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<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Mol. Biosci.</journal-id>
<journal-title>Frontiers in Molecular Biosciences</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Mol. Biosci.</abbrev-journal-title>
<issn pub-type="epub">2296-889X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">878148</article-id>
<article-id pub-id-type="doi">10.3389/fmolb.2022.878148</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Molecular Biosciences</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Dynamic Modelling of DNA Repair Pathway at the Molecular Level: A New Perspective</article-title>
<alt-title alt-title-type="left-running-head">Lecca and Ihekwaba-Ndibe</alt-title>
<alt-title alt-title-type="right-running-head">Dynamical Modelling of DNA Repair Pathway</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Lecca</surname>
<given-names>Paola</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/201561/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Ihekwaba-Ndibe</surname>
<given-names>Adaoha E. C.</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/310621/overview"/>
</contrib>
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<aff id="aff1">
<sup>1</sup>
<institution>Faculty of Computer Science</institution>, <institution>Free University of Bozen-Bolzano</institution>, <addr-line>Bolzano</addr-line>, <country>Italy</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Faculty of Health and Life Sciences</institution>, <institution>Coventry University</institution>, <addr-line>Coventry</addr-line>, <country>United Kingdom</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/681131/overview">Ernesto Perez-Rueda</ext-link>, Universidad Nacional Aut&#xf3;noma de M&#xe9;xico, Mexico</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/1289438/overview">Arvind Panday</ext-link>, Harvard Medical School, United States</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/174125/overview">Valentina Tozzini</ext-link>, Consiglio Nazionale delle Ricerche, Italy</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Paola Lecca, <email>Paola.Lecca@unibz.it</email>; Adaoha E. C. Ihekwaba-Ndibe, <email>Adaoha.Ihekwaba@coventry.ac.uk</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Biological Modeling and Simulation, a section of the journal Frontiers in Molecular Biosciences</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>13</day>
<month>09</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>9</volume>
<elocation-id>878148</elocation-id>
<history>
<date date-type="received">
<day>17</day>
<month>02</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>22</day>
<month>06</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Lecca and Ihekwaba-Ndibe.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Lecca and Ihekwaba-Ndibe</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>DNA is the genetic repository for all living organisms, and it is subject to constant changes caused by chemical and physical factors. Any change, if not repaired, erodes the genetic information and causes mutations and diseases. To ensure overall survival, robust DNA repair mechanisms and damage-bypass mechanisms have evolved to ensure that the DNA is constantly protected against potentially deleterious damage while maintaining its integrity. Not surprisingly, defects in DNA repair genes affect metabolic processes, and this can be seen in some types of cancer, where DNA repair pathways are disrupted and deregulated, resulting in genome instability. Mathematically modelling the complex network of genes and processes that make up the DNA repair network will not only provide insight into how cells recognise and react to mutations, but it may also reveal whether or not genes involved in the repair process can be controlled. Due to the complexity of this network and the need for a mathematical model and software platform to simulate different investigation scenarios, there must be an automatic way to convert this network into a mathematical model. In this paper, we present a topological analysis of one of the networks in DNA repair, specifically homologous recombination repair (HR). We propose a method for the automatic construction of a system of rate equations to describe network dynamics and present results of a numerical simulation of the model and model sensitivity analysis to the parameters. In the past, dynamic modelling and sensitivity analysis have been used to study the evolution of tumours in response to drugs in cancer medicine. However, automatic generation of a mathematical model and the study of its sensitivity to parameter have not been applied to research on the DNA repair network so far. Therefore, we present this application as an approach for medical research against cancer, since it could give insight into a possible approach with which central nodes of the networks and repair genes could be identified and controlled with the ultimate goal of aiding cancer therapy to fight the onset of cancer and its progression.</p>
</abstract>
<kwd-group>
<kwd>DNA damage</kwd>
<kwd>DNA repair genes</kwd>
<kwd>dynamical networks</kwd>
<kwd>ODE models</kwd>
<kwd>parametric sensitivity analysis</kwd>
<kwd>centrality measure analysis</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>DNA molecules packaged in our chromosomes carry our genetic blueprint, and their preservation is essential for the coordination of cellular function and organization of life (<xref ref-type="bibr" rid="B9">Branzei and Foiani, 2008</xref>). As DNA is the repository of our genetic information, we would expect its structure to be highly stable. This is not the case for the DNA (<xref ref-type="bibr" rid="B92">Reed and Waters, 2005</xref>). Damage to DNA is a constant threat (<xref ref-type="bibr" rid="B71">Lindahl, 1993</xref>; <xref ref-type="bibr" rid="B1">Alberts, 2015</xref>). The DNA molecule is intrinsically reactive, as it is very susceptible to chemical and physical factors, which can lead to DNA lesions, such as base loss, base modification, and double-strand DNA breaks (<xref ref-type="bibr" rid="B47">Hoeijmakers, 2009</xref>; <xref ref-type="bibr" rid="B11">&#xc7;a&#x11f;layan and Wilson, 2015</xref>; <xref ref-type="bibr" rid="B93">Ross and Truant, 2016</xref>; <xref ref-type="bibr" rid="B111">Yadav et al., 2020</xref>). Physiological conditions such as oxygen-rich, aqueous, or pH 7.4 (<xref ref-type="bibr" rid="B71">Lindahl, 1993</xref>) as well as chemical events such as hydrolysis and exposure to reactive oxygen species (ROS) or other reactive metabolites can damage DNA. Exogenous chemicals or endogenous metabolic processes trigger chemical reactions. Although exogenous stressors can be extremely powerful, endogenous threats are constant and unabating. It is estimated that a single cell experiences up to 10<sup>5</sup> spontaneous or induced DNA lesions per day (<xref ref-type="bibr" rid="B71">Lindahl, 1993</xref>; <xref ref-type="bibr" rid="B23">Bont, 2004</xref>; <xref ref-type="bibr" rid="B61">Kovalchuk, 2016</xref>; <xref ref-type="bibr" rid="B17">Chatterjee and Walker, 2017</xref>).</p>
<p>DNA damage has far-reaching consequences, such as preventing RNA polymerase from transcribing the correct messenger RNA sequence to produce the correct protein. In the longer term, cellular malfunctions such as cancer initiation, inborn defects, and ageing that result after damaged DNA replicates are examples of unpredictable long-term consequences of DNA damage; as base misincorporation causes mutations which alter the genetic code (<xref ref-type="bibr" rid="B92">Reed and Waters, 2005</xref>). Therefore, a coordinated response to DNA damage is necessary in order to ensure cellular viability and prevent diseases. Cells, fortunately, possess a robust system of mechanisms that function together to reduce the adverse consequences of DNA damage and ensure that their genetic information is faithfully replicated, thus maintaining the integrity of their genome (<xref ref-type="bibr" rid="B39">Ganai and Johansson, 2016</xref>). This coordinated effort, known as DNA damage response (DDR) operates by sensing and signalling the genotoxic events, and the damage is then resolved either by DNA repair machineries, or cell death if DNA cannot be repaired. DNA repair functions as part of the DNA damage response (DDR) (<xref ref-type="bibr" rid="B75">Liu, 2001</xref>; <xref ref-type="bibr" rid="B17">Chatterjee and Walker, 2017</xref>; <xref ref-type="bibr" rid="B92">Reed and Waters, 2005</xref>; <xref ref-type="bibr" rid="B46">Hoeijmakers, 2001</xref>, <xref ref-type="bibr" rid="B47">2009</xref>).</p>
<p>DNA repair has so far been shown to exist in both prokaryotic and eukaryotic organisms, with over 150 proteins directly involved in safeguarding the genome (<xref ref-type="bibr" rid="B97">Sancar et al., 2004</xref>; <xref ref-type="bibr" rid="B38">Friedberg et al., 2005</xref>; <xref ref-type="bibr" rid="B109">Wood et al., 2005</xref>; <xref ref-type="bibr" rid="B113">Yousefzadeh et al., 2021</xref>). DNA repair processes restore DNA back to its normal sequence and structure after damage (<xref ref-type="bibr" rid="B37">Friedberg et al., 2006</xref>), and are characterised traditionally by the type of damage they repair. There are five major DNA repair pathways available to cells to deal with DNA damage burdens. Each of these processes recognises a particular type of DNA lesions, and together work in preventing mutagenesis. They include 1) direct reversal repairs that repairs lesion induced mainly by alkylating agents, 2) Base excision repair (BER), for small base modifications like single-strand breaks (SSBs) and non-bulky damaged DNA bases, 3) Nucleotide excision repair (NER), that corrects bulky, helix-distorting DNA lesions, 4) mismatch repair (MMR), that repairs base-base mismatch and insertion or deletion loops (IDLs), 5) Recombinational repair, which is divided into non-homologous end joining (NHEJ) and homologous recombination repair (HR), both of which repairs DNA double-strand breaks (DSBs). Other types of DSB repairs include alternative non-homologous end-joining (alt-NHEJ, MMEJ) and translesion synthesis (TLS), which operates as a tolerance mechanism for DNA damage (<xref ref-type="bibr" rid="B53">Jackson and Bartek, 2009</xref>; <xref ref-type="bibr" rid="B48">Hosoya and Miyagawa, 2014</xref>; <xref ref-type="bibr" rid="B68">Li et al., 2021</xref>).</p>
<p>For frequently occurring DNA damage, direct reversal of DNA damage by specialised proteins is the most efficient and most straightforward method of DNA repair. However, this approach is only used by a small proportion of DNA repair types. Most damage to DNA is repaired by the removal of damaged bases and is followed by resynthesis of the removed/excised region (replacement) (<xref ref-type="bibr" rid="B21">Cooper, 2000</xref>). The pathways involved in the removal of base damage are base excision repair (BER), nucleotide excision repair (NER) and mismatch repair (MMR) (<xref ref-type="bibr" rid="B21">Cooper, 2000</xref>). The rest of the pathways repair damage to DNA structure/backbone. DNA damage can cause breaks in the DNA backbone, single-strand breaks in one strand, or double-strand breaks on both strands. Single-strand breaks are repaired by mechanisms sharing common steps in the BER pathway; however, DSBs are especially harmful as, by definition, no unbroken complementary strand exit which can serve as a template for repair when both strands break (<xref ref-type="bibr" rid="B5">Bennett et al., 1993</xref>; <xref ref-type="bibr" rid="B37">Friedberg et al., 2006</xref>). For cells with DNA already replicated prior to cell division, the duplicate copy can easily supply the missing information. So in these cells, DSBs can be repaired by HR, involving the exchange of DNA strands.</p>
<p>Even so, very efficient repair mechanisms can sometimes fail to provide a clean template for DNA synthesis. Replication errors can make it past these mechanisms, as DNA repair can also undergo mutations and become dysregulated. DNA repair gene mutations have been known to cause a variety of rare inherited human syndromes. Some of which include premature ageing phenotypes, increased sensitivity to ionising radiation exposure, and increased cancer risk (<xref ref-type="bibr" rid="B37">Friedberg et al., 2006</xref>; <xref ref-type="bibr" rid="B76">Lok and Powell, 2012</xref>; <xref ref-type="bibr" rid="B13">Carusillo and Mussolino, 2020</xref>). It has also been found that inherited defects in each of the DNA repair pathways are associated with distinct genome instability syndromes (<xref ref-type="bibr" rid="B113">Yousefzadeh et al., 2021</xref>), syndromes characterised by developmental defects (<xref ref-type="bibr" rid="B8">Bouwman and Jonkers, 2012</xref>; <xref ref-type="bibr" rid="B42">Ghosal and Chen, 2013</xref>; <xref ref-type="bibr" rid="B107">Wolters and Schumacher, 2013</xref>; <xref ref-type="bibr" rid="B108">Wood, 2018</xref>).</p>
<p>The dysregulation of DNA repair gene networks underlies many human genetic diseases that affect a wide range of body systems but all share a common trait, predisposition to cancer (<xref ref-type="bibr" rid="B17">Chatterjee and Walker, 2017</xref>). Almost all human cancers are spontaneous, not inherited, and are caused by environmental or genetic factors. It is of great public health interest to determine which genetic variations increase cancer risk in normal populations, and DNA repair genes are likely contenders. Therefore, elucidating the molecular mechanism behind DNA repair defects may provide a framework for understanding the complex pattern of genetic variations that contribute to spontaneous human cancers.</p>
<p>In this study, we demonstrate how to translate a network (mathematically definable as a hyper-graph) into a set of first-order differential equations of the mass action law type. Once the model has been established, we present its numerical solution and carry out a sensitivity analysis of its kinetic rates, whose numerical values are mostly unknown. The results of the analysis of network dynamics complement those produced by the calculation of centrality measures, and together they produce a set of genes of similar biological interest, and in perspective also of medical interest, due to their characteristics of topological centrality and vulnerability to stimuli. The paper is organized as follows: in <xref ref-type="sec" rid="s2">Section 2</xref> we describe the mechanisms of double-strand break repair pathway homologous recombination repair necessary to understand and interpret the results of the computational analysis, in <xref ref-type="sec" rid="s3">Section 3</xref> we describe the rules on which the automatic translation of the network into a rate equation system is based and the methods of sensitivity analysis of the model. In <xref ref-type="sec" rid="s4">Section 4</xref> we present the results of the analysis, and, finally, in <xref ref-type="sec" rid="s5">Section 5</xref>, we draw some conclusions.</p>
</sec>
<sec id="s2">
<title>2 Double-Strand Break Repair Pathway Homologous Recombination Repair</title>
<p>DSBs are the most serious DNA damage, as both DNA strands are impaired simultaneously. Therefore, due to the magnitude of differing factors leading to DSBs, the effectiveness of their repair is crucial for cell survival and the functioning and prevention of DNA fragmentation, chromosomal translocation and deletion. DSBs can be repaired in mammalian cells by NHEJ, HR, and single-strand annealing (SSA). Unrepaired SSBs result in much more cytotoxic DSBs formation during the S-phase progression of the cell cycle (<xref ref-type="bibr" rid="B57">Kennedy and D&#x2019;Andrea, 2006</xref>). Homologous recombination is a process by which DSBs are repaired through the alignment of homologous sequences of DNA (<xref ref-type="bibr" rid="B26">Dietlein and Reinhardt, 2014</xref>) and occurs primarily during the late S to G2 phase of the cell cycle (<xref ref-type="bibr" rid="B15">Cerbinskaite et al., 2012</xref>; <xref ref-type="bibr" rid="B17">Chatterjee and Walker, 2017</xref>).</p>
<p>Homologous recombination is the second major DSB repair pathway and requires a second, homologous DNA sequence to function as donor template. There are two phases to this process, the first phase triggered by sensor proteins that belong to the MRN complex, and the second phase by the stimulation of resection steps, initiated in the first phase and subsequently extended. HR generally involves the following stages:<list list-type="simple">
<list-item>
<p>1. DSBs are recognised and sensed by the MRN complex (<xref ref-type="bibr" rid="B59">Kim et al., 1994</xref>), which activates ATM kinase, initiating the DSB end resection steps, where CtBP-interacting protein (CtIP) and the MRN complex work together to generate single-strand DNA (ssDNA) at the DSB ends ((<xref ref-type="bibr" rid="B115">Zhao et al., 2020</xref>).</p>
</list-item>
<list-item>
<p>2. The exposed ssDNA is recognised by and coated with DNA replication protein A (RPA) complex, which recruits the major homologous recombination regulator RAD52 to the site to facilitate HR repair (<xref ref-type="bibr" rid="B78">Mar&#xe9;chal and Zou, 2014</xref>; <xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>).</p>
</list-item>
<list-item>
<p>3. The nucleoprotein filament RAD51, is then assembled, mediated by BReast CAncer type 2 susceptibility protein (BRCA2), to replace RPA on ssDNA to perform homology sequence searching and strand invasion (<xref ref-type="bibr" rid="B62">Kowalczykowski, 2015</xref>).</p>
</list-item>
<list-item>
<p>4. DSBs are then restored by branch migration, DNA synthesis, ligation, and resolution of Holliday junctions (<xref ref-type="bibr" rid="B115">Zhao et al., 2020</xref>).</p>
</list-item>
</list>
</p>
<p>Following the recognition and sensing of DSBs, a process known as DNA end resection is activated, a critical function in HR (<xref ref-type="bibr" rid="B74">Liu and Huang, 2016</xref>; <xref ref-type="bibr" rid="B115">Zhao et al., 2020</xref>). DNA end resection catalyses the nucleolytic degradation of the broken ends of DSBs (by the CtIPMRN complex) in the 5&#x2032; to 3&#x2032; direction generating 3&#x2032; single-stranded DNA (ssDNA). The 3&#x2032; ssDNA then provides a platform for the recruitment of HR repair-related proteins (<xref ref-type="bibr" rid="B50">Huertas, 2010</xref>; <xref ref-type="bibr" rid="B74">Liu and Huang, 2016</xref>; <xref ref-type="bibr" rid="B115">Zhao et al., 2020</xref>). Following the generation of ssDNA, downstream nucleases and helicases, such as exonuclease 1 (EXO1) or DNA replication ATP-dependent helicase/nuclease DNA replication helicasenuclease 2 (DNA2) and Bloom syndrome protein (BLM), are conscripted to extend the 3&#x2019; ssDNA for HR repair (<xref ref-type="bibr" rid="B51">Huertas and Jackson, 2009</xref>; <xref ref-type="bibr" rid="B114">Yun and Hiom, 2009</xref>; <xref ref-type="bibr" rid="B115">Zhao et al., 2020</xref>). The identities of these DNA helicases and nucleases are yet to be clearly defined in humans (as in yeast), partly because there are many candidate proteins. Although five RecQ helicase homologs have so far been identified in yeast (Bloom helicase [BLM], Werner helicase/nuclease [WRN], RECQ1, RECQ4, and RECQ5) (<xref ref-type="bibr" rid="B20">Chu and Hickson, 2009</xref>; <xref ref-type="bibr" rid="B77">Lu and Davis, 2021</xref>), convincing evidence point up BLM in resection (<xref ref-type="bibr" rid="B43">Gravel et al., 2008</xref>; <xref ref-type="bibr" rid="B84">Nimonkar et al., 2008</xref>). Following resection, the exposed single-strand DNA (ssDNA) is recognised and bound by RPA complex for protection.</p>
<p>RPA plays a significant role in coordinating DNA resection processes and simultaneously preserving the integrity of the resultant ssDNA (<xref ref-type="bibr" rid="B102">Sun et al., 2019</xref>). RPA is a heterotrimeric ssDNA binding protein essential to nearly all DNA processing events and associates with ssDNA with very high affinity (Kd sim 109&#x2013;1010&#xa0;M) (<xref ref-type="bibr" rid="B78">Mar&#xe9;chal and Zou, 2014</xref>). It is comprised of three protein subunits, RPA70, RPA32 and RPA14 and contains multiple oligonucleotideoligosaccharide (OB)-folds that interact with both ssDNA and proteins (<xref ref-type="bibr" rid="B59">Kim et al., 1994</xref>; <xref ref-type="bibr" rid="B31">Fanning, 2006</xref>; <xref ref-type="bibr" rid="B32">Feldkamp et al., 2014</xref>; <xref ref-type="bibr" rid="B78">Mar&#xe9;chal and Zou, 2014</xref>). RPA is flexible (<xref ref-type="bibr" rid="B117">Brosey et al., 2013</xref>). Its versatile nature allows it to coordinate the recruitment, activation and exchange of many proteins whose combined activities allow for the protection and propagation of eukaryotic genomes (<xref ref-type="bibr" rid="B78">Mar&#xe9;chal and Zou, 2014</xref>). How multiple RPAs associate on ssDNA and coordinate its vast array of processes remains to be determined (<xref ref-type="bibr" rid="B102">Sun et al., 2019</xref>). However, a critical feature of RPA is that, though it can bind nucleic acids with very high affinity, it can easily be displaced by other enzymes for further downstream processing (<xref ref-type="bibr" rid="B102">Sun et al., 2019</xref>).</p>
<p>When ssDNA length is sufficient for HR repair, the end resection process is terminated (<xref ref-type="bibr" rid="B116">Zhao et al., 2015</xref>). Although the regulation of DNA end resection termination are not yet clearly understood, several studies suggest that under physiological conditions, end resection is terminated by RAD51-RPA switching (<xref ref-type="bibr" rid="B116">Zhao et al., 2015</xref>). This switching is regulated by BRCA2-DSS1. DSS1 - SEM1 in yeast - is a small, highly acidic protein that competes with ssDNA, by mimicking ssDNA in order to remove RPA from the genuine ssDNA (<xref ref-type="bibr" rid="B116">Zhao et al., 2015</xref>; <xref ref-type="bibr" rid="B100">Stefanovie et al., 2019</xref>; <xref ref-type="bibr" rid="B65">Le et al., 2020</xref>; <xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>). The DSS1 then binds to BRCA2 in order to facilitate RAD51 filament formation (<xref ref-type="bibr" rid="B73">Liu et al., 2010</xref>; <xref ref-type="bibr" rid="B100">Stefanovie et al., 2019</xref>; <xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>). DSS1 does not seem to bind DNA on its own but appears to enhance ssDNA binding activities of BRCA2 and RAD52 to promote DSB repair (<xref ref-type="bibr" rid="B116">Zhao et al., 2015</xref>). BRCA2 then recruits RAD51 to complete the switch (<xref ref-type="bibr" rid="B116">Zhao et al., 2015</xref>; <xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>). For cells with DNA already replicated prior to cell division, RAD51 will oligomerise and form a nucleoprotein filament on the resected, single-stranded DNA (ssDNA) end of the DSB, and search for the homologous DNA sequence on the undamaged sister chromatid, performs strand exchange (invasion), and produce a joint molecule called a D-loop (<xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>). DNA polymerase will then use the homologous DNA strand as a template from the D-loop, and the 3&#x2032;-end of the broken DNA strand as a primer to commence DNA repair synthesis (<xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>). The other end of the double-strand break is then apprehended by RAD52, joining it to the D-loop, through the annealing process, causing the displaced strand to act as a template for the second strand synthesis (<xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>). When DNA synthesis is complete, the D-loops are then dissociated by RAD54, a protein that interacts with RAD51 to promote branch migration, or interacts with helicases like BLM (<xref ref-type="bibr" rid="B104">van Brabant et al., 2000</xref>; <xref ref-type="bibr" rid="B10">Bugreev et al., 2006</xref>; <xref ref-type="bibr" rid="B56">Kawale and Sung, 2020</xref>; <xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>). DNA is further extended by DNA polymerase, annealed to the ssDNA part of the second broken DNA, gap filled and finally restored (<xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>). In <xref ref-type="fig" rid="F1">Figure 1</xref> we summarise what is described in this section about the DSB signalling mechanisms.</p>
<p>Homologous recombination is able to repair DSBs error-free using the undamaged sister chromatid (<xref ref-type="bibr" rid="B26">Dietlein and Reinhardt, 2014</xref>). As the accuracy of homologous recombination repair is important for DSBs (<xref ref-type="bibr" rid="B101">Sugiyama and Kantake, 2009</xref>), if it is impaired, chemotherapeutic opportunities may arise (<xref ref-type="bibr" rid="B49">Huang and Zhou, 2021</xref>).</p>
</sec>
<sec id="s3">
<title>3 Graph Representation and Mathematical Model</title>
<p>We considered HDR through Homologous Recombination (HRR) network as available in Pathways Commons (<xref ref-type="bibr" rid="B14">Cerami et al., 2010</xref>) in the SIF (Simple Interaction Format) format at the link in the reference (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>). See these data also reported in <xref ref-type="sec" rid="s11">Supplementary Tables S1&#x2013;S3</xref>.</p>
<p>We implemented an R script, that takes as input the HR network and is able to.<list list-type="simple">
<list-item>
<p>&#x2022; analyse the topology of the network through the calculation of standard and new centrality measures. The standard node centrality measures considered in this study are the degree (in-, out- and total), the betweenness, the clustering coefficient, the eingenvector centrality, the vibrational centrality, the subgraph centrality, and the information centrality (see (<xref ref-type="bibr" rid="B79">Marsden, 2005</xref>; <xref ref-type="bibr" rid="B60">Kosch&#xfc;tzki and Schreiber, 2008</xref>; <xref ref-type="bibr" rid="B41">Ghasemi et al., 2014</xref>; <xref ref-type="bibr" rid="B106">Wang et al., 2014</xref>; <xref ref-type="bibr" rid="B35">Fornito et al., 2016</xref>; <xref ref-type="bibr" rid="B54">Jalili et al., 2016</xref>; <xref ref-type="bibr" rid="B2">Ashtiani et al., 2018</xref>) for a concise but comprehensive report on the meaning and the use of these measure in molecular biology). We considered also a new centrality measures, such as vibrational centrality, introduced by Estrada in (<xref ref-type="bibr" rid="B27">Estrada and Hatano, 2010</xref>) that we will discuss in more detail in the next section (we also refer the reader to (<xref ref-type="bibr" rid="B67">Lecca and Re, 2019</xref>) for a review on vibrational centrality); for the reader&#x2019;s convenience, we list the definition of these centrality indices in <xref ref-type="sec" rid="s11">Supplementary Table S4</xref>, that are also extensively covered in many textbooks on graph theory, and in various articles in the applied sciences. We refer the reader to Estrada&#x2019;s numerous works, a comprehensive compendium of which can be found in the book (<xref ref-type="bibr" rid="B27">Estrada and Hatano, 2010</xref>; <xref ref-type="bibr" rid="B30">Estrada, 2011</xref>);</p>
</list-item>
<list-item>
<p>&#x2022; automatically generate a system of rate equations, specifically first order mass action differential equations, describing the dynamics of the network.</p>
</list-item>
</list>
</p>
<p>and a R script implementing parametric sensitivity analysis of the dynamics model.</p>
<p>In the dynamics model, by default the kinetic rate constants <italic>k</italic> a well as the initial values of the proteins and molecules concentrations are set equal to random values in fixed ranges. Nevertheless these ranges can be modified by the user as shown by the interactive console output reported in <xref ref-type="table" rid="T1">Table 1</xref>. However, we note that the interval of definition of the uniform distribution cannot exceed the maximal range of parameter variability within which the system of rate equations has a solution. We refer the reader to a previous work of us (<xref ref-type="bibr" rid="B66">Lecca et al., 2016</xref>) for more details on this.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Interactive graphical user interface of NADS software showing the options and the task concerning the generation of ODE equations and their solution.</p>
</caption>
<table>
<tbody valign="top">
<tr>
<td align="center">
<inline-graphic xlink:href="FMOLB_fmolb-2022-878148_wc_tfx1.tif"/>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>In a first experiment, the initial values of the proteins concentration (not experimentally known) has been drawn randomly in a range [1, 100] a. u., and the simulation time interval was [0, 10] a. u. In a second experiment, the numerical simulation of the model was performed by assigning an initial quantity between 18 and 20 (expressed in arbitrary units a. u.) to each node and for <italic>t</italic> &#x2208; [0, 1400] (in arbitrary units). The solution of the system of 25 differential equations converges for values of rate constants in the range <inline-formula id="inf1">
<mml:math id="m1">
<mml:mrow>
<mml:mo stretchy="false">[</mml:mo>
<mml:mo stretchy="false">]</mml:mo>
</mml:mrow>
<mml:mn>0,0.01</mml:mn>
<mml:mfenced open="" close="]">
</mml:mfenced>
</mml:math>
</inline-formula> a. u. in the first experiment, and in the range <inline-formula id="inf2">
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<mml:mo stretchy="false">]</mml:mo>
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<mml:mrow>
<mml:mn>0</mml:mn>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>6</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mo>,</mml:mo>
<mml:mn>1</mml:mn>
<mml:msup>
<mml:mrow>
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<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>5</mml:mn>
</mml:mrow>
</mml:msup>
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</mml:mfenced>
</mml:math>
</inline-formula> a.u. in the second experiment. To the best of our knowledge, the <italic>in vivo</italic> concentrations of the proteins that are part of the HR network are not known. Combined with the lack of knowledge of the values of rate constants, this means that we cannot assign units to these values that reflect <italic>in vivo</italic> kinetics. However, the initial values of the protein concentrations have been chosen from the order of magnitude at which various <italic>in vitro</italic> experiments operate and express these concentrations in nM and time in seconds. The literature we have referred to includes the works of (<xref ref-type="bibr" rid="B112">Yang et al., 2010</xref>; <xref ref-type="bibr" rid="B83">Nguyen et al., 2013</xref>; <xref ref-type="bibr" rid="B34">Foertsch et al., 2019</xref>).</p>
<p>We changed the parameters one at a time while keeping the values of the others fixed. Since for each parameter <italic>p</italic>
<sub>
<italic>h</italic>
</sub> (<italic>h</italic> ranges from 1 to the number of parameters in the equations), we sampled <italic>N</italic>
<sub>
<italic>P</italic>
</sub> values, and consequently we performed <italic>N</italic>
<sub>
<italic>P</italic>
</sub> model simulations. Let us denote with <italic>x</italic>
<sub>
<italic>s</italic>
</sub>(<italic>t</italic>), (<italic>s</italic> &#x3d; 1, 2, <italic>&#x2026;</italic>, <italic>d</italic>) the time series expressing the numerical solutions of the rate equations, where <italic>d</italic> is the number of the proteins in the network. The index of sensitivity of <italic>x</italic>
<sub>
<italic>s</italic>
</sub>(<italic>t</italic>) with respect to the change of <italic>h</italic>-th parameter from the value <italic>p</italic>
<sub>
<italic>h</italic>
</sub> to the value <inline-formula id="inf3">
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</mml:mrow>
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</mml:math>
</inline-formula> is calculated as in (<xref ref-type="bibr" rid="B66">Lecca et al., 2016</xref>) by<disp-formula id="e1">
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<label>(1)</label>
</disp-formula>where <italic>N</italic> is the length of the time series <inline-formula id="inf4">
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</mml:mrow>
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</mml:mrow>
</mml:msub>
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<mml:msubsup>
<mml:mrow>
<mml:mi>p</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>h</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2032;</mml:mo>
</mml:mrow>
</mml:msubsup>
</mml:mrow>
</mml:mfenced>
<mml:mo>.</mml:mo>
</mml:math>
<label>(2)</label>
</disp-formula>where &#x201c;<inline-formula id="inf5">
<mml:math id="m7">
<mml:msub>
<mml:mrow>
<mml:mi>p</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>h</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2190;</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mi>p</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>h</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2032;</mml:mo>
</mml:mrow>
</mml:msubsup>
</mml:math>
</inline-formula>&#x201d; means &#x201c;<italic>p</italic>
<sub>
<italic>h</italic>
</sub> replaced by <inline-formula id="inf6">
<mml:math id="m8">
<mml:msubsup>
<mml:mrow>
<mml:mi>p</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>h</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2032;</mml:mo>
</mml:mrow>
</mml:msubsup>
</mml:math>
</inline-formula>&#x201d;. The <xref ref-type="disp-formula" rid="e1">Eq. 1</xref> defines the mean of the standard deviations of the distributions of the simulated values of a protein/gene abundance at time points <italic>t</italic>
<sub>
<italic>k</italic>
</sub>.</p>
<p>In case the user knows the values of the rate constants, he/she can add them as an extra column to the SIF format of the input files. At the moment of writing, for most interactions the values of the kinetic constants are not known and there are no time-resolved data from which it is possible to infer them. It is precisely this context that justifies our choice to study the dynamics of the system in a range of values of the model parameters and more generally to provide a software that can be used as a platform for in silico experiments.</p>
<p>We implemented Network Analyser and Dynamics Simulator (NADS) consists of three modules written in R language:<list list-type="simple">
<list-item>
<p>&#x2022; network_analysis_functions.R: this module implements the functions that processes the SIF data-frames to make them suitable to their conversion into a graph. This module also implement the functions to rank the nodes according to their centrality measures;</p>
</list-item>
<list-item>
<p>&#x2022; graph_parser.R: this module converts the SIF format network into an R script that solves the corresponding ordinary differential equations;</p>
</list-item>
<list-item>
<p>&#x2022; network_analysis.R: this module first calls network_analysis_functions.R and performs the networks analysis, and secondly it calls the module graph_parser.R that generates the script dynamics.R containing the differential equations of the network dynamics.</p>
</list-item>
</list>
</p>
<p>The user can launch the software simply by running in RStudio the script network_analysis.R, and then by answering to the questions in the interactive interface as shown in <xref ref-type="table" rid="T2">Table 2</xref>.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Interactive graphical user interface of NADS software showing the options and the task concerning the analysis of network topology.</p>
</caption>
<table>
<tbody valign="top">
<tr>
<td align="center">
<inline-graphic xlink:href="FMOLB_fmolb-2022-878148_wc_tfx2.tif"/>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>We provide also the fourth module implementing the parametric sensitivity analysis, named sensitivity_analysis.R, which takes as an input the system of equations automatically generated by network_analysis.R.</p>
<p>The main module is the script network_analysis.R. As soon as the user runs it from the R Studio GUI (<xref ref-type="bibr" rid="B91">R Studio, 2022</xref>) or from a terminal, an interactive output is displayed as in <xref ref-type="table" rid="T2">Tables 2</xref>, <xref ref-type="table" rid="T3">3</xref>. The program asks the user to select the network to be analysed and then.<list list-type="simple">
<list-item>
<p>&#x2022; it calculates the centralities measures</p>
</list-item>
<list-item>
<p>&#x2022; it translates the SIF network into a hyper-graph structure according to the rules reported in <xref ref-type="fig" rid="F2">Figure 2</xref>
</p>
</list-item>
<list-item>
<p>&#x2022; then, it translates the hyper-graph into a set of ordinary differential equations, according to the rules reported in <xref ref-type="table" rid="T3">Table 3</xref>,</p>
</list-item>
<list-item>
<p>&#x2022; and, finally, it solves them.</p>
</list-item>
</list>
</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>The signalling of a DSB is initiated via the binding of the MRN complex which initiates resection. During HR, the ends of the double-strand break (DSB) are resected by nucleases, exposing single-strand DNA (ssDNA) that becomes bound by RPA. The mediator protein, BRCA2 initiates the loading of RAD51 onto ssDNA, helping to displace RPA. RAD51 oligomerizes, forms a nucleoprotein filament, and then searches for the homologous DNA sequence on the intact chromosome. RAD51 filament invades the intact dsDNA and forms a D-loop structure. It is further processed by DNA polymerases, chromatin remodelers (RAD54), nucleases, and ligases to restore it back to its original sequences. (Adapted from (<xref ref-type="bibr" rid="B94">Rossi et al., 2021</xref>).</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g001.tif"/>
</fig>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Conversion of the SIF format interactions into a (hyper-)graph structure.</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g002.tif"/>
</fig>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>Translation of BioPAX interactions into simple ordinary differential equations. See in <xref ref-type="fig" rid="F2">Figure 2</xref> the (hyper-)graph representation of these interactions.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Interaction</th>
<th align="center">Differential equation</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">A controls production of B</td>
<td align="center">
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<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>B</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>k</mml:mi>
<mml:mi>A</mml:mi>
</mml:math>
</inline-formula>, <inline-formula id="inf8">
<mml:math id="m10">
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>A</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0</mml:mn>
</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td align="left">B controls consumption of A</td>
<td align="center">
<inline-formula id="inf9">
<mml:math id="m11">
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>A</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>k</mml:mi>
<mml:mi>B</mml:mi>
</mml:math>
</inline-formula>, <inline-formula id="inf10">
<mml:math id="m12">
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>B</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0</mml:mn>
</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td align="left">A interacts with B</td>
<td align="center">
<inline-formula id="inf11">
<mml:math id="m13">
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>A</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>B</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>k</mml:mi>
<mml:mi>A</mml:mi>
<mml:mi>B</mml:mi>
</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td align="left">A catalysis precedes B</td>
<td align="center">
<inline-formula id="inf12">
<mml:math id="m14">
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>B</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mo>&#xb1;</mml:mo>
<mml:mi>k</mml:mi>
<mml:mi>A</mml:mi>
</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td align="left">A used to produce B</td>
<td align="center">
<inline-formula id="inf13">
<mml:math id="m15">
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>B</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>k</mml:mi>
<mml:mi>A</mml:mi>
</mml:math>
</inline-formula>
</td>
</tr>
<tr>
<td align="left">A chemical affects B</td>
<td align="center">
<inline-formula id="inf14">
<mml:math id="m16">
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>A</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0</mml:mn>
</mml:math>
</inline-formula>, <inline-formula id="inf15">
<mml:math id="m17">
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>B</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x3d;</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>k</mml:mi>
<mml:mi>B</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mo>&#x2212;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:msup>
<mml:mrow>
<mml:mi>B</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2a;</mml:mo>
</mml:mrow>
</mml:msup>
</mml:mrow>
<mml:mrow>
<mml:mi>d</mml:mi>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfrac>
</mml:math>
</inline-formula>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The program returns also the execution times for the tasks expected to be the most computationally demanding, such as integrating the equation.</p>
</sec>
<sec id="s4">
<title>4 Results</title>
<p>The HR network considered in this study has 25 nodes and 250 edges, as reported in <xref ref-type="sec" rid="s11">Supplementary Tables S1&#x2013;S3</xref>. The right part of the <xref ref-type="fig" rid="F4">Figure 4</xref> shows the HR network in circular layout. The network analysis phase of our study calculated the centrality measures distributions show in <xref ref-type="fig" rid="F3">Figure 3</xref>, and identified six genes, as shown in <xref ref-type="table" rid="T4">Table 4</xref>:<list list-type="simple">
<list-item>
<p>1. BLM, scoring first for vibrational centrality</p>
</list-item>
<list-item>
<p>2. RAD50 scores first for sub-graph centrality</p>
</list-item>
<list-item>
<p>3. RAD52, scoring first for clustering coefficient</p>
</list-item>
<list-item>
<p>4. RPA1, scoring first for total degree and betweenness</p>
</list-item>
<list-item>
<p>5. RPA2, scoring first for in-degree and eigenvector centrality</p>
</list-item>
<list-item>
<p>6. RPA3, scoring first for out-degree, hub centrality, and sub-graph centrality</p>
</list-item>
<list-item>
<p>7. RPA4, scoring first for clustering coefficient</p>
</list-item>
<list-item>
<p>8. SEM1, scoring first for clustering coefficient.</p>
</list-item>
</list>
</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Distributions of the centrality measures of HR pathway (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>). We observe that the majority of node have low betweenness, low information centrality and high vibrational centrality.</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g003.tif"/>
</fig>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>HR network and FANCM network. Colors vary from yellow to green according to increasing degree values. Node sizes grow as the betweenness centrality of nodes.</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g004.tif"/>
</fig>
<table-wrap id="T4" position="float">
<label>TABLE 4</label>
<caption>
<p>Values of the centrality measures for the HR pathway in (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>). In bold, we marked the genes/proteins with the highest scores.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Protein</th>
<th align="center">Total degree</th>
<th align="center">In-degree</th>
<th align="center">Out-degree</th>
<th align="center">Hub centrality</th>
<th align="center">Betweenness</th>
<th align="center">Clustering coefficient</th>
<th align="center">Eigenvector centrality</th>
<th align="center">Vibrational centrality</th>
<th align="center">Subgraph centrality</th>
<th align="center">Information centrality</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">BLM</td>
<td align="char" char=".">30</td>
<td align="char" char=".">19</td>
<td align="char" char=".">11</td>
<td align="center">4.08E-01</td>
<td align="char" char=".">39.5138622</td>
<td align="center">0.2183908</td>
<td align="char" char=".">0.81043641</td>
<td align="char" char=".">
<bold>1.0771148</bold>
</td>
<td align="char" char=".">7408.13084</td>
<td align="char" char=".">0.08351073</td>
</tr>
<tr>
<td align="left">EME1</td>
<td align="char" char=".">13</td>
<td align="char" char=".">0</td>
<td align="char" char=".">13</td>
<td align="center">5.21E-01</td>
<td align="char" char=".">0</td>
<td align="center">0.5384615</td>
<td align="char" char=".">0.2589557</td>
<td align="char" char=".">0.9579369</td>
<td align="char" char=".">2709.62496</td>
<td align="char" char=".">0.13185164</td>
</tr>
<tr>
<td align="left">MRE11</td>
<td align="char" char=".">26</td>
<td align="char" char=".">16</td>
<td align="char" char=".">10</td>
<td align="center">3.69E-01</td>
<td align="char" char=".">9.2926175</td>
<td align="center">0.1969231</td>
<td align="char" char=".">0.73968044</td>
<td align="char" char=".">1.0587524</td>
<td align="char" char=".">6020.65076</td>
<td align="char" char=".">0.08957011</td>
</tr>
<tr>
<td align="left">MUS81</td>
<td align="char" char=".">13</td>
<td align="char" char=".">1</td>
<td align="char" char=".">12</td>
<td align="center">5.18E-01</td>
<td align="char" char=".">0</td>
<td align="center">0.5384615</td>
<td align="char" char=".">0.2589557</td>
<td align="char" char=".">0.9547013</td>
<td align="char" char=".">2291.00787</td>
<td align="char" char=".">0.13177729</td>
</tr>
<tr>
<td align="left">NBN</td>
<td align="char" char=".">27</td>
<td align="char" char=".">17</td>
<td align="char" char=".">10</td>
<td align="center">3.67E-01</td>
<td align="char" char=".">9.2926175</td>
<td align="center">0.1823362</td>
<td align="char" char=".">0.76703983</td>
<td align="char" char=".">1.0603542</td>
<td align="char" char=".">6020.65076</td>
<td align="char" char=".">0.08786049</td>
</tr>
<tr>
<td align="left">POLD1</td>
<td align="char" char=".">26</td>
<td align="char" char=".">9</td>
<td align="char" char=".">17</td>
<td align="center">6.83E-01</td>
<td align="char" char=".">7.8121197</td>
<td align="center">0.36</td>
<td align="char" char=".">0.67253587</td>
<td align="char" char=".">0.9655278</td>
<td align="char" char=".">7684.50086</td>
<td align="char" char=".">0.08965382</td>
</tr>
<tr>
<td align="left">POLD2</td>
<td align="char" char=".">23</td>
<td align="char" char=".">5</td>
<td align="char" char=".">18</td>
<td align="center">7.10E-01</td>
<td align="char" char=".">5.8377525</td>
<td align="center">0.4624506</td>
<td align="char" char=".">0.57100865</td>
<td align="char" char=".">0.9672104</td>
<td align="char" char=".">9065.81813</td>
<td align="char" char=".">0.09552092</td>
</tr>
<tr>
<td align="left">POLD3</td>
<td align="char" char=".">23</td>
<td align="char" char=".">8</td>
<td align="char" char=".">15</td>
<td align="center">6.45E-01</td>
<td align="char" char=".">5.8377525</td>
<td align="center">0.4624506</td>
<td align="char" char=".">0.57100865</td>
<td align="char" char=".">0.961071</td>
<td align="char" char=".">5521.89505</td>
<td align="char" char=".">0.09524672</td>
</tr>
<tr>
<td align="left">POLD4</td>
<td align="char" char=".">23</td>
<td align="char" char=".">7</td>
<td align="char" char=".">16</td>
<td align="center">6.66E-01</td>
<td align="char" char=".">5.8377525</td>
<td align="center">0.4624506</td>
<td align="char" char=".">0.57100865</td>
<td align="char" char=".">0.963361</td>
<td align="char" char=".">6513.86378</td>
<td align="char" char=".">0.09533952</td>
</tr>
<tr>
<td align="left">
<bold>RAD50</bold>
</td>
<td align="char" char=".">27</td>
<td align="char" char=".">13</td>
<td align="char" char=".">14</td>
<td align="center">5.79E-01</td>
<td align="char" char=".">10.2729789</td>
<td align="center">0.2108262</td>
<td align="char" char=".">0.75819149</td>
<td align="char" char=".">1.0206621</td>
<td align="char" char=".">
<bold>11427.9652</bold>
</td>
<td align="char" char=".">0.08811688</td>
</tr>
<tr>
<td align="left">RAD51</td>
<td align="char" char=".">23</td>
<td align="char" char=".">12</td>
<td align="char" char=".">11</td>
<td align="center">4.03E-01</td>
<td align="char" char=".">30.3997662</td>
<td align="center">0.4426877</td>
<td align="char" char=".">0.49447273</td>
<td align="char" char=".">0.9038147</td>
<td align="char" char=".">1403.03278</td>
<td align="char" char=".">0.09426237</td>
</tr>
<tr>
<td align="left">RAD51B</td>
<td align="char" char=".">14</td>
<td align="char" char=".">12</td>
<td align="char" char=".">2</td>
<td align="center">8.58E-02</td>
<td align="char" char=".">0.3636364</td>
<td align="center">0.7032967</td>
<td align="char" char=".">0.31841389</td>
<td align="char" char=".">0.9960094</td>
<td align="char" char=".">74.47586</td>
<td align="char" char=".">0.12453711</td>
</tr>
<tr>
<td align="left">RAD51C</td>
<td align="char" char=".">21</td>
<td align="char" char=".">9</td>
<td align="char" char=".">12</td>
<td align="center">4.96E-01</td>
<td align="char" char=".">1.6614219</td>
<td align="center">0.4095238</td>
<td align="char" char=".">0.47619405</td>
<td align="char" char=".">0.9027594</td>
<td align="char" char=".">1911.88011</td>
<td align="char" char=".">0.09955242</td>
</tr>
<tr>
<td align="left">RAD51D</td>
<td align="char" char=".">16</td>
<td align="char" char=".">11</td>
<td align="char" char=".">5</td>
<td align="center">2.15E-01</td>
<td align="char" char=".">0.5127787</td>
<td align="center">0.7166667</td>
<td align="char" char=".">0.3593928</td>
<td align="char" char=".">0.9248884</td>
<td align="char" char=".">282.05774</td>
<td align="char" char=".">0.11524626</td>
</tr>
<tr>
<td align="left">
<bold>RAD52</bold>
</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">1.01E-01</td>
<td align="char" char=".">0</td>
<td align="center">
<bold>1</bold>
</td>
<td align="char" char=".">0.1247068</td>
<td align="char" char=".">0.9567526</td>
<td align="char" char=".">254.41809</td>
<td align="char" char=".">0.30199153</td>
</tr>
<tr>
<td align="left">
<bold>RPA1</bold>
</td>
<td align="char" char=".">
<bold>41</bold>
</td>
<td align="char" char=".">20</td>
<td align="char" char=".">21</td>
<td align="center">9.02E-01</td>
<td align="char" char=".">
<bold>93.2152627</bold>
</td>
<td align="center">0.1512195</td>
<td align="char" char=".">0.89284007</td>
<td align="char" char=".">0.9069973</td>
<td align="char" char=".">8617.68902</td>
<td align="char" char=".">0.0726257</td>
</tr>
<tr>
<td align="left">
<bold>RPA2</bold>
</td>
<td align="char" char=".">
<bold>41</bold>
</td>
<td align="char" char=".">
<bold>22</bold>
</td>
<td align="char" char=".">19</td>
<td align="center">8.46E-01</td>
<td align="char" char=".">32.6964097</td>
<td align="center">0.1487805</td>
<td align="char" char=".">
<bold>1</bold>
</td>
<td align="char" char=".">0.9404821</td>
<td align="char" char=".">8508.98841</td>
<td align="char" char=".">0.07306925</td>
</tr>
<tr>
<td align="left">
<bold>RPA3</bold>
</td>
<td align="char" char=".">34</td>
<td align="char" char=".">11</td>
<td align="char" char=".">
<bold>23</bold>
</td>
<td align="center">
<bold>1.00E&#x2b;00</bold>
</td>
<td align="char" char=".">25.979693</td>
<td align="center">0.2174688</td>
<td align="char" char=".">0.819185</td>
<td align="char" char=".">0.9803911</td>
<td align="char" char=".">
<bold>14870.10272</bold>
</td>
<td align="char" char=".">0.07928594</td>
</tr>
<tr>
<td align="left">
<bold>RPA4</bold>
</td>
<td align="char" char=".">3</td>
<td align="char" char=".">0</td>
<td align="char" char=".">3</td>
<td align="center">1.27E-01</td>
<td align="char" char=".">0</td>
<td align="center">
<bold>1</bold>
</td>
<td align="char" char=".">0.10547581</td>
<td align="char" char=".">0.9592952</td>
<td align="char" char=".">700.52299</td>
<td align="char" char=".">0.37822514</td>
</tr>
<tr>
<td align="left">
<bold>SEM1</bold>
</td>
<td align="char" char=".">3</td>
<td align="char" char=".">1</td>
<td align="char" char=".">2</td>
<td align="center">9.14E-02</td>
<td align="char" char=".">0</td>
<td align="center">
<bold>1</bold>
</td>
<td align="char" char=".">0.06803348</td>
<td align="char" char=".">0.9398974</td>
<td align="char" char=".">63.99639</td>
<td align="char" char=".">0.37757664</td>
</tr>
<tr>
<td align="left">TOP3A</td>
<td align="char" char=".">24</td>
<td align="char" char=".">12</td>
<td align="char" char=".">12</td>
<td align="center">4.64E-01</td>
<td align="char" char=".">9.2926175</td>
<td align="center">0.2318841</td>
<td align="char" char=".">0.68062612</td>
<td align="char" char=".">1.0251952</td>
<td align="char" char=".">8739.44955</td>
<td align="char" char=".">0.09349123</td>
</tr>
<tr>
<td align="left">XRCC2</td>
<td align="char" char=".">15</td>
<td align="char" char=".">14</td>
<td align="char" char=".">1</td>
<td align="center">5.60E-02</td>
<td align="char" char=".">0.8476272</td>
<td align="center">0.7142857</td>
<td align="char" char=".">0.34875334</td>
<td align="char" char=".">1.0105203</td>
<td align="char" char=".">55.0254</td>
<td align="char" char=".">0.11916455</td>
</tr>
<tr>
<td align="left">XRCC3</td>
<td align="char" char=".">13</td>
<td align="char" char=".">12</td>
<td align="char" char=".">1</td>
<td align="center">4.68E-02</td>
<td align="char" char=".">0.3333333</td>
<td align="center">0.8076923</td>
<td align="char" char=".">0.2842042</td>
<td align="char" char=".">0.5530372</td>
<td align="char" char=".">0</td>
<td align="char" char=".">0.13016119</td>
</tr>
<tr>
<td align="left">BRCA2</td>
<td align="char" char=".">16</td>
<td align="char" char=".">16</td>
<td align="char" char=".">0</td>
<td align="center">1.40E-16</td>
<td align="char" char=".">0</td>
<td align="center">0.45</td>
<td align="char" char=".">0.36198393</td>
<td align="char" char=".">0</td>
<td align="char" char=".">0</td>
<td align="char" char=".">0.11465992</td>
</tr>
<tr>
<td align="left">
<bold>TOP3B</bold>
</td>
<td align="char" char=".">1</td>
<td align="char" char=".">1</td>
<td align="char" char=".">0</td>
<td align="center">8.77E-18</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.03472425</td>
<td align="char" char=".">0</td>
<td align="char" char=".">0</td>
<td align="char" char=".">
<bold>0.86898249</bold>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>Of particular interest is the fact that BLM has the highest vibration centre. The interpretation of this result is that BLM is the node most sensitive to stresses and/or stimuli, i.e., according to the vibrational centrality measure, it is the most vulnerable node in the network (<xref ref-type="bibr" rid="B27">Estrada and Hatano, 2010</xref>). This result is of particular interest in light of the crucial role this gene plays in the HR network. Indeed, the key role of BLM is well know, and alterations in this protein is linked to different diseases including cancer (<xref ref-type="bibr" rid="B55">Kaur et al., 2021</xref>). BLM is a 3&#x2032;-5&#x2032; ATP-dependent RecQ DNA helicase. It is a genome stabilizer playing an essential role in the DNA replication regulation, DNA recombination, and both homologous and non-homologous pathways of DSB repair. The high vulnerability of the BLM node to external stimuli and conditions suggests the need to identify which conditions and/or stimuli may be altering it, in order to preserve its proper functioning and/or to understand how it can be restored if it is altered. The high vulnerability of this node could also be explained by a recent study by <xref ref-type="bibr" rid="B55">Kaur et al. (2021</xref>). These authors report that BLM has a dual function both as a tumour suppressor and possibly as a proto-oncogene, being probably involved in the mechanisms of its deregulation in tumours.</p>
<p>The analysis also correctly identifies the SEM1 gene as a node with a high clustering coefficient. Indeed, as reported in (<xref ref-type="bibr" rid="B96">Safran et al., 2021</xref>; <xref ref-type="bibr" rid="B40">GeneCard, 2022</xref>), SEM1 gene encodes for a protein that is part of a 26S proteasome, which is a multiprotein complex with a function in the ATP-dependent degradation of ubiquitinated proteins. This complex contributes to the maintenance of protein homeostasis by removing misfolded or damaged proteins, which could jeopardize the healthy cellular functions, and by removing proteins no longer need. Therefore, 26S proteasome is involved in numerous cellular processes, including cell cycle progression, apoptosis, or DNA damage repair (<xref ref-type="bibr" rid="B99">Sone et al., 2004</xref>).</p>
<p>SEM1 was found also as a subunit in experiments of affinity purification of the yeast 19S proteasome, and its human homolog, DSS1, was found to copurify with the human 19S proteasome (<xref ref-type="bibr" rid="B63">Krogan et al., 2004</xref>). DSS1 is associated with the tumour suppressor protein BRCA2 involved in DNA DSBs repair. The authors in (<xref ref-type="bibr" rid="B63">Krogan et al., 2004</xref>) proved that SEM1 is essential for efficient repair of an HO-generated yeast DSB using both HR and nonhomologous end joining (NHEJ) pathways. Moreover, they showed that deletion of SEM1 contributes to cause defects in (synthetic) growth and hypersensitivity to genotoxins when combined with mutations in certain well-established genes involved in the DNA DSB repair.</p>
<p>Similarly to SEM1, the result of a high clustering coefficient is also expected for RPA4, as RPA4 is also part of a complex (<xref ref-type="bibr" rid="B58">Keshav et al., 1995</xref>). RPA4 gene encodes a single-stranded DNA-binding protein that is a subunit of the replication protein A complex (<xref ref-type="bibr" rid="B40">GeneCard, 2022</xref>). Replication protein A is essential for DNA DSB repair and plays a crucial role in the activation of cell cycle checkpoints. As regards the RPA complex, we have already seen in the previous sections that the RPA complex controls DNA repair and DNA damage checkpoint activation as well. In particular, the network analysis shows that RPA1 highly scores by total degree and betweenness. These results reflect the fact that RPA1 is an active route of communication exchanges between various nodes in the network. RPA1 is part of the heterotrimeric replication protein A complex (RPA/RP-A). It stabilizes single-stranded DNA intermediates, that form during DNA replication or upon DNA stress In (<xref ref-type="bibr" rid="B3">Bass et al., 2016</xref>; <xref ref-type="bibr" rid="B44">Haahr et al., 2016</xref>; <xref ref-type="bibr" rid="B52">Human Protein Atlas, 2022</xref>). It prevents the reannealing of single-stranded DNA intermediates and recruits and activates different proteins and complexes forming part of DNA metabolism. Thereby, it is a key protein both in DNA replication and in the cellular response to DNA damage (<xref ref-type="bibr" rid="B70">Lin et al., 1998</xref>). RPA2 shows high score for in-degree and eigenvevtor centrality, meaning that it is interacting with protein also highly scoring by eigenvector centrality and degree (<xref ref-type="bibr" rid="B45">Hansen et al., 2020</xref>), and thence with proteins which have a great influence in the HR network. Indeed RPA 2 gene has been found highly expressed in low grade carcinomas and its expression has a gradual significant decrease from stage I to stage IV carcinomas. All the three subunits RPA1, RPA2, and RPA3, were more abundant (with statistical significance evidence) in lymph node negative and earlier stage (stage I and II) gastric carcinomas (<xref ref-type="bibr" rid="B36">Fourtziala et al., 2020</xref>). Finally, of particular interest and the fact that RPA3 ranks first in terms of centrality out-degree, hub-centrality and sub-graph centrality. Since subgraph centrality of a node is the number of subgraphs a node participates in (weighted according to their size) (<xref ref-type="bibr" rid="B28">Estrada and Rodr&#xed;guez-Vel&#xe1;zquez, 2005</xref>), it means that RPA3 take part into a number of subgraphs of significant size relatively to the whole network size. From our analysis it results that RPA3 versus RPA1 and RPA2, although its roles are similar to those of RPA2, has thus a great influence on pathways of crucial importance more than on subset of unconnected nodes or single nodes.</p>
<p>The analysis also highlights RAD50 that is a component of the MRN complex The protein complex is involved in numerous enzymatic activities required for nonhomologous joining of DNA ends. It is protein is essential for DNA double-strand break repair, cell cycle checkpoint activation, telomere maintenance, and meiotic recombination. (<xref ref-type="bibr" rid="B12">Carney et al., 1998</xref>; <xref ref-type="bibr" rid="B24">de Jager et al., 2001</xref>; <xref ref-type="bibr" rid="B29">Estrada and Ross, 2018</xref>; <xref ref-type="bibr" rid="B7">Bian et al., 2019</xref>; <xref ref-type="bibr" rid="B4">Beikzadeh and Latham, 2021</xref>; <xref ref-type="bibr" rid="B82">National library of Medicine, 2022</xref>). This role is reflected by th ehigh sungraph centrality that measures the centrality of a node by taking into account the number of subgraphs the node participates in. Specifically, the subgraph centrality of a node is the number of closed loops originating at the node, where longer loops are exponentially downweighted. Consequently, subgraph centrality measures how close a node is to the other nodes in the network.</p>
<p>The results of this analysis reveal a correspondence between the measure of centrality and the role of the protein. On the basis of this, when the role of the protein is known, this information can be used to work out the correctness of the computational analysis. When, on the other hand, the role of the protein is not known, knowledge of its centrality measurements can suggest the type or set of types of possible roles.</p>
<p>In <xref ref-type="table" rid="T5">Tables 5</xref>, <xref ref-type="table" rid="T6">6</xref> we show the rate equations of the HR network dynamics generated as the automatic translation of the network (see the script dynamics.R in the GitLab repository of NADS software). In file Simulations_of_Dynamics_HR_pathway.pdf provided in the Supplementary Material, we show the time evolution curves of each node of the HR network obtained as a solution of the equations.</p>
<table-wrap id="T5" position="float">
<label>TABLE 5</label>
<caption>
<p>This is the PART I of the table of ordinary differential equations of the dynamics of HR network, in R code formalism. The <italic>k</italic> followed by a number denote the kinetic rate constant, and the letter &#x201c;d&#x201d; in front of the name of the proteins denote the temporal derivative of it concentration.</p>
</caption>
<table>
<tbody valign="top">
<tr>
<td align="center">
<inline-graphic xlink:href="FMOLB_fmolb-2022-878148_wc_tfx3.tif"/>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<table-wrap id="T6" position="float">
<label>TABLE 6</label>
<caption>
<p>This is the PART II (continuation) of the table of ordinary differential equations of the dynamics of HR network, in R code formalism. The <italic>k</italic> followed by a number denote the kinetic rate constant, and the letter &#x201c;d&#x201d; in front of the name of the proteins denote the temporal derivative of it concentration.</p>
</caption>
<table>
<tbody valign="top">
<tr>
<td align="center">
<inline-graphic xlink:href="FMOLB_fmolb-2022-878148_wc_tfx4.tif"/>
</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The parameter sensitivity analysis was conducted by perturbing each parameter in the convergence range of the solution and yielded the results shown in <xref ref-type="table" rid="T7">Table 7</xref>; <xref ref-type="fig" rid="F5">Figures 5</xref>, <xref ref-type="fig" rid="F6">6</xref>. In <xref ref-type="table" rid="T7">Table 7</xref> we report the kinetic rate constants for which the sensitivity index belongs ot the 98th percentile of the sensitivity index distribution. They correspond to the most sensitive parameters, i.e. to the interactions whose alterations can significantly alter the dynamics of the network. To find out which interactions they refer to, the reader can refer to the <xref ref-type="sec" rid="s11">Supplementary Tables S1&#x2013;S3</xref>. <xref ref-type="fig" rid="F5">Figure 5</xref> we shows that MRE11, followed by POLD1, BLM has the highest average sensitivity index. In <xref ref-type="fig" rid="F6">Figure 6</xref> we show the coefficient of variation of each protein in the HR network. The coefficient of variation, being the ratio of the standard deviation to the mean, measures the extent of variability in relation to the mean of the population. The higher the coefficient of variation, the greater the dispersion. BLM, followed by MRE11 and RPA2 exhibits the lowest coefficient of variation of the sensitivity index. This mean that BLM, MRE11 and RPA2 have high sensitivity indices, and that the distribution of the sensitivity indices is well shaped around its mean, i.e. these protein exhibit almost the same sensitivity for all the parameters of the model. In this study we have therefore found that the BLM and RPA2 are sensitive nodes and that their sensitivity has two components: a topological sensitivity expressed by vibrational centrality, eigenvector centrality and clustering coefficient, and a dynamic sensitivity expressed by the parameter sensitivity index.</p>
<table-wrap id="T7" position="float">
<label>TABLE 7</label>
<caption>
<p>For each gene/protein in the HR pathway in (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>) we selected the kinetic rates whose sensitivity index belongs to the 98th percentile of the sensitivity index distribution. The sensitity index is calculated using the <xref ref-type="disp-formula" rid="e1">formula (1)</xref>.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Gene</th>
<th align="center">Kinetic rate to which it is highly sensitive</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">BLM</td>
<td align="center">k12, k34, k107, k138, k222</td>
</tr>
<tr>
<td align="left">BRCA2</td>
<td align="center">k13, k58, k108, k139, k250</td>
</tr>
<tr>
<td align="left">EME1</td>
<td align="center">k24, k138, k140, k144, k227</td>
</tr>
<tr>
<td align="left">MRE11</td>
<td align="center">k14, k34, k109, k204, k223</td>
</tr>
<tr>
<td align="left">MUS81</td>
<td align="center">k24, k138, k140, k144, k227</td>
</tr>
<tr>
<td align="left">NBN</td>
<td align="center">k15, k32, k34, k60, k110</td>
</tr>
<tr>
<td align="left">POLD1</td>
<td align="center">k72, k73, k89, k90, k91</td>
</tr>
<tr>
<td align="left">POLD2</td>
<td align="center">k72, k73, k89, k90, k91</td>
</tr>
<tr>
<td align="left">POLD3</td>
<td align="center">k72, k89, k90, k91, k122</td>
</tr>
<tr>
<td align="left">POLD4</td>
<td align="center">k73, k89, k90, k91, k122</td>
</tr>
<tr>
<td align="left">RAD50</td>
<td align="center">k16, k61, k78, k111, k137</td>
</tr>
<tr>
<td align="left">RAD51</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">RAD51B</td>
<td align="center">k18, k63, k113, k140, k163</td>
</tr>
<tr>
<td align="left">RAD51C</td>
<td align="center">k19, k64, k81, k114, k157</td>
</tr>
<tr>
<td align="left">RAD51D</td>
<td align="center">k20, k65, k115, k141, k162</td>
</tr>
<tr>
<td align="left">RAD52</td>
<td align="center">k142, k168, k222, k227, k228</td>
</tr>
<tr>
<td align="left">RPA1</td>
<td align="center">k8, k29, k66, k83, k116</td>
</tr>
<tr>
<td align="left">RPA2</td>
<td align="center">k30, k33, k117, k144, k206</td>
</tr>
<tr>
<td align="left">RPA3</td>
<td align="center">k31, k68, k118, k222, k227</td>
</tr>
<tr>
<td align="left">RPA4</td>
<td align="center">k29, k227, k232, k233, k234</td>
</tr>
<tr>
<td align="left">SEM1</td>
<td align="center">k139, k145, k235, k236, k250</td>
</tr>
<tr>
<td align="left">TOP3A</td>
<td align="center">k21, k69, k86, k119, k248</td>
</tr>
<tr>
<td align="left">TOP3B</td>
<td align="center">k29, k66, k83, k116, k188</td>
</tr>
<tr>
<td align="left">XRCC2</td>
<td align="center">k22, k70, k120, k146, k149</td>
</tr>
<tr>
<td align="left">XRCC3</td>
<td align="center">k23, k121, k147, k166, k250</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Mean of the sensitivity index distributions for the proteins in HR network (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>). These results refer to simulation in the time interval [0, 10] a.u., and initial values of the proteins randomly sampled in the range [1, 100] a. u. and kinetics rates values sampled in the interval [0, 0.01].</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g005.tif"/>
</fig>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Coefficient of variation of the sensitivity index distributions for the proteins in HR network <xref ref-type="bibr" rid="B85">Orlic-Milacic, (2015)</xref>. These results refer to simulation in the time interval [0, 10] a.u., and initial values of the proteins randomly sampled in the range [1, 100] a. u. and kinetics rates values sampled in the interval [0, 0.01].</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g006.tif"/>
</fig>
<p>As with the BLM and RPA2 proteins, sensitivity analysis also highlights the MRE11 protein, which is highly sensitive to kinetic parameters, and its vibrational centrality is 1.0587524, very close to the maximum value exhibited by BLM (see <xref ref-type="table" rid="T4">Table 4</xref>). Its eigenvector centrality is 0.7397 which, although not the maximum, is very close to it (see <xref ref-type="table" rid="T4">Table 4</xref>). Indeed, MRE11 is an integral part of the protein complex of RAD50-MRE11A-NBS1 known as the MRN complex (<xref ref-type="bibr" rid="B90">Porras, 2014</xref>; <xref ref-type="bibr" rid="B98">Shibata et al., 2014</xref>; <xref ref-type="bibr" rid="B81">Mukherjee et al., 2019</xref>). It plays a key role in homologous recombination, and it is generally believed that MRE11 initiates double-strand breaks resection. In particular, the authors show that the loss of MRE11 reduces the efficiency of homologous recombination in human TK6 cells without affecting double-strand breaks resection, indicating a role for MRE11 in homologous recombination also at a post-resection step.</p>
<p>The high value of the eigenvector centrality fork BLM, RPA2 and MRE11 confirms the crucial role of these proteins in the network and expresses the fact that they are pointed by nodes that have a high value of the eigenvector centrality too. Indeed, if a node is pointed to by many nodes (which also have high eigenvector centrality) then that node will have high eigenvector centrality (<xref ref-type="bibr" rid="B33">Fletcher and Wennekers, 2018</xref>). The high sensitivity to the parameters characterising the dynamics of the interactions between these proteins and the partners pointing to them indicates the great influence that these partner nodes have on these proteins. Interestingly, RAD51 does not result sensitive to any parameter. The RAD51 encodes a protein that is essential for repairing damaged DNA. Recent findings have indicated RAD51 protein is overexpressed in a variety of tumours <xref ref-type="bibr" rid="B19">Chen et al. (2017)</xref>. The overexpression of RAD51 causes improper and hyper-recombination, and thus contributes to genomic instability and genetic diversity. Genomic instability might, in turn, drive regular cells towards neoplastic transformation or further contributes to cancer metastatic progression (<xref ref-type="bibr" rid="B18">Chen et al., 2007</xref>). The RAD51 protein binds to the DNA at the site of a break and encapsulates it in a protein sheath, initiating the repair process <xref ref-type="bibr" rid="B80">MedlinePlus (2022)</xref>; <xref ref-type="bibr" rid="B103">Uniprot (2022)</xref>. RAD51 protein interacts with BRCA1 and BRCA2, to fix damaged DNA. The BRCA2 protein regulates the activity of the RAD51 protein by transporting it in the nucleus to sites of DNA damage. Although the interaction between the BRCA1 protein and the RAD51 protein has still to be elucidate, research suggests that BRCA1 may also activate RAD51 in response to DNA damage (<xref ref-type="bibr" rid="B22">Cousineau et al., 2005</xref>; <xref ref-type="bibr" rid="B16">Chappell et al., 2016</xref>). The result of the sensitivity analysis found seems to contradict the important role of this protein in these interactions. Indeed, for example, one might expect a high sensitivity of RAD51 to the k139 due to its interaction with BRCA2 (see <xref ref-type="sec" rid="s11">Supplementary Table S2</xref>). One explanation for this contradiction could be that since the mechanisms of interaction of RAD51 with these proteins are not fully known, the model used in this study could be an oversimplification of the interaction of RAD51 with its partners. If more accurate models in the future confirm the low sensitivity of RAD51 to the parameters of the rate equations describing the dynamics of the network, it will be necessary to investigate the physical and biological characteristics that make it so stable to perturbations. The fact that RAD51 has a low value of vibrational centrality in this study is a factor in favour of the possible confirmation of this case.</p>
<p>In <xref ref-type="fig" rid="F7">Figures 7</xref>, <xref ref-type="fig" rid="F8">8</xref> we report the results of the sensitivity analysis obtained selecting different ranges of initial conditions and parameters values. The plots highlights RAD51C, MRE11, RAD50 and BRCA2 as the most sensitive nodes to the parameters. We comment in the Section Remarks the expected differences and similarities in the results of sensitivity analysis when we change the intervals of initial conditions and parameters.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Mean of the sensitivity index distributions for the proteins in HR network <xref ref-type="bibr" rid="B85">Orlic-Milacic, (2015)</xref>. These results refer to simulation in the time interval [0, 1400] a.u., and initial values of the proteins randomly sampled in the range [18, 20] a. u. and kinetics rate values sample in [10<sup>&#x2013;5</sup>, 10<sup>&#x2013;6</sup>] a. u.</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g007.tif"/>
</fig>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>Coefficient of variation of the sensitivity index distributions for the proteins in HR network (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>). These results refer to simulation in the time interval [18, 20] a.u., and initial values of the proteins randomly sampled in the range [10<sup>&#x2013;5</sup>, 10<sup>&#x2013;6</sup>] a. u.</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g008.tif"/>
</fig>
<sec id="s4-1">
<title>4.1 Analysis of the HR Pathway Merged With FANCM Pathway</title>
<p>We repeated the analysis on the HR&#x2019;s network extended by adding the pathways of FANCM gene (Fanconi Anaemia Group M Protein), obtained from Pathways Commons (<xref ref-type="bibr" rid="B88">Pathways Commons, 2022</xref>) given its important role in genome duplication, repair mechanisms and its involvement in the development of Fanconi anaemia, which several studies report to be a syndrome related to cancer predisposition (<xref ref-type="bibr" rid="B25">Deans and West, 2009</xref>; <xref ref-type="bibr" rid="B110">Xue et al., 2015</xref>; <xref ref-type="bibr" rid="B6">Bhattacharjee and Nandi, 2017</xref>; <xref ref-type="bibr" rid="B86">Pan et al., 2017</xref>; <xref ref-type="bibr" rid="B105">Wang et al., 2018</xref>). Finally, a recent study of Panday et al. reports that FANCM regulates repair pathway choice at stalled replication forks (<xref ref-type="bibr" rid="B72">Ling et al., 2016</xref>; <xref ref-type="bibr" rid="B87">Panday et al., 2021</xref>). FANCM and BLM have a similar role and cooperatively act in the DNA repair mechanisms (<xref ref-type="bibr" rid="B87">Panday et al., 2021</xref>), and through this analysis we want to investigate on this similarity.</p>
<p>The new network including HR and FANCM pathways is made up of 46 nodes and 316 edges. The left part of <xref ref-type="fig" rid="F4">Figure 4</xref> shows the FANCM pathway and its connection with HR network. As reported in <xref ref-type="table" rid="T8">Table 8</xref>, the calculation of centrality measures led to the following results:<list list-type="simple">
<list-item>
<p>&#x2022; BLM has the highest score in vibrational centrality</p>
</list-item>
<list-item>
<p>&#x2022; FANCM has the highest score in total degree, in degree and betweenness</p>
</list-item>
<list-item>
<p>&#x2022; RAD50 scores first for subgraph centrality</p>
</list-item>
<list-item>
<p>&#x2022; RAD52 scores first for clustering coefficient</p>
</list-item>
<list-item>
<p>&#x2022; RPA1 scores first for out-degree</p>
</list-item>
<list-item>
<p>&#x2022; RPA2 scores first for eigenvector centrality</p>
</list-item>
<list-item>
<p>&#x2022; RPA3 scores first for hub centrality</p>
</list-item>
<list-item>
<p>&#x2022; RPA4 scores first for clustering coefficient</p>
</list-item>
<list-item>
<p>&#x2022; SEM1 scores first for clustering coefficient.</p>
</list-item>
</list>
</p>
<table-wrap id="T8" position="float">
<label>TABLE 8</label>
<caption>
<p>Values of the centrality measures for the HR pathway in (Orlic-Milacic, 2015) merged with the FANCM pathway in (Pathways Commons, 2022). In bold, we marked the genes with the highest scores.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Protein</th>
<th align="center">Total degree</th>
<th align="center">In-degree</th>
<th align="center">Out-degree</th>
<th align="center">Hub centrality</th>
<th align="center">Betweenness</th>
<th align="center">Clustering coefficient</th>
<th align="center">Eigenvector centrality</th>
<th align="center">Vibrational centrality</th>
<th align="center">Subgraph centrality</th>
<th align="center">Information centrality</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">BLM</td>
<td align="char" char=".">32</td>
<td align="char" char=".">19</td>
<td align="char" char=".">13</td>
<td align="center">4.83E-01</td>
<td align="char" char=".">117.0805289</td>
<td align="center">0.72058824</td>
<td align="char" char=".">0.83056114</td>
<td align="center">
<bold>1.107752</bold>
</td>
<td align="char" char=".">7408.39241</td>
<td align="char" char=".">0.1204394</td>
</tr>
<tr>
<td align="left">EME1</td>
<td align="char" char=".">15</td>
<td align="char" char=".">0</td>
<td align="char" char=".">15</td>
<td align="center">5.92E-01</td>
<td align="char" char=".">0</td>
<td align="center">0.48351648</td>
<td align="char" char=".">0.28101096</td>
<td align="center">9.68E-01</td>
<td align="char" char=".">2727.280253</td>
<td align="char" char=".">0.1730775</td>
</tr>
<tr>
<td align="left">MRE11</td>
<td align="char" char=".">26</td>
<td align="char" char=".">16</td>
<td align="char" char=".">10</td>
<td align="center">3.71E-01</td>
<td align="char" char=".">9.2926175</td>
<td align="center">0.82051282</td>
<td align="char" char=".">0.73943396</td>
<td align="center">1.08E&#x2b;00</td>
<td align="char" char=".">6025.93013</td>
<td align="char" char=".">0.1319644</td>
</tr>
<tr>
<td align="left">MUS81</td>
<td align="char" char=".">13</td>
<td align="char" char=".">1</td>
<td align="char" char=".">12</td>
<td align="center">5.18E-01</td>
<td align="char" char=".">0</td>
<td align="center">0.53846154</td>
<td align="char" char=".">0.25936455</td>
<td align="center">9.56E-01</td>
<td align="char" char=".">2292.062046</td>
<td align="char" char=".">0.1868928</td>
</tr>
<tr>
<td align="left">NBN</td>
<td align="char" char=".">27</td>
<td align="char" char=".">17</td>
<td align="char" char=".">10</td>
<td align="center">3.69E-01</td>
<td align="char" char=".">9.2926175</td>
<td align="center">0.82051282</td>
<td align="char" char=".">0.76658977</td>
<td align="center">1.08E&#x2b;00</td>
<td align="char" char=".">6025.93013</td>
<td align="char" char=".">0.1296602</td>
</tr>
<tr>
<td align="left">POLD1</td>
<td align="char" char=".">26</td>
<td align="char" char=".">9</td>
<td align="char" char=".">17</td>
<td align="center">6.82E-01</td>
<td align="char" char=".">7.8121197</td>
<td align="center">0.76470588</td>
<td align="char" char=".">0.67199489</td>
<td align="center">9.86E-01</td>
<td align="char" char=".">7688.630996</td>
<td align="char" char=".">0.1322165</td>
</tr>
<tr>
<td align="left">POLD2</td>
<td align="char" char=".">23</td>
<td align="char" char=".">5</td>
<td align="char" char=".">18</td>
<td align="center">7.10E-01</td>
<td align="char" char=".">5.8377525</td>
<td align="center">0.76470588</td>
<td align="char" char=".">0.57047643</td>
<td align="center">9.81E-01</td>
<td align="char" char=".">9071.417868</td>
<td align="char" char=".">0.1400556</td>
</tr>
<tr>
<td align="left">POLD3</td>
<td align="char" char=".">23</td>
<td align="char" char=".">8</td>
<td align="char" char=".">15</td>
<td align="center">6.44E-01</td>
<td align="char" char=".">5.8377525</td>
<td align="center">0.76470588</td>
<td align="char" char=".">0.57047643</td>
<td align="center">9.78E-01</td>
<td align="char" char=".">5524.141817</td>
<td align="char" char=".">0.1396592</td>
</tr>
<tr>
<td align="left">POLD4</td>
<td align="char" char=".">23</td>
<td align="char" char=".">7</td>
<td align="char" char=".">16</td>
<td align="center">6.65E-01</td>
<td align="char" char=".">5.8377525</td>
<td align="center">0.76470588</td>
<td align="char" char=".">0.57047643</td>
<td align="center">9.80E-01</td>
<td align="char" char=".">6516.909994</td>
<td align="char" char=".">0.1397968</td>
</tr>
<tr>
<td align="left">
<bold>RAD50</bold>
</td>
<td align="char" char=".">27</td>
<td align="char" char=".">13</td>
<td align="char" char=".">14</td>
<td align="center">5.81E-01</td>
<td align="char" char=".">10.2729789</td>
<td align="center">0.81318681</td>
<td align="char" char=".">0.75778635</td>
<td align="center">1.04E&#x2b;00</td>
<td align="char" char=".">
<bold>11437.382893</bold>
</td>
<td align="char" char=".">0.1300547</td>
</tr>
<tr>
<td align="left">RAD51</td>
<td align="char" char=".">23</td>
<td align="char" char=".">12</td>
<td align="char" char=".">11</td>
<td align="center">4.02E-01</td>
<td align="char" char=".">30.3997662</td>
<td align="center">0.65497076</td>
<td align="char" char=".">0.4937734</td>
<td align="center">9.17E-01</td>
<td align="char" char=".">1403.106256</td>
<td align="char" char=".">0.1386277</td>
</tr>
<tr>
<td align="left">RAD51B</td>
<td align="char" char=".">14</td>
<td align="char" char=".">12</td>
<td align="char" char=".">2</td>
<td align="center">8.53E-02</td>
<td align="char" char=".">0.3636364</td>
<td align="center">0.82051282</td>
<td align="char" char=".">0.31833841</td>
<td align="center">1.01E&#x2b;00</td>
<td align="char" char=".">74.55065</td>
<td align="char" char=".">0.1774293</td>
</tr>
<tr>
<td align="left">RAD51C</td>
<td align="char" char=".">21</td>
<td align="char" char=".">9</td>
<td align="char" char=".">12</td>
<td align="center">4.93E-01</td>
<td align="char" char=".">1.6614219</td>
<td align="center">0.81904762</td>
<td align="char" char=".">0.47562207</td>
<td align="center">9.12E-01</td>
<td align="char" char=".">1911.911354</td>
<td align="char" char=".">0.1453357</td>
</tr>
<tr>
<td align="left">RAD51D</td>
<td align="char" char=".">16</td>
<td align="char" char=".">11</td>
<td align="char" char=".">5</td>
<td align="center">2.13E-01</td>
<td align="char" char=".">0.5127787</td>
<td align="center">0.81904762</td>
<td align="char" char=".">0.3597479</td>
<td align="center">9.38E-01</td>
<td align="char" char=".">282.219746</td>
<td align="char" char=".">0.1656386</td>
</tr>
<tr>
<td align="left">RAD52</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">1.00E-01</td>
<td align="char" char=".">0</td>
<td align="center">
<bold>1</bold>
</td>
<td align="char" char=".">0.12449815</td>
<td align="center">9.63E-01</td>
<td align="char" char=".">254.418337</td>
<td align="char" char=".">0.3917785</td>
</tr>
<tr>
<td align="left">
<bold>RPA1</bold>
</td>
<td align="char" char=".">43</td>
<td align="char" char=".">20</td>
<td align="char" char=".">
<bold>23</bold>
</td>
<td align="center">9.74E-01</td>
<td align="char" char=".">215.4152627</td>
<td align="center">0.49802372</td>
<td align="char" char=".">0.91307865</td>
<td align="center">9.47E-01</td>
<td align="char" char=".">8620.183617</td>
<td align="char" char=".">0.1074375</td>
</tr>
<tr>
<td align="left">
<bold>RPA2</bold>
</td>
<td align="char" char=".">41</td>
<td align="char" char=".">22</td>
<td align="char" char=".">19</td>
<td align="center">8.45E-01</td>
<td align="char" char=".">32.6964097</td>
<td align="center">0.64210526</td>
<td align="char" char=".">
<bold>1</bold>
</td>
<td align="center">9.82E-01</td>
<td align="char" char=".">8511.793141</td>
<td align="char" char=".">0.1095086</td>
</tr>
<tr>
<td align="left">
<bold>RPA3</bold>
</td>
<td align="char" char=".">34</td>
<td align="char" char=".">11</td>
<td align="char" char=".">23</td>
<td align="center">
<bold>1</bold>
</td>
<td align="char" char=".">25.979693</td>
<td align="center">0.64210526</td>
<td align="char" char=".">0.81828849</td>
<td align="center">9.98E-01</td>
<td align="char" char=".">14877.81448</td>
<td align="char" char=".">0.1182323</td>
</tr>
<tr>
<td align="left">
<bold>RPA4</bold>
</td>
<td align="char" char=".">3</td>
<td align="char" char=".">0</td>
<td align="char" char=".">3</td>
<td align="center">1.27E-01</td>
<td align="char" char=".">0</td>
<td align="center">
<bold>1</bold>
</td>
<td align="char" char=".">0.10543731</td>
<td align="center">9.63E-01</td>
<td align="char" char=".">700.745966</td>
<td align="char" char=".">0.4815787</td>
</tr>
<tr>
<td align="left">
<bold>SEM1</bold>
</td>
<td align="char" char=".">3</td>
<td align="char" char=".">1</td>
<td align="char" char=".">2</td>
<td align="center">9.07E-02</td>
<td align="char" char=".">0</td>
<td align="center">
<bold>1</bold>
</td>
<td align="char" char=".">0.0682632</td>
<td align="center">9.28E-01</td>
<td align="char" char=".">64.063815</td>
<td align="char" char=".">0.4810717</td>
</tr>
<tr>
<td align="left">
<bold>TOP3A</bold>
</td>
<td align="char" char=".">26</td>
<td align="char" char=".">12</td>
<td align="char" char=".">14</td>
<td align="center">5.39E-01</td>
<td align="char" char=".">43.5259509</td>
<td align="center">0.73626374</td>
<td align="char" char=".">0.70171805</td>
<td align="center">1.04E&#x2b;00</td>
<td align="char" char=".">8739.804106</td>
<td align="char" char=".">0.1322725</td>
</tr>
<tr>
<td align="left">XRCC2</td>
<td align="char" char=".">15</td>
<td align="char" char=".">14</td>
<td align="char" char=".">1</td>
<td align="center">5.59E-02</td>
<td align="char" char=".">0.8476272</td>
<td align="center">0.82417582</td>
<td align="char" char=".">0.3492084</td>
<td align="center">1.03E&#x2b;00</td>
<td align="char" char=".">55.032467</td>
<td align="char" char=".">0.1704502</td>
</tr>
<tr>
<td align="left">XRCC3</td>
<td align="char" char=".">13</td>
<td align="char" char=".">12</td>
<td align="char" char=".">1</td>
<td align="center">4.65E-02</td>
<td align="char" char=".">0.3333333</td>
<td align="center">0.80769231</td>
<td align="char" char=".">0.28356645</td>
<td align="center">5.52E-01</td>
<td align="char" char=".">0</td>
<td align="char" char=".">0.1844967</td>
</tr>
<tr>
<td align="left">BRCA1</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.53E-01</td>
<td align="char" char=".">15.252907</td>
<td align="char" char=".">0.6489791</td>
</tr>
<tr>
<td align="left">CENPS</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.53E-01</td>
<td align="char" char=".">15.252907</td>
<td align="char" char=".">0.6489791</td>
</tr>
<tr>
<td align="left">CENPX</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.53E-01</td>
<td align="char" char=".">15.252907</td>
<td align="char" char=".">0.6489791</td>
</tr>
<tr>
<td align="left">EME2</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.53E-01</td>
<td align="char" char=".">15.252907</td>
<td align="char" char=".">0.6489791</td>
</tr>
<tr>
<td align="left">FAAP100</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.04496402</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.3943335</td>
</tr>
<tr>
<td align="left">FAAP20</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.53E-01</td>
<td align="char" char=".">15.252907</td>
<td align="char" char=".">0.6489791</td>
</tr>
<tr>
<td align="left">FAAP24</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.53E-01</td>
<td align="char" char=".">15.252907</td>
<td align="char" char=".">0.6489791</td>
</tr>
<tr>
<td align="left">FANCA</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.04496402</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.3943335</td>
</tr>
<tr>
<td align="left">FANCB</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.04496402</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.3943335</td>
</tr>
<tr>
<td align="left">FANCC</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.04496402</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.3943335</td>
</tr>
<tr>
<td align="left">FANCD2</td>
<td align="char" char=".">2</td>
<td align="char" char=".">1</td>
<td align="char" char=".">1</td>
<td align="center">3.59E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.77E-01</td>
<td align="char" char=".">3.563227</td>
<td align="char" char=".">0.6504898</td>
</tr>
<tr>
<td align="left">FANCE</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.04496402</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.3943335</td>
</tr>
<tr>
<td align="left">FANCF</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.04496402</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.3943335</td>
</tr>
<tr>
<td align="left">FANCG</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.04496402</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.3943335</td>
</tr>
<tr>
<td align="left">FANCI</td>
<td align="char" char=".">3</td>
<td align="char" char=".">1</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.03372301</td>
<td align="center">9.77E-01</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.4827827</td>
</tr>
<tr>
<td align="left">FANCL</td>
<td align="char" char=".">4</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.04496402</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">14.252907</td>
<td align="char" char=".">0.3943335</td>
</tr>
<tr>
<td align="left">
<bold>FANCM</bold>
</td>
<td align="char" char=".">
<bold>66</bold>
</td>
<td align="char" char=".">
<bold>44</bold>
</td>
<td align="char" char=".">22</td>
<td align="center">4.35E-16</td>
<td align="char" char=".">
<bold>481</bold>
</td>
<td align="center">0.01811594</td>
<td align="char" char=".">0.29119966</td>
<td align="center">5.13E-01</td>
<td align="char" char=".">131.839388</td>
<td align="char" char=".">0.0955692</td>
</tr>
<tr>
<td align="left">RMI1</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.53E-01</td>
<td align="char" char=".">15.252907</td>
<td align="char" char=".">0.6489791</td>
</tr>
<tr>
<td align="left">RMI2</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="char" char=".">2</td>
<td align="center">7.17E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">9.53E-01</td>
<td align="char" char=".">15.252907</td>
<td align="char" char=".">0.6489791</td>
</tr>
<tr>
<td align="left">UBE2T</td>
<td align="char" char=".">3</td>
<td align="char" char=".">2</td>
<td align="char" char=".">1</td>
<td align="center">3.59E-02</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.03372301</td>
<td align="center">1.00E&#x2b;00</td>
<td align="char" char=".">3.563227</td>
<td align="char" char=".">0.4815848</td>
</tr>
<tr>
<td align="left">BRCA2</td>
<td align="char" char=".">16</td>
<td align="char" char=".">16</td>
<td align="char" char=".">0</td>
<td align="center">1.09E-16</td>
<td align="char" char=".">0</td>
<td align="center">0.69230769</td>
<td align="char" char=".">0.36151501</td>
<td align="center">-4.08E-18</td>
<td align="char" char=".">0</td>
<td align="char" char=".">0.1645300</td>
</tr>
<tr>
<td align="left">TOP3B</td>
<td align="char" char=".">1</td>
<td align="char" char=".">1</td>
<td align="char" char=".">0</td>
<td align="center">6.80E-18</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.03524702</td>
<td align="center">0.00E&#x2b;00</td>
<td align="char" char=".">0</td>
<td align="char" char=".">
<bold>1.1169817</bold>
</td>
</tr>
<tr>
<td align="left">HES1</td>
<td align="char" char=".">2</td>
<td align="char" char=".">2</td>
<td align="char" char=".">0</td>
<td align="center">1.36E-17</td>
<td align="char" char=".">0</td>
<td align="center">NA</td>
<td align="char" char=".">0.02248201</td>
<td align="center">0.00E&#x2b;00</td>
<td align="char" char=".">0</td>
<td align="char" char=".">0.6438225</td>
</tr>
<tr>
<td align="left">MAX SCORE</td>
<td align="char" char=".">43</td>
<td align="char" char=".">22</td>
<td align="char" char=".">23</td>
<td align="center">0.9743705</td>
<td align="char" char=".">215.4152627</td>
<td align="center">0.82417582</td>
<td align="char" char=".">0.91307865</td>
<td align="center">1.08361</td>
<td align="char" char=".">14877.81448</td>
<td align="char" char=".">0</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The distribution of the centrality measures on the entire network is shown in <xref ref-type="fig" rid="F9">Figure 9</xref>. These results not only re-emphasise as central the genes/proteins already identified in the analysis of the HR network alone in (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>), but also highlight the central role of FANCM and as a node of particular relevance due to their high in-degree and high betweenness. By assigning an initial quantity between 18 and 20 (expressed in arbitrary units) to each node, the solution of the system of 46 differential equations converges for values of rate constants in the range 10<sup>&#x2013;4</sup> and 10<sup>&#x2013;5</sup> a.u. In file Simulations_of_Dynamics_HR_FANCM_pathway.pdf provided in the Supplementary Material, we show the time evolution curves (obtained as a solution of the equations) of each node of the HR pathway merged with FANCM pathway. The parameter sensitivity analysis was conducted by perturbing each parameter in the convergence range of the solution and yielded the results shown in <xref ref-type="fig" rid="F10">Figures 10</xref>, <xref ref-type="fig" rid="F11">11</xref>. We found that the nodes most sensitive to the parameters are RAD50, NBN, BRCA2, MRE11 and RAD51B. Compared to what was obtained in the analysis of the HR network alone, we find here that BLM is no longer at the top in terms of parameter sensitivity while still maintaining a central role in terms of vibration centrality.</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>Distributions of the centrality measures of HR pathway (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>) merged with FANCM pathway (<xref ref-type="bibr" rid="B88">Pathways Commons, 2022</xref>). We observe that the majority of node have low betweenness, and high vibrational centrality.</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g009.tif"/>
</fig>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>Mean of the sensitivity index distributions for the proteins in HR network <xref ref-type="bibr" rid="B85">Orlic-Milacic, (2015)</xref> merged with FANCM pathway (<xref ref-type="bibr" rid="B88">Pathways Commons, 2022</xref>). These results refer to simulation in the time interval [0, 1400] a.u., and initial values of the proteins randomly sampled in the range [18, 20] a. u. and kinetics rate values sample in [10<sup>&#x2013;5</sup>, 10<sup>&#x2013;6</sup>] a. u.</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g010.tif"/>
</fig>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>Coefficient of variation of the sensitivity index distributions for the proteins in HR network (<xref ref-type="bibr" rid="B85">Orlic-Milacic, 2015</xref>) merged with FANCM pathway (<xref ref-type="bibr" rid="B88">Pathways Commons, 2022</xref>). These results refer to simulation in the time interval [18, 20] a.u., and initial values of the proteins randomly sampled in the range [10<sup>&#x2013;5</sup>, 10<sup>&#x2013;6</sup>] a. u.</p>
</caption>
<graphic xlink:href="fmolb-09-878148-g011.tif"/>
</fig>
</sec>
<sec id="s4-2">
<title>4.2 Remarks</title>
<p>The method provides a range of values for the rate constants within which the solution to the problem exists at the given set of initial values for the node concentration/abundance. We can interpret this range as that of the &#x2018;most probable&#x2019; range of values if.<list list-type="simple">
<list-item>
<p>&#x2022; the initial conditions are known</p>
</list-item>
<list-item>
<p>&#x2022; the analysed network does not exclude important interactions occurring <italic>in vivo</italic> and if the system is subjected to the conditions of the real system <italic>in vitro</italic> and <italic>in vivo</italic>. The network considered is only an extract of a much more complex network (still not completely known) that operates <italic>in vivo</italic> and in interaction with environmental factors.</p>
</list-item>
</list>
</p>
<p>We also note that we do not dispose of experimental time curves that can be used to calibrate the model. Calibration from experimental data rather than sensitivity analysis would be the most appropriate method to use to obtain an estimated (even interval) parameter estimate. In the absence of both experimental data. We agree with the Reviewer that sensitivity analysis provides information on the minimum set of parameters to be inferred from experimental data, since the parameters to which the model is less sensitive are less influential.</p>
<p>Finally, we also observe that having fixed a set of initial values for the concentrations/abundances of the network components, more than one set of intervals for the rate constants could guarantee the convergence of the numerical method of solving the system of differential equations. It is also true that by changing the initial values of the concentrations, the range of values of the rate constants for which the system converges could change. The results that we report in this new version of the manuscript show, for example, that if the range of the initial concentration values is between 0 and 100, the numerical solution is found for rate constant values between 0 and 0.01, whereas if the range of the initial concentration values is a few tens, the numerical solution is found for rate constant values between 10<sup>&#x2013;6</sup> and 106&#x2013;5. A reduction of 10 in the order of magnitude of the initial concentration values thus corresponds to a reduction of 10<sup>&#x2013;3</sup> in the order of magnitude of the rate constants. This is an indication that the system is underdetermined, and in fact consists of more parameters than the number of variables and in the complete absence of experimental data. All this also shows that calibrating the model in the light of experimental data is the best way to hope for a set of &#x2018;probable&#x2019; values of the rate constants.</p>
<p>The work shown in this study therefore does not so much emphasise the numerical solutions, but, through a mathematical model, wants to test the susceptibility of the network components to the parameters and wants to integrate it with the role that the network components have (estimated by the centrality measurements).</p>
</sec>
</sec>
<sec id="s5">
<title>5 Conclusion</title>
<p>This report presented an application of network analysis and mathematical modelling to the double-strand break repair pathway homologous recombination repair (HR). The complexity of the network of repair mechanisms itself, as well as the complexity of its interactions with the surrounding environment (<xref ref-type="bibr" rid="B69">Li et al., 2009</xref>; <xref ref-type="bibr" rid="B17">Chatterjee and Walker, 2017</xref>; <xref ref-type="bibr" rid="B64">Kusakabe et al., 2019</xref>; <xref ref-type="bibr" rid="B89">Poetsch, 2020</xref>; <xref ref-type="bibr" rid="B95">Roux et al., 2021</xref>), and the mutations of its components make its mathematical modelling particularly difficult, especially when based on rate equations. It is therefore of great necessity to have a tool that can implement these two important steps:<list list-type="simple">
<list-item>
<p>1. network analysis including standard centrality measures and new measures to quantify the robustness and responsiveness of the network to stimuli and stresses not dependent on the network topology</p>
</list-item>
<list-item>
<p>2. automatic construction of a mathematical model, for its analysis, and which allows to carry out refinements and modifications, when new data and new experimental knowledge make it necessary.</p>
</list-item>
</list>
</p>
<p>The implementation of these step is an innovative perspective for the analysis of DNA repair mechanisms. So far in the literature, there are many studies and analyses focused on the genetic and genomic aspects of the pathways, but studies on the mathematical modelling of its dynamics are absent. Our study therefore aims to fill this gap, since the mechanisms of DNA repair are governed by genes, proteins and pathways in continuous communication with the environment. For this reason, the analysis of the dynamics of the network is particularly useful, since it can quantify the vulnerability of the network and the modes of response to stimuli and exogenous stress. To the best of our knowledge there are no schemes for translating a graph associated with a biological network into a set of dynamic equations. The main reason for this is that there is no unambiguously defined semantics of a graphic representation of a biological network, i.e. there is no unambiguous definition of the graphic symbolism in terms of the mathematical equation describing the interaction indicated by that symbolism. The translation model we propose in this study is a basic model that describes the interactions indicated by the graph with linear first-order differential equations in the parameters. The code that implements this translation, however, gives the user the possibility to modify the model where he/she deems it appropriate in the light of available biological knowledge, or in the case he/she like to generate new hypothetical scenarios. We believe that the availability of a tool such as NADS can support the investigation of such a complex network that is subject to continuous interaction with external agents, not only to understand its dynamics, but also to predict its evolution and identify points of vulnerability for the benefit of the medical applications that this research may provide.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s6">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="sec" rid="s11">Supplementary Material</xref>, further inquiries can be directed to the corresponding authors. the software used int eh analysis is available at <ext-link ext-link-type="uri" xlink:href="https://gitlab.inf.unibz.it/Paola.Lecca/network-analyzer-and-dynamics-simulator">https://gitlab.inf.unibz.it/Paola.Lecca/network-analyzer-and-dynamics-simulator</ext-link>.</p>
</sec>
<sec id="s7">
<title>Author Contributions</title>
<p>PL designed the methods and implemented the R codes for the analysis of the biological network, the automatic translation of the hypergraph into a set of rate equations, the numerical solution of the model and the sensitivity analysis. AI-N provided the biological background and provided the interpretation of the results obtained, in the light of an extensive literature search. Both authors contributed to the conceptualisation of the paper, its writing and revision.</p>
</sec>
<sec id="s8">
<title>Funding</title>
<p>This study has been supported by the COMPANET RTD 2019 Project funds, issued to PL (Principal Investigator) by the Faculty of Computer Science, Free University of Bozen-Bolzano, Italy.</p>
</sec>
<sec sec-type="COI-statement" id="s9">
<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="s10">
<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>
<sec id="s11">
<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/fmolb.2022.878148/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fmolb.2022.878148/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="Presentation1.zip" id="SM1" mimetype="application/zip" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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