#x2013;pulmonary vein (PV) junction, was performed. In all patients, radiofrequency (RF) ablation was performed to create a single circumferential line around contiguous veins. RF pulses were delivered with a temperature setting of up to 43&#xb0;C and 35 W using the THERMOCOOL SMARTTOUCH SF Catheter (Biosense Webster, Diamond Bar, CA, United States) targeting an ablation index (AI) of 500 for both the anterior wall and roof and 400 for the posterior wall and floor of LA. The ablation lines consisted of contiguous local lesions &#x3c;5 mm from each other and at a distance of &#x3e;5 mm from the ostia of the PVs using the wide antral circumferential ablation technique (<xref ref-type="bibr" rid="B26">Proietti et al., 2014</xref>). In cases of LVAs on the LA posterior wall, posterior box isolation was performed (<xref ref-type="bibr" rid="B30">Romero et al., 2023</xref>). Procedural success was defined according to universally accepted criteria for pulmonary vein isolation (PVI) and LA posterior war isolation by checking entrance and exit blocks (<xref ref-type="bibr" rid="B36">Tzeis et al., 2024</xref>).</p>
</sec>
<sec id="s2-3">
<title>2.3 Data acquisition and processing</title>
<p>During LA mapping, bipolar signals were routinely acquired for 2.5 s and stored along with the 3D location of the mapping catheter at the time of recording. The set of locations visited by the mapping electrodes (mean &#x3d; 13,000 &#xb1; 4,242) was presented as a cloud of points in space. An atrial mesh was also derived using signals &#x3c;3.5 mV of amplitude, which was considered the noise threshold (more details on its creation are given in <xref ref-type="sec" rid="s2-3-1">Section 2.3.1</xref>). The main steps of data acquisition and processing are summarized in green and blue boxes in <xref ref-type="fig" rid="F1">Figure 1</xref>, respectively.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Workflow of data acquisition and processing. The green box (top) represents the data acquisition. For each patient, a cloud of points representing the 3D locations of the EGM signals was collected. An atrial mesh was computed and processed by several steps to associate points and signals with the vertices, as represented in the blue box (bottom). <bold>(A)</bold> The normal of the vertex was outlined and represented. <bold>(B)</bold> The sphere with center in the vertex was used to exclude the farthest points. <bold>(C,D)</bold> The additional criterion based on the distance between the vertex and the points was represented to obtain the neighboring area (a cylinder), outlined in <bold>(E). (F)</bold> Red points ideally represent the vertices of the mesh, the triangles represent the locations of the acquired EGM signals, and the resulting associated points are depicted by green triangles. From these, the average peak-to-peak (PP) of the EGMs was computed as shown in <bold>(G)</bold>, obtaining a voltage map of the mesh on which the Shannon entropy was computed <bold>(H)</bold>.</p>
</caption>
<graphic xlink:href="fphys-15-1474568-g001.tif"/>
</fig>
<sec id="s2-3-1">
<title>2.3.1 Mesh creation and downsampling</title>
<p>The resolution of LA mesh obtained by CARTO 3 varied among patients, and depending on the number of vertices and triangles acquired during mapping. In order to compare results among different patients, the mesh was downsampled, setting a value of 5,000 vertices per patient with a tolerance of &#xb1; 100 vertices. In those cases with the number of vertices lower than 5,000, upsampling was performed. The resampling process was carried out through the open-source software &#x201c;Meshtool&#x201d; (<xref ref-type="bibr" rid="B21">Neic et al., 2020</xref>). This tool reduces mesh resolution by initially collapsing all edges smaller than a specified minimum value. Subsequently, it divides edges larger than the maximum edge length. The triangles are defined according to the Delaunay triangulation.</p>
</sec>
<sec id="s2-3-2">
<title>2.3.2 Voltage map determination</title>
<p>After mesh homogenization, a surrogate of entropy measure was derived from each EGM associated with the vertex of the mesh. To accomplish this objective, (I) the vector corresponding to the normal of the mesh at each vertex (outward direction aligned with the mesh&#x2019;s conformation and passing through the vertex) was determined (<xref ref-type="fig" rid="F1">Figure 1A</xref>); (II) a sphere with the center located at the vertex was drawn, and only EGMs collected at positions inside the sphere were considered &#x201c;candidates&#x201d; associated with the vertex (<xref ref-type="fig" rid="F1">Figure 1B</xref>); (III) the radius of the sphere was chosen empirically (8 mm) to encompass positions that, due to atrial movements, fell either below or above the vertex along the normal; and (IV) among the candidate EGMs, only those within a predefined distance from the normal were selected (<xref ref-type="fig" rid="F1">Figure 1C</xref>). This further criterion was conceived to consider possible movements of the atria and account for deformations of the atrial wall during the electrophysiological procedure. From this concept, a cylinder was created by the summation of neighboring points, with its axis normal to the internal surface of the mesh and a radius of 2 mm (empirically determined considering the average distance between vertices) (<xref ref-type="fig" rid="F1">Figure 1D</xref>).</p>
<p>Upon the completion of the neighboring points&#x2019; identification phase, it was possible to define a set of vertices <inline-formula id="inf1">
<mml:math id="m1">
<mml:mrow>
<mml:mi mathvariant="script">V</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mfenced open="{" close="}" separators="|">
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mo>&#x2026;</mml:mo>
<mml:mo>,</mml:mo>
<mml:mi>v</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula>, which were those of the mesh, associated with a set of neighbors <inline-formula id="inf2">
<mml:math id="m2">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="script">N</mml:mi>
<mml:mi>v</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mfenced open="{" close="}" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>:</mml:mo>
<mml:mi>n</mml:mi>
<mml:mtext>&#x2009;neighbor&#x2009;of&#x2009;</mml:mtext>
<mml:mi>v</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mtext>&#x2002;</mml:mtext>
<mml:mi>v</mml:mi>
<mml:mo>&#x2208;</mml:mo>
<mml:mi mathvariant="script">V</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>. Hence, the neighboring points related to a vertex <inline-formula id="inf3">
<mml:math id="m3">
<mml:mrow>
<mml:mi>v</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> were defined as those within the sphere and having a distance from the normal vector that was less than the average distance between vertices (2 mm). This set of points <inline-formula id="inf4">
<mml:math id="m4">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="script">N</mml:mi>
<mml:mi>v</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> had cardinality <inline-formula id="inf5">
<mml:math id="m5">
<mml:mrow>
<mml:msub>
<mml:mi>N</mml:mi>
<mml:mi>v</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mo>&#x23;</mml:mo>
<mml:msub>
<mml:mi mathvariant="script">N</mml:mi>
<mml:mi>v</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (indicated by the same colors in <xref ref-type="fig" rid="F1">Figure 1</xref>, panel e, and green triangles in <xref ref-type="fig" rid="F1">Figure 1F</xref>).</p>
<p>For each vertex <inline-formula id="inf6">
<mml:math id="m6">
<mml:mrow>
<mml:mi>v</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> of the mesh, the range of voltage amplitudes (through the peak-to-peak amplitude formulation <inline-formula id="inf7">
<mml:math id="m7">
<mml:mrow>
<mml:mi mathvariant="italic">max</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>x</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mi mathvariant="italic">min</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>x</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula>) was computed on the EGMs acquired at each selected neighboring point, where <italic>x</italic>
<sub>
<italic>n</italic>
</sub> represents the <italic>n</italic>th 2.5-s EGM associated with the <italic>n</italic> point. The average of the amplitude range of all neighbors, i.e., <inline-formula id="inf8">
<mml:math id="m8">
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>N</mml:mi>
<mml:mi>v</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:msub>
<mml:mi>N</mml:mi>
<mml:mi>v</mml:mi>
</mml:msub>
</mml:munderover>
</mml:mstyle>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi mathvariant="italic">max</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>x</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mi mathvariant="italic">min</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>x</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula>, was then taken as the voltage range in <inline-formula id="inf9">
<mml:math id="m9">
<mml:mrow>
<mml:mi>v</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> and used to determine the voltage map (<xref ref-type="fig" rid="F1">Figure 1G</xref>).</p>
</sec>
<sec id="s2-3-3">
<title>2.3.3 Entropy computation</title>
<p>Discrete entropy <inline-formula id="inf10">
<mml:math id="m10">
<mml:mrow>
<mml:mi>H</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> was computed from the probability distribution of the amplitude range values associated with each vertex of the mesh, represented by histograms (<xref ref-type="fig" rid="F1">Figure 1H</xref>). The resulting formulation expressed as a sum over all bins of the histogram was<disp-formula id="equ1">
<mml:math id="m11">
<mml:mrow>
<mml:mi>H</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mi>I</mml:mi>
</mml:munderover>
</mml:mstyle>
<mml:mrow>
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#x2061;</mml:mo>
<mml:mi mathvariant="italic">log</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mi>w</mml:mi>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>where <inline-formula id="inf11">
<mml:math id="m12">
<mml:mrow>
<mml:mi>w</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> was the width of each bin (100 a.u. corresponding to 0.3 mv, with a conversion factor of 0.003 mV/a. u.) and <inline-formula id="inf12">
<mml:math id="m13">
<mml:mrow>
<mml:mi mathvariant="script">I</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mrow>
<mml:mfenced open="{" close="}" separators="|">
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>,</mml:mo>
<mml:mo>&#x2026;</mml:mo>
<mml:mo>,</mml:mo>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> was the set comprising all bins of the histogram with cardinality <inline-formula id="inf13">
<mml:math id="m14">
<mml:mrow>
<mml:mi>I</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mo mathvariant="script">&#x23;</mml:mo>
<mml:mi mathvariant="script">I</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>. Summarizing the methodology, it was possible to define the probability of the <inline-formula id="inf14">
<mml:math id="m15">
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>th bin as follows (where <inline-formula id="inf15">
<mml:math id="m16">
<mml:mrow>
<mml:msub>
<mml:mi>w</mml:mi>
<mml:mn>0</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is a constant value):<disp-formula id="equ2">
<mml:math id="m17">
<mml:mrow>
<mml:msub>
<mml:mi>p</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mo>&#x23;</mml:mo>
<mml:mrow>
<mml:mfenced open="{" close="}" separators="|">
<mml:mrow>
<mml:mi>v</mml:mi>
<mml:mo>:</mml:mo>
<mml:msub>
<mml:mi>w</mml:mi>
<mml:mn>0</mml:mn>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>w</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x2264;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mi>N</mml:mi>
<mml:mi>v</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:munder>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>n</mml:mi>
<mml:mo>&#x2208;</mml:mo>
<mml:msub>
<mml:mi mathvariant="script">N</mml:mi>
<mml:mi>v</mml:mi>
</mml:msub>
</mml:mrow>
</mml:munder>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi mathvariant="italic">max</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>x</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mi mathvariant="italic">min</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msub>
<mml:mi>x</mml:mi>
<mml:mi>n</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mtext>&#x2002;</mml:mtext>
<mml:mo>&#x3c;</mml:mo>
<mml:mtext>&#x2009;</mml:mtext>
<mml:msub>
<mml:mi>w</mml:mi>
<mml:mn>0</mml:mn>
</mml:msub>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>w</mml:mi>
<mml:mi>i</mml:mi>
<mml:mo>,</mml:mo>
<mml:mi>v</mml:mi>
<mml:mo>&#x2208;</mml:mo>
<mml:mi mathvariant="script">V</mml:mi>
<mml:mtext>&#x2009;</mml:mtext>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x23;</mml:mo>
<mml:mi mathvariant="script">V</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>.</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
</p>
<p>The bin width <inline-formula id="inf16">
<mml:math id="m18">
<mml:mrow>
<mml:mi>w</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> &#x3d; 0.3 mV was selected to improve the capability to distinguish between scar tissue and noise. Voltage amplitude levels below 0.5 mV are widely recognized as indicative of significant fibrosis or scar tissue within the cardiac substrate. Notably, a very recent study identified 0.3 mV as the cutoff voltage that effectively enhanced the identification of scar tissue from the surrounding healthy myocardium (<xref ref-type="bibr" rid="B28">Roca-Luque et al., 2023</xref>).</p>
</sec>
</sec>
<sec id="s2-4">
<title>2.4 Statistical analysis</title>
<p>All quantitative variables displayed a normal distribution, which was verified empirically by the visual inspection of the histogram. They were reported as the mean &#xb1; standard deviation and compared using a one-tailed Student&#x2019;s t-test. <italic>p</italic> &#x3c; 0.05 was considered significant. To evaluate the degree of agreement or comparability between continuous variables of measurements obtained from the calculation of entropy on the first mesh and the downsampled mesh, a Bland&#x2013;Altman analysis was performed. Discrimination, i.e., the model&#x2019;s ability to differentiate between patients with abnormal and normal LA, was examined using the area under the receiver operating characteristic (AUROC) curve. AUROC analysis was also performed to calculate cutoff values, sensitivity, and specificity. Finally, the cutoff points were calculated by obtaining the best Youden index (sensitivity &#x2b; specificity &#x2212;1). All statistical analyses were performed by two blinded researchers, and then, the results were compared for reproducibility using k-statistics. Data were analyzed using R software version 3.6.2 (R Foundation for Statistical Computing, Vienna, Austria).</p>
</sec>
</sec>
<sec sec-type="results" id="s3">
<title>3 Results</title>
<sec id="s3-1">
<title>3.1 Study population and procedure characteristics</title>
<p>The main characteristics of the study population (mean age, 63 &#xb1; 14 years; 41% male) are summarized in <xref ref-type="table" rid="T1">Table 1</xref>. Overall, 16 patients (59%) suffered from paAF, while the remaining patients were affected by the persistent type. A normal LA substrate was reported in 15 patients with paAF (94%) and 2 patients with peAF (18%). The EAM was obtained during SR in 13 patients (48%), and the average number of collected EGMs per map was 3,029 &#xb1; 702 points. The mean skin-to-skin time was 56.3 &#xb1; 7.2 min, with a mean mapping time of 15.6 &#xb1; 3.4 min. Procedural success was achieved in all cases without procedural complications. After discharge, patients underwent follow-up for a mean time of 15 &#xb1; 2 months. At 1 year, two cases of AF recurrence were reported among peAF patients.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Characteristics of the study population.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th colspan="2" align="left">Clinical characteristic</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">No. of patients</td>
<td align="left">27</td>
</tr>
<tr>
<td align="left">Age</td>
<td align="left">63 &#xb1; 14</td>
</tr>
<tr>
<td align="left">Male sex</td>
<td align="left">11 (41%)</td>
</tr>
<tr>
<td align="left">Former smoking</td>
<td align="left">6 (22%)</td>
</tr>
<tr>
<td align="left">Paroxysmal AF</td>
<td align="left">16 (59%)</td>
</tr>
<tr>
<td align="left">Hypertension</td>
<td align="left">10 (37%)</td>
</tr>
<tr>
<td align="left">Dyslipidemia</td>
<td align="left">6 (22%)</td>
</tr>
<tr>
<td align="left">Diabetes mellitus</td>
<td align="left">3 (11%)</td>
</tr>
<tr>
<td align="left">AAD</td>
<td align="left">14 (52%)</td>
</tr>
<tr>
<td colspan="2" align="left">Procedural characteristics</td>
</tr>
<tr>
<td align="left">SR during mapping</td>
<td align="left">13 (48%)</td>
</tr>
<tr>
<td align="left">Normal LA substrate at voltage map</td>
<td align="left">17 (63%)</td>
</tr>
<tr>
<td align="left">LVA, cm<sup>2</sup> (mean, minimum, and maximum)<break/>&#x2003;Paroxysmal AF<break/>&#x2003;Persistent AF<break/>LVA/LA volume, %<break/>&#x2003;Paroxysmal AF<break/>&#x2003;Persistent AF</td>
<td align="left">
<break/>2 (0&#x2013;3)<break/>14 (8&#x2013;21)<break/>
<break/>&#x3c;2<break/>23 (16&#x2013;27)</td>
</tr>
<tr>
<td align="left">Skin-to-skin time, min</td>
<td align="left">62.3 &#xb1; 6.9</td>
</tr>
<tr>
<td align="left">Mapping time, min</td>
<td align="left">15.6 &#xb1; 3.4</td>
</tr>
<tr>
<td align="left">No. of acquired points</td>
<td align="left">2029 &#xb1; 602</td>
</tr>
<tr>
<td align="left">RF time, min</td>
<td align="left">31.3 &#xb1; 5.3</td>
</tr>
<tr>
<td align="left">AF recurrence during follow up (%)</td>
<td align="left">2 (7%)</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>AAD, antiarrhythmic drug; AF, atrial fibrillation; LA, left atrial; RF, radiofrequency; LVA, low-voltage area; SR, sinus rhythm.</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
<sec id="s3-2">
<title>3.2 LASE values</title>
<p>The mean entropy calculated from the original mesh was 5.87 &#xb1; 0.47. After mesh downsampling, the mean entropy was 6.27 &#xb1; 0.53. <xref ref-type="fig" rid="F2">Figure 2</xref> shows an example of the distribution of two patients with high and low entropy values, while the values computed for the entire dataset are given in <xref ref-type="table" rid="T2">Table 2</xref>. The Bland&#x2013;Altman analysis was performed to evaluate the degree of agreement between measurements obtained from the calculation of entropy on the first mesh and on the downsampled mesh (<xref ref-type="fig" rid="F3">Figure 3</xref>). The average of the differences was &#x2212;0.35, a bias value related to the calculation of the entropy in the original mesh. The measurements were, however, largely in agreement, with all but one case falling within the 95% confidence interval of the mean (between &#x2212;0.81 and 0.12) and most within a range &#xb1;0.2 with respect to the mean (23 cases out of 27). First, all samples and related histograms of entropy distribution were qualitatively examined. Statistical tests were carried out on the entropy values relating to the type of substrate, the type of AF, and the heart rhythm during the procedure. Entropy values significantly differed between patients with paAF and peAF (6.45 &#xb1; 0.41 <italic>versus</italic> 5.87 &#xb1; 0.53; <italic>p</italic> &#x3d; 0.028), as well as in patients with normal and abnormal LA substrates (6.42 &#xb1; 0.42 <italic>versus</italic> 5.87 &#xb1; 0.56; <italic>p</italic> &#x3d; 0.043). Finally, it is worth noting that the entropy values were independent of the presence of SR or AF during the procedure (6.33 &#xb1; 0.41 <italic>versus</italic> 6.11 &#xb1; 0.63; <italic>p</italic> &#x3d; 0.619). LASE and EGM distributions according to patients&#x2019; characteristics are given in <xref ref-type="fig" rid="F4">Figures 4</xref>, <xref ref-type="fig" rid="F5">5</xref>, respectively. Compared to LASE, the EGM boxplot analysis did not distinguish between paAF and peAF (<italic>p</italic> &#x3d; 0.053) or between normal and abnormal LA substrates (<italic>p</italic> &#x3d; 0.22). Moreover, the basal rhythm significantly influenced the EGM values (<italic>p</italic> &#x3d; &#x3c;0.001). The accordance between the LASE and abnormal substrate identified in the voltage map was confirmed using the ROC curve (AUC: 0.81; CI: 0.62&#x2013;0.99) (<xref ref-type="fig" rid="F6">Figure 6</xref>). The cutoff with the best accuracy, according to the Youden index, was estimated at 6.06, demonstrating a sensitivity of 80% and a specificity of 80%. All results were compared for reproducibility, with a k-statistic of 0.82.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Examples of voltage maps superimposed to their corresponding atrial mesh (right) and their distributions (left) for a patient with paAF <bold>(A)</bold> and peAF <bold>(B)</bold>.</p>
</caption>
<graphic xlink:href="fphys-15-1474568-g002.tif"/>
</fig>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Substrates, AF types, and derived LASE for each patient in the study.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="center">Patient ID</th>
<th align="center">Substrate</th>
<th align="center">AF type</th>
<th align="center">Basal rhythm</th>
<th align="center">Entropy from the original mesh</th>
<th align="center">LASE</th>
<th align="center">AF recurrence</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="center">1</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">6.206</td>
<td align="center">6.693</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">2</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">6.135</td>
<td align="center">6.543</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">3</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">5.804</td>
<td align="center">6.533</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">4</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">4.374</td>
<td align="center">4.885</td>
<td align="center">Yes</td>
</tr>
<tr>
<td align="center">5</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">AF</td>
<td align="center">5.892</td>
<td align="center">6.358</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">6</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">4.170</td>
<td align="center">4.532</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">7</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">AF</td>
<td align="center">6.319</td>
<td align="center">6.767</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">8</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">AF</td>
<td align="center">6.737</td>
<td align="center">6.998</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">9</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">5.557</td>
<td align="center">5.831</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">10</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">5.803</td>
<td align="center">5.940</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">11</td>
<td align="center">Normal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">5.509</td>
<td align="center">5.755</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">12</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">SR</td>
<td align="center">5.652</td>
<td align="center">5.988</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">13</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">5.448</td>
<td align="center">4.839</td>
<td align="center">Yes</td>
</tr>
<tr>
<td align="center">14</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">AF</td>
<td align="center">6.535</td>
<td align="center">6.767</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">15</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">6.556</td>
<td align="center">6.960</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">16</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">5.281</td>
<td align="center">5.707</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">17</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">5.872</td>
<td align="center">6.251</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">18</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">5.914</td>
<td align="center">6.380</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">19</td>
<td align="center">Normal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">5.101</td>
<td align="center">5.439</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">20</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">6.662</td>
<td align="center">7.167</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">21</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">6.216</td>
<td align="center">6.665</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">22</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">5.156</td>
<td align="center">5.432</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">23</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">6.625</td>
<td align="center">7.096</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">24</td>
<td align="center">Normal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">6.340</td>
<td align="center">6.594</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">25</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">5.354</td>
<td align="center">5.573</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">26</td>
<td align="center">Abnormal</td>
<td align="center">Paroxysmal</td>
<td align="center">SR</td>
<td align="center">5.228</td>
<td align="center">5.872</td>
<td align="center">No</td>
</tr>
<tr>
<td align="center">27</td>
<td align="center">Abnormal</td>
<td align="center">Persistent</td>
<td align="center">AF</td>
<td align="center">5.310</td>
<td align="center">5.500</td>
<td align="center">No</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Bland&#x2013;Altman plot of entropy values obtained from the original and downsampled meshes. The horizontal axis shows the average of the two entropy values and the vertical axis the difference between the two values.</p>
</caption>
<graphic xlink:href="fphys-15-1474568-g003.tif"/>
</fig>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Distributions of LASE according to patients&#x2019; characteristics.</p>
</caption>
<graphic xlink:href="fphys-15-1474568-g004.tif"/>
</fig>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Distributions of EGM according to patients&#x2019; characteristics.</p>
</caption>
<graphic xlink:href="fphys-15-1474568-g005.tif"/>
</fig>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>ROC curve to explore the diagnostic ability of LASE in identifying LA abnormal substrates.</p>
</caption>
<graphic xlink:href="fphys-15-1474568-g006.tif"/>
</fig>
<p>At follow-up, patients with AF recurrence were characterized by the lowest LASE.</p>
</sec>
</sec>
<sec sec-type="discussion" id="s4">
<title>4 Discussion</title>
<p>To the best of our knowledge, this is the first study using spatial entropy for further characterization of the whole LA electrical substrate in patients affected by AF, independent of common EGM thresholds of the bipolar map. The main findings of the study are as follows: (i) the LASE significantly differentiated paAF (higher LASE) from peAF (lower LASE), as well as the presence of normal (higher LASE) or abnormal (lower LASE) LA substrate; (ii) LASE was independent of the heart rhythm (SR vs. AF) during map acquisition; (iii) LASE was in accordance with the EAM map with a high sensibility and specificity.</p>
<sec id="s4-1">
<title>4.1 Models of entropy translated to AF</title>
<p>According to information theory (<xref ref-type="bibr" rid="B32">Shannon, 1948</xref>; <xref ref-type="bibr" rid="B19">Rivolta, 2024</xref>), entropy provides an estimate of the number of bits required to encode a random event. If the probability of a certain event is high, its informative content tends to 0. Therefore, if one event in the distribution is nearly certain to happen, only one bit is necessary. Conversely, if the probability of the event is low, the number of bits required for encoding it will be high (<xref ref-type="bibr" rid="B27">Ribeiro et al., 2021</xref>). Subsequently, the higher the probability of a group of events occurring with the same frequency, the higher the value of entropy. On the contrary, if the probability of the events occurring with the same frequency is low, entropy will be low.</p>
<p>Numerous studies used entropy to address multiple tasks related to physiological signals, including cardiac data recording (<xref ref-type="bibr" rid="B19">Rivolta, 2024</xref>; <xref ref-type="bibr" rid="B7">Ganesan et al., 2014</xref>; <xref ref-type="bibr" rid="B16">Manikandan and Soman, 2012</xref>). Applying this concept to the electrical activity of LA, if the range of atrial voltage amplitudes is uniform in every region, its entropy will be high. This occurs because the probability of encountering a specific voltage is similar across all locations explored during mapping. Conversely, if the electrical activity is not uniformly distributed due to the presence of fibrosis or LVAs, resulting in a skewed probability distribution, entropy will be lower.</p>
<p>In the context of the present study, the histogram pattern in panel A of <xref ref-type="fig" rid="F2">Figure 2</xref> (wider but more homogeneous distribution of probability) is representative (with statistical significance) of a typical profile for a normal substrate and paroxysmal AF, and it corresponds to the presence of similar amplitudes in different locations. Contrarily, panel B of <xref ref-type="fig" rid="F2">Figure 2</xref> is typical of an abnormal substrate, with different values of voltage across the atrial tissue. Intriguingly, the probability of voltage amplitude distribution seems independent of the rhythm present at the time of mapping. Therefore, it remains significantly higher in patients with normal substrate even if the data acquisition was performed during AF, which usually represents an important limitation for bipolar mapping. This is probably because the data acquisition of the explored area was based on a sample of voltage amplitude distribution and not only on the single voltage value recorded at a certain time. For this reason, LASE may overcome some well-known limitations of conventional bipolar mapping, such as arbitrary LVA thresholds, basal rhythm, and the direction of the wavefront relative to the orientation of the mapping catheter electrode (<xref ref-type="bibr" rid="B6">de Bakker, 2019</xref>; <xref ref-type="bibr" rid="B39">Yamaguchi et al., 2019</xref>).</p>
</sec>
<sec id="s4-2">
<title>4.2 LASE computation</title>
<p>As the variability observed in the original meshes across different patients may influence the comparability of the findings, we downsampled the mesh by reducing the vertex count, providing more uniformity. This reduction aimed to standardize the datasets for inter-patient comparison and provide faster computation and processing. This process did not lead to the loss of information, as confirmed by the results of the comparative analysis.</p>
<p>The criteria for selecting candidate EGMs considered their proximity to the normal to the inner surface of the LA. The aim was to address potential issues related to atrial movements and wall deformations during the electrophysiological procedure. This method added a valuable refinement layer based on the average distance between vertices.</p>
<p>The definition of LVA was historically arbitrarily defined, with large differences among studies (<xref ref-type="bibr" rid="B13">Junarta et al., 2022</xref>). Previously, LVAs were defined by at least three points of low voltage acquired using the ablation catheter, which is typically equipped with only two dipoles. This method has provided conflicting results regarding the long-term effectiveness of adding ablation of these regions to conventional PV ablation (<xref ref-type="bibr" rid="B40">Yang et al., 2022</xref>; <xref ref-type="bibr" rid="B14">Kircher et al., 2018</xref>). However, these studies confirmed the beneficial role of voltage maps in identifying patients with peAF and normal LA substrates, who may achieve excellent rhythm control with PV isolation alone. The proposed workflow enables the assessment of the SE across the entire atrium based on voltage maps. Alternative approaches based on localized evaluations within specific areas (e.g., left/right pulmonary veins) or leveraging surrogate data through bootstrapping techniques may offer a wider view of the entropy distribution and its variability.</p>
<p>The relevance of entropy within the electrophysiological framework supports its wider application, particularly in the field of AF, which is, by definition, the most chaotic rhythm (<xref ref-type="bibr" rid="B23">Nicolet et al., 2019</xref>). In addition, it may be interesting to explore other concepts of entropy applied to voltage maps, such as dispersion entropy (<xref ref-type="bibr" rid="B31">Rostaghi and Azami, 2016</xref>) and fuzzy entropy (<xref ref-type="bibr" rid="B4">Chen et al., 2007</xref>). In this regard, additional characteristics of the EGM signals different from voltage amplitude or SE of the time series may be analyzed.</p>
</sec>
<sec id="s4-3">
<title>4.3 Clinical implications</title>
<p>To date, several mapping tools have been developed to improve our understanding of AF, such as CFAE (<xref ref-type="bibr" rid="B10">Hunter et al., 2011</xref>) and CARTOFINDER (<xref ref-type="bibr" rid="B9">Honarbakhsh et al., 2018</xref>), which aim to detect high-rate focal or rotational activity. However, these tools have failed to improve long-term outcomes and are dependent on the presence of FA during mapping (<xref ref-type="bibr" rid="B20">Narayan and John, 2024</xref>). Recently, omnipolar and multipolar mapping techniques have been introduced to overcome the well-known limitations of bipolar mapping, providing optimistic results in substrate mapping and identifying gaps in the ablation lines around the pulmonary veins (<xref ref-type="bibr" rid="B3">Butcher et al., 2023</xref>). Finally, the most recent functional mapping method was proposed to analyze, during SR, the response to short-coupled atrial extrastimuli to identify areas of hidden slow conduction within the LA (<xref ref-type="bibr" rid="B34">Silva Garcia et al., 2023</xref>). In our study, we investigate the relationship between LASE and the clinical patterns of AF, as well as LASE and LA substrate. The clinical behavior of AF and the presence of LVAs in the voltage map are widely accepted surrogate markers of the degree of atrial structural and electrical remodeling and are associated with a worse outcome after ablation (<xref ref-type="bibr" rid="B35">Starek et al., 2023</xref>). However, these factors lack accuracy in predicting AF recurrence patient by patient. This is partially explained by the fact that AF is a complex arrhythmia without a full understanding of its underlying mechanisms. Therefore, performing CA with the EAM system is not only a therapeutic procedure but also a diagnostic opportunity, providing useful insights into the degree of the disease.</p>
<p>Since high-density substrate mapping of the LA encounters several limitations, LASE was used to increase its diagnostic accuracy. Previous studies used entropy to improve the diagnostic power of already existing tools designed to identify such functional electrical anomalies underlying arrhythmia sustainability (<xref ref-type="bibr" rid="B22">Ng et al., 2010</xref>). However, all these methods reported contrasting results in terms of effectiveness and capability, and their use is not yet suggested by the guidelines. Our research aimed to identify a novel indicator capable of working synergistically with the EAM system to provide useful information about the underlying AF mechanism and risk recurrence at follow-up. The LASE diagnostic potential was significant, reporting an AUC of 0.81 with 80% sensibility and specificity in predicting abnormal LA substrates. Of note, patients with early recurrence of AF at follow-up were characterized by very low LASE. This finding may be proof for further studies exploring the utility of this tool in predicting post-CA arrhythmia recurrences, compared to conventional parameters that are routinely considered.</p>
<p>Ultimately, LASE demonstrated to be both a feasible and reliable measure, capable of being calculated from a standard bipolar map at any given moment after retrospective exporting and processing. This might facilitate eventual comparative analysis of ablations within the same patient or across different patients. Consequently, this novel tool can be easily translated into the clinical setting of CA, assisting a tailored substrate-based strategy.</p>
</sec>
<sec id="s4-4">
<title>4.4 Study limitations</title>
<p>The small sample is a major limitation to the study, warranting the need for larger validation studies to confirm our findings. Since all EAMs were produced using the CARTO 3 system, LASE remains, at present, a tool developed for a single-mapping system and, therefore, influenced by all its inherent limitations, limiting its applicability to other mapping technologies. The accuracy and reliability of the results should be independent of the number and density of acquired points. In this study, we adhered to a general practice of utilizing maps comprising a minimum of 1,000 points to ensure accuracy and reliability. However, the selection of the threshold was arbitrary, and the impact of such map density on LASE remains uncertain. This hypothesis necessitates further confirmation. Finally, the specific supplementary insights provided by LASE with respect to standard voltage mapping and its power in predicting AF recurrences after CA are still unresolved questions. Regional LASE assessed at different parts of LA may potentially guide the ablation strategy, particularly in non-exhaustive bipolar maps.</p>
</sec>
</sec>
<sec sec-type="conclusion" id="s5">
<title>5 Conclusion</title>
<p>A continuum of electrophysiological abnormalities characterizes the progression of the electrical atrial substrate and AF recurrence after CA. In our study, LASE was correlated with the clinical classification of AF and EAM of LA, independent of basal rhythm.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s6">
<title>Data availability statement</title>
<p>The raw data supporting the conclusion of this article will be made available by the authors, without undue reservation.</p>
</sec>
<sec sec-type="ethics-statement" id="s7">
<title>Ethics statement</title>
<p>The studies involving humans were approved by the Niguarda Hospital Ethic Committee. The studies were conducted in accordance with the local legislation and institutional requirements. The participants provided their written informed consent to participate in this study.</p>
</sec>
<sec sec-type="author-contributions" id="s8">
<title>Author contributions</title>
<p>LG: writing&#x2013;original draft. AP: writing&#x2013;original draft. MS: formal analysis, investigation, and writing&#x2013;original draft. MV: conceptualization, formal analysis, methodology, and writing&#x2013;review and editing. MC: data curation and writing&#x2013;original draft. MB: resources and writing&#x2013;review and editing. MV: investigation and writing&#x2013;review and editing. SV: resources and writing&#x2013;review and editing. FG: methodology and writing&#x2013;review and editing. AF: methodology and writing&#x2013;review and editing. LP: validation and writing&#x2013;review and editing. GC: supervision, validation, and writing&#x2013;review and editing. CA: supervision, validation, and writing&#x2013;review and editing. PM: funding acquisition, project administration, supervision, and writing&#x2013;review and editing. RS: conceptualization, project administration, resources, software, supervision, and writing&#x2013;review and editing.</p>
</sec>
<sec sec-type="funding-information" id="s9">
<title>Funding</title>
<p>The author(s) declare that no financial support was received for the research, authorship, and/or publication of this article.</p>
</sec>
<sec sec-type="COI-statement" id="s10">
<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="s11">
<title>Publisher&#x2019;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>
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