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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Physiol.</journal-id>
<journal-title>Frontiers in Physiology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Physiol.</abbrev-journal-title>
<issn pub-type="epub">1664-042X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fphys.2021.767892</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physiology</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Unraveling A&#x03B2;-Mediated Multi-Pathway Calcium Dynamics in Astrocytes: Implications for Alzheimer&#x2019;s Disease Treatment From Simulations</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Liu</surname> <given-names>Langzhou</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="author-notes" rid="fn002"><sup>&#x2020;</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Gao</surname> <given-names>Huayi</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="author-notes" rid="fn002"><sup>&#x2020;</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Zaikin</surname> <given-names>Alexey</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<xref ref-type="aff" rid="aff4"><sup>4</sup></xref>
<xref ref-type="aff" rid="aff5"><sup>5</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/78276/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Chen</surname> <given-names>Shangbin</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>&#x002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/225387/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Britton Chance Center for Biomedical Photonics, Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology</institution>, <addr-line>Wuhan</addr-line>, <country>China</country></aff>
<aff id="aff2"><sup>2</sup><institution>MoE Key Laboratory for Biomedical Photonics, School of Engineering Sciences, Huazhong University of Science and Technology</institution>, <addr-line>Wuhan</addr-line>, <country>China</country></aff>
<aff id="aff3"><sup>3</sup><institution>Institute of Information Technologies, Mathematics and Mechanics, Lobachevsky State University of Nizhny Novgorod</institution>, <addr-line>Nizhny Novgorod</addr-line>, <country>Russia</country></aff>
<aff id="aff4"><sup>4</sup><institution>Institute for Women&#x2019;s Health and Department of Mathematics, University College London</institution>, <addr-line>London</addr-line>, <country>United Kingdom</country></aff>
<aff id="aff5"><sup>5</sup><institution>World-Class Research Center &#x201C;Digital Biodesign and Personalized Healthcare&#x201D;, Sechenov First Moscow State Medical University</institution>, <addr-line>Moscow</addr-line>, <country>Russia</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Antonio Batista, Universidade Estadual de Ponta Grossa, Brazil</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Paulo Ricardo Protachevicz, University of S&#x00E3;o Paulo, Brazil; Arthur Valencio, University of Campinas, Brazil; Ewandson L. Lameu, University of Calgary, Canada</p></fn>
<corresp id="c001">&#x002A;Correspondence: Shangbin Chen, <email>sbchen@mail.hust.edu.cn</email></corresp>
<fn fn-type="equal" id="fn002"><p><sup>&#x2020;</sup>These authors have contributed equally to this work and share first authorship</p></fn>
<fn fn-type="other" id="fn004"><p>This article was submitted to Fractal Physiology, a section of the journal Frontiers in Physiology</p></fn>
</author-notes>
<pub-date pub-type="epub">
<day>28</day>
<month>10</month>
<year>2021</year>
</pub-date>
<pub-date pub-type="collection">
<year>2021</year>
</pub-date>
<volume>12</volume>
<elocation-id>767892</elocation-id>
<history>
<date date-type="received">
<day>31</day>
<month>08</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>08</day>
<month>10</month>
<year>2021</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x00A9; 2021 Liu, Gao, Zaikin and Chen.</copyright-statement>
<copyright-year>2021</copyright-year>
<copyright-holder>Liu, Gao, Zaikin and Chen</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>The accumulation of amyloid &#x03B2; peptide (A&#x03B2;) in the brain is hypothesized to be the major factor driving Alzheimer&#x2019;s disease (AD) pathogenesis. Mounting evidence suggests that astrocytes are the primary target of A&#x03B2; neurotoxicity. A&#x03B2; is known to interfere with multiple calcium fluxes, thus disrupting the calcium homeostasis regulation of astrocytes, which are likely to produce calcium oscillations. Ca<sup>2+</sup> dyshomeostasis has been observed to precede the appearance of clinical symptoms of AD; however, it is experimentally very difficult to investigate the interactions of many mechanisms. Given that Ca<sup>2+</sup> disruption is ubiquitously involved in AD progression, it is likely that focusing on Ca<sup>2+</sup> dysregulation may serve as a potential therapeutic approach to preventing or treating AD, while current hypotheses concerning AD have so far failed to yield curable therapies. For this purpose, we derive and investigate a concise mathematical model for A&#x03B2;-mediated multi-pathway astrocytic intracellular Ca<sup>2+</sup> dynamics. This model accounts for how A&#x03B2; affects various fluxes contributions through voltage-gated calcium channels, A&#x03B2;-formed channels and ryanodine receptors. Bifurcation analysis of A&#x03B2; level, which reflected the corresponding progression of the disease, revealed that A&#x03B2; significantly induced the increasing [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and frequency of calcium oscillations. The influence of inositol 1,4,5-trisphosphate production (IP<sub>3</sub>) is also investigated in the presence of A&#x03B2; as well as the impact of changes in resting membrane potential. In turn, the Ca<sup>2+</sup> flux can be considerably changed by exerting specific interventions, such as ion channel blockers or receptor antagonists. By doing so, a &#x201C;combination therapy&#x201D; targeting multiple pathways simultaneously has finally been demonstrated to be more effective. This study helps to better understand the effect of A&#x03B2;, and our findings provide new insight into the treatment of AD.</p>
</abstract>
<kwd-group>
<kwd>A&#x03B2;</kwd>
<kwd>Alzheimer&#x2019;s disease</kwd>
<kwd>astrocyte</kwd>
<kwd>calcium oscillations</kwd>
<kwd>dyshomeostasis</kwd>
<kwd>therapy</kwd>
</kwd-group>
<counts>
<fig-count count="8"/>
<table-count count="2"/>
<equation-count count="23"/>
<ref-count count="77"/>
<page-count count="16"/>
<word-count count="12041"/>
</counts>
</article-meta>
</front>
<body>
<sec sec-type="intro" id="S1">
<title>Introduction</title>
<p>Alzheimer&#x2019;s disease (AD) is currently the most common neurodegenerative disease and is the major dementia type, which accounts for 60&#x2013;70% of cases (<xref ref-type="bibr" rid="B53">Prince, 2015</xref>; <xref ref-type="bibr" rid="B16">Canter et al., 2016</xref>). The Alzheimer Disease International estimated in 2019 that over 50 million people were living with dementia and this number is expected to exceed 150 million by 2050 (<xref ref-type="bibr" rid="B45">Lynch, 2020</xref>). The disease has already caused incalculable losses worldwide. Little is known about the complex pathophysiology of AD, and thus, there is no cure. Pathological characteristics of accumulation of amyloid &#x03B2;-peptide (A&#x03B2;), is considered to be drivers in AD pathogenesis (<xref ref-type="bibr" rid="B35">Hardy and Selkoe, 2002</xref>; <xref ref-type="bibr" rid="B13">Birch, 2014</xref>).</p>
<p>Astrocytes were historically considered to provide support for neurons (<xref ref-type="bibr" rid="B17">Carmignoto and G&#x00F3;mez-Gonzalo, 2010</xref>). Since they were found to be involved in many brain functions and neurodegenerative diseases such as AD and Parkinson&#x2019;s disease etc., astrocytes have become a hot topic in neuroscience research over the past few decades (<xref ref-type="bibr" rid="B67">Tewari and Majumdar, 2012</xref>; <xref ref-type="bibr" rid="B68">Tewari and Parpura, 2013</xref>; <xref ref-type="bibr" rid="B10">Bazargani and Attwell, 2016</xref>). In cultures of mixed neurons and astrocytes treated with A&#x03B2;, astrocytes always exhibit pathological alterations before neuronal death suggesting that astrocytes appear to be the primary target of A&#x03B2; (<xref ref-type="bibr" rid="B1">Abramov et al., 2003</xref>). Their role as protector and housekeeper in central nervous system is universally acknowledged, however, A&#x03B2; impairs important supportive astrocyte functions in AD cases (<xref ref-type="bibr" rid="B73">Verkhratsky and Nedergaard, 2018</xref>).</p>
<p>Astrocytes do not generate electrical signals like neurons (<xref ref-type="bibr" rid="B74">Wu et al., 2015</xref>). However, the concept of &#x201C;cellular excitability&#x201D; in astrocytes has been recently formalized to describe the changes in cytosolic Ca<sup>2+</sup> concentration in response to chemical or mechanical stimulation (<xref ref-type="bibr" rid="B72">Verkhratsky, 2019</xref>). For example, they encode synaptic information via the modulation of intracellular calcium dynamics in response to synaptic activity (<xref ref-type="bibr" rid="B23">De Pitt&#x00E0; et al., 2009</xref>). However, this kind of Ca<sup>2+</sup> homeostasis can be disrupted by A&#x03B2;, whether in neurons or astrocytes, especially its soluble oligomeric form is more harmful (<xref ref-type="bibr" rid="B26">Demuro et al., 2010</xref>). In an AD mouse model, astrocytes displayed higher basal astrocyte Ca<sup>2+</sup> levels and increased transient Ca<sup>2+</sup> signals (<xref ref-type="bibr" rid="B38">Kuchibhotla et al., 2009</xref>).</p>
<p>A&#x03B2; is known to interfere with multiple calcium fluxes in astrocytes. A&#x03B2; oligomers deposition not only form pores in the lipid bilayer permeable to cationic ions, but also directly or indirectly activate L-type Ca<sub><italic>V</italic></sub>, which increases the concentration of intracellular Ca<sup>2+</sup> (<xref ref-type="bibr" rid="B4">Alves et al., 2019</xref>). Additionally, the expression of astroglial mGluR<sub>5</sub> is up-regulated by exposure to A&#x03B2; (<xref ref-type="bibr" rid="B42">Lim et al., 2013</xref>). Inside astrocytes, A&#x03B2; can induce endoplasmic reticulum (ER) Ca<sup>2+</sup> release through ryanodine receptors (RyRs) and inositol triphosphate receptors (IP<sub>3</sub>Rs) (<xref ref-type="bibr" rid="B3">Alberdi et al., 2013</xref>). How to combine these different findings to understand the big picture is crucial for further research (<xref ref-type="bibr" rid="B47">Markowetz, 2017</xref>). However, it is experimentally very difficult to investigate the interactions of many mechanisms of Ca<sup>2+</sup> dyshomeostasis (<xref ref-type="bibr" rid="B21">Cutsuridis and Moustafa, 2017</xref>), e.g., the limitations of Ca<sup>2+</sup> indicators and imaging techniques.</p>
<p>Simulation based on the mathematical model has been an invaluable tool to investigate complex interactions. There are hundreds of computational models on astrocyte Ca<sup>2+</sup> dynamics and homeostasis either in a single astrocyte or in astrocyte networks or in neuron-astrocyte synapses (<xref ref-type="bibr" rid="B46">Manninen et al., 2018</xref>). Here, we focus primarily on modeling efforts in single astrocyte. Most of them studied Ca<sup>2+</sup> oscillations, while a small part of them modeled spontaneous Ca<sup>2+</sup> activity (<xref ref-type="bibr" rid="B40">Lavrentovich and Hemkin, 2008</xref>; <xref ref-type="bibr" rid="B58">Riera et al., 2011b</xref>); some assessed neurotransmitter-evoked Ca<sup>2+</sup> excitability (<xref ref-type="bibr" rid="B23">De Pitt&#x00E0; et al., 2009</xref>; <xref ref-type="bibr" rid="B30">Dupont et al., 2011</xref>). These computational studies are mostly based on classic models, including components for calcium-induced calcium release (CICR) and the sarco-endoplasmic Ca<sup>2+</sup> ATPase pump (SERCA). In astrocytes, intracellular Ca<sup>2+</sup> oscillations depend mainly on CICR, while Ca<sup>2+</sup> influx from extracellular space via receptors or channels on membrane such as voltage-gated calcium channels (VGCCs) has also been linked with Ca<sup>2+</sup> oscillations (<xref ref-type="bibr" rid="B40">Lavrentovich and Hemkin, 2008</xref>; <xref ref-type="bibr" rid="B77">Zeng et al., 2009</xref>). <xref ref-type="bibr" rid="B64">Taheri et al. (2017)</xref> modeled capacitive Ca<sup>2+</sup> entry, which is mediated via store-operated Ca<sup>2+</sup> channels. <xref ref-type="bibr" rid="B27">Ding et al. (2018)</xref> constructed two stochastic models, one describing the VGCC channel noise and the other describing the stochastic IP<sub>3</sub>R dynamics. Recently, some modeling work has addressed the effect of A&#x03B2; on Ca<sup>2+</sup> dynamics in generic cells (<xref ref-type="bibr" rid="B39">Latulippe et al., 2018</xref>). We established an A&#x03B2;-mediated calcium signaling model in astrocytes for the pilot study (<xref ref-type="bibr" rid="B33">Gao et al., 2020</xref>). All the models have useful implications for understanding Ca<sup>2+</sup> signaling. However, no model has integrated the abovementioned putative mechanisms (<xref ref-type="bibr" rid="B1">Abramov et al., 2003</xref>; <xref ref-type="bibr" rid="B3">Alberdi et al., 2013</xref>; <xref ref-type="bibr" rid="B42">Lim et al., 2013</xref>; <xref ref-type="bibr" rid="B4">Alves et al., 2019</xref>) to simulate Ca<sup>2+</sup> dynamics in astrocytes. The synergistic effect of the different Ca<sup>2+</sup> fluxes on Ca<sup>2+</sup> dynamics is not well understood so far. In particular, the current development of the theme lacks results regarding restoring the Ca<sup>2+</sup> homeostasis in astrocytes during the progression of AD.</p>
<p>To date, the treatment of AD has remained a challenge. Although some promising drugs are under continuous development, clinical trials in recent years fail to get satisfied results (<xref ref-type="bibr" rid="B54">Qian et al., 2015</xref>). The currently approved anti-AD drugs fall into two types: cholinesterase inhibitors (donepezil, rivastigmine and galantamine) and N-methyl-D-aspartic acid receptor antagonists (memantine) (<xref ref-type="bibr" rid="B9">Aupperle, 2006</xref>). On the one hand, these drugs can only relieve symptoms but do not prevent the progression of AD, suggesting that their targets might not be the disease origin (<xref ref-type="bibr" rid="B44">Liu et al., 2019</xref>). On the other hand, memantine can prevent NMDAR-mediated Ca<sup>2+</sup> flux indicating that other Ca<sup>2+</sup> mechanisms may be a potential target for the treatment of AD when they have been demonstrated to play a proximal role in AD.</p>
<p>Here, a comprehensive model integrating multiple A&#x03B2;-affected Ca<sup>2+</sup> pathways is proposed. This model of astrocytes describes Ca<sup>2+</sup> signals as individual Ca<sup>2+</sup> transport pathways rather than a macroscopic flow of Ca<sup>2+</sup>, including both intracellular release and extracellular influx. With this computational model, we can begin to study how A&#x03B2; affects each source of Ca<sup>2+</sup> through various pathways. Recent wet-lab data are also incorporated into modeling work to obtain insights into AD treatment (<xref ref-type="bibr" rid="B60">Sadick and Liddelow, 2019</xref>). The explicit intention is to test the specific treatment strategy for AD.</p>
</sec>
<sec id="S2" sec-type="materials|methods">
<title>Materials and Methods</title>
<sec id="S2.SS1">
<title>Biophysical Model</title>
<p>Intracellular Ca<sup>2+</sup> levels are modulated by influx from the extracellular space or controlled release from intracellular Ca<sup>2+</sup> stores such as the ER. Generally, Ca<sup>2+</sup> entry into astrocytes includes active transport by different types of VGCCs distributed in the membrane and passive leakage. In astrocytes, however, IP<sub>3</sub>-dependent CICR from the ER is considered the primary mechanism responsible for intracellular Ca<sup>2+</sup> dynamics (<xref ref-type="bibr" rid="B2">Agulhon et al., 2008</xref>). CICR is essentially controlled by efflux from the ER to the cytoplasm that is mediated both by IP<sub>3</sub>R and RyR and influx into the ER, which is due to the action of SERCA pumps. A&#x03B2; can interfere with some of these Ca<sup>2+</sup> fluxes and the detailed modeling methods for A&#x03B2; are described in section &#x201C;A&#x03B2; Assumption.&#x201D; So, the whole-cell model is shown in <xref ref-type="fig" rid="F1">Figure 1</xref>.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption><p>Mechanisms involved in intracellular Ca<sup>2+</sup> dysregulation in AD. In this model, <italic>J</italic><sub><italic>VGCC</italic></sub> and <italic>J</italic><sub><italic>in</italic></sub> are Ca<sup>2+</sup> influxes from the extracellular space. The two separate mechanisms involved in the process of Ca<sup>2+</sup> release from the ER via IP<sub>3</sub>Rs and RyRs are <italic>J</italic><sub><italic>CICR</italic></sub> and <italic>J</italic><sub><italic>RyR</italic></sub>, respectively. <italic>J</italic><sub><italic>SERCA</italic></sub> represents the SERCA pump of the ER refilling the ER by pumping Ca<sup>2+</sup> back from the cytosol. <italic>J</italic><sub><italic>leak</italic></sub> is the leakage Ca<sup>2+</sup> flux from the ER into the cytosol. <italic>J</italic><sub><italic>out</italic></sub> is Ca<sup>2+</sup> efflux by Ca<sup>2+</sup>-ATPase pump. Red lines represent the functional pathway of A&#x03B2;, and green lines represent the inhibitory effects of drugs.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-767892-g001.tif"/>
</fig>
<sec id="S2.SS1.SSS1">
<title>Intracellular Ca<sup>2+</sup> Dynamics</title>
<p>We describe the model by tracking the flux in and out of the cytoplasm. Then, the change in intracellular Ca<sup>2+</sup> is governed by</p>
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<p>where [<italic>Ca</italic><sup>2 +</sup>]<sub><italic>i</italic></sub> and [Ca<sup>2 +</sup>]<sub><italic>ER</italic></sub>denote the concentration of Ca<sup>2+</sup> in the cytoplasm and ER, respectively. c<sub>1</sub>is the ratio of ER volume to the cytoplasmic volume. We assumed a spatially homogeneous astrocyte whose volume was fixed. As such, the ER and cytoplasm are simplified as two points of the cell for better quantifying and identifying key mechanisms behind certain Ca<sup>2+</sup> fluxes.</p>
<p>The term <italic>J</italic><sub><italic>VGCC</italic></sub> represents the pathway of Ca<sup>2+</sup> influx through four types of VGCCs, including L-, N-, T-, and R-types. When the volume of the cell is constant, the Ca<sup>2+</sup> flux and current are related by the equations (<xref ref-type="bibr" rid="B77">Zeng et al., 2009</xref>):</p>
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</disp-formula>
<p>where <italic>I</italic><sub><italic>VGCC</italic></sub> is the VGCC-conducted Ca<sup>2+</sup> current, and <italic>I</italic><sub><italic>Ca,L</italic></sub>, <italic>I</italic><sub><italic>Ca,T</italic></sub>, <italic>I</italic><sub><italic>Ca,N</italic></sub>, <italic>I</italic><sub><italic>Ca,R</italic></sub> represent the current through different types of channels. <italic>z</italic> is the valence of Ca<sup>2+</sup>, <italic>F</italic> is the Faraday constant and <italic>V</italic><sub><italic>ast</italic></sub> is the volume of the astrocyte. The concrete formula for every type of calcium current is given in detail in <xref ref-type="table" rid="T1">Table 1</xref>.</p>
<table-wrap position="float" id="T1">
<label>TABLE 1</label>
<caption><p>Details of the voltage-gated calcium channels.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left">Channel type</td>
<td valign="top" align="center">Equation of channel dynamics</td>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">T-type</td>
<td valign="top" align="center"><italic>I</italic><sub><italic>Ca</italic>,<italic>T</italic></sub>=<italic>g</italic><sub><italic>T</italic></sub><italic>m</italic><sub><italic>T</italic></sub>(<italic>h</italic><sub><italic>Tf</italic></sub> + 0.04<italic>h</italic><sub><italic>Ts</italic></sub>)(<italic>V</italic><sub><italic>m</italic></sub>&#x2212;<italic>E</italic><sub><italic>Ca</italic></sub>)</td>
</tr>
<tr>
<td/>
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</tr>
<tr>
<td valign="top" align="left">L-type</td>
<td valign="top" align="center"><italic>I</italic><sub><italic>Ca</italic>,<italic>L</italic></sub>=<italic>g</italic><sub><italic>L</italic></sub><italic>m</italic><sub><italic>L</italic></sub><italic>h</italic><sub><italic>L</italic></sub>(<italic>V</italic><sub><italic>m</italic></sub>&#x2212;<italic>E</italic><sub><italic>Ca</italic></sub>)</td>
</tr>
<tr>
<td/>
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</tr>
<tr>
<td valign="top" align="left">N-type</td>
<td valign="top" align="center"><italic>I</italic><sub><italic>Ca</italic>,<italic>N</italic></sub>=<italic>g</italic><sub><italic>N</italic></sub><italic>m</italic><sub><italic>N</italic></sub><italic>h</italic><sub><italic>N</italic></sub>(<italic>V</italic><sub><italic>m</italic></sub>&#x2212;<italic>E</italic><sub><italic>Ca</italic></sub>)</td>
</tr>
<tr>
<td/>
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</tr>
<tr>
<td valign="top" align="left">R-type</td>
<td valign="top" align="center"><italic>I</italic><sub><italic>Ca</italic>,<italic>R</italic></sub>=<italic>g</italic><sub><italic>R</italic></sub><italic>m</italic><sub><italic>R</italic></sub><italic>h</italic><sub><italic>R</italic></sub>(<italic>V</italic><sub><italic>m</italic></sub>&#x2212;<italic>E</italic><sub><italic>Ca</italic></sub>)</td>
</tr>
<tr>
<td/>
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</tr>
</tbody>
</table>
<table-wrap-foot>
<fn><p><italic><italic>Here</italic>,<italic>g</italic> <italic>is the conductance of the channel</italic>,<italic>V</italic><sub><italic>m</italic></sub> <italic>is the resting membrane potential</italic>,<italic>E</italic><sub><italic>Ca</italic></sub> <italic>is the Nernst potential of the VGCC and is expressed as</italic> <inline-formula><mml:math id="INEQ17"><mml:mrow><mml:mpadded width="+3.3pt"><mml:msub><mml:mi>E</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mo>&#x2062;</mml:mo><mml:mi>a</mml:mi></mml:mrow></mml:msub></mml:mpadded><mml:mo rspace="5.8pt">=</mml:mo><mml:mrow><mml:mfrac><mml:mrow><mml:mi>R</mml:mi><mml:mo>&#x2062;</mml:mo><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>z</mml:mi><mml:mo>&#x2062;</mml:mo><mml:mi>F</mml:mi></mml:mrow></mml:mfrac><mml:mo>&#x2062;</mml:mo><mml:mi>l</mml:mi><mml:mo>&#x2062;</mml:mo><mml:mi>n</mml:mi><mml:mo>&#x2062;</mml:mo><mml:mfrac><mml:msub><mml:mrow><mml:mo stretchy="false">[</mml:mo><mml:mrow><mml:mi>C</mml:mi><mml:mo>&#x2062;</mml:mo><mml:msup><mml:mi>a</mml:mi><mml:mrow><mml:mn>2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow><mml:mo stretchy="false">]</mml:mo></mml:mrow><mml:mi>o</mml:mi></mml:msub><mml:msub><mml:mrow><mml:mo stretchy="false">[</mml:mo><mml:mrow><mml:mi>C</mml:mi><mml:mo>&#x2062;</mml:mo><mml:msup><mml:mi>a</mml:mi><mml:mrow><mml:mn>2</mml:mn><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow><mml:mo stretchy="false">]</mml:mo></mml:mrow><mml:mi>i</mml:mi></mml:msub></mml:mfrac></mml:mrow></mml:mrow></mml:math></inline-formula>, <italic>m and</italic> <italic>h</italic> <italic>are gating variables;</italic> <inline-formula><mml:math id="INEQ19"><mml:mover accent="true"><mml:mi>m</mml:mi><mml:mo>&#x00AF;</mml:mo></mml:mover></mml:math></inline-formula>, <inline-formula><mml:math id="INEQ20"><mml:mover accent="true"><mml:mi>h</mml:mi><mml:mo>&#x00AF;</mml:mo></mml:mover></mml:math></inline-formula> <italic>are steady states of the channel activation and inactivation variables, respectively.</italic></italic></p></fn>
</table-wrap-foot>
</table-wrap>
<p><italic>J</italic><sub><italic>in</italic></sub> is a passive leakage from the extracellular space. <xref ref-type="bibr" rid="B59">Riera et al. (2011a)</xref> used a heuristic strategy to determine <italic>J</italic><sub><italic>in</italic></sub> = 0.036 &#x03BC;M/s for healthy astrocytes:</p>
<disp-formula id="S2.E5">
<label>(5)</label>
<mml:math id="M5">
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<mml:mrow>
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</mml:mrow>
<mml:mo>.</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>To represent the kinetics of the IP<sub>3</sub>R, we used a simplification form (<xref ref-type="bibr" rid="B70">Ullah et al., 2006</xref>) described as</p>
<disp-formula id="S2.E6">
<label>(6)</label>
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<mml:mo>,</mml:mo>
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</disp-formula>
<p>where <italic>v<sub>1</sub></italic> determines the maximal rate of transported Ca<sup>2+</sup>, <italic>m</italic>, <italic>n</italic> and <italic>h</italic> are gating variables of IP<sub>3</sub>R. The first two are assumed to have instantaneous kinetics, <italic>m</italic>=<italic>m</italic><sub>&#x221E;</sub>, <italic>n</italic>=<italic>n</italic><sub>&#x221E;</sub>, while <italic>h</italic> obeys Hodgkin-Huxley formalism. They are specified as follows:</p>
<disp-formula id="S2.E7">
<label>(7)</label>
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<mml:mi>m</mml:mi>
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<disp-formula id="S2.E9">
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</disp-formula>
<p><italic><italic>d<sub>1</sub></italic></italic> and <italic><italic>d<sub>5</sub></italic></italic> determine the dissociation of IP<sub>3</sub> and Ca<sup>2+</sup> by the channel&#x2019;s subunits, whereas <italic><italic>d<sub>2</sub></italic></italic> and <italic><italic>d<sub>3</sub></italic></italic> is the inactivation dissociation constant of Ca<sup>2+</sup> and IP<sub>3</sub>, respectively. <italic><italic>a<sub>2</sub></italic></italic> determines the IP<sub>3</sub>R binding rate for Ca<sup>2+</sup> inhibition.</p>
<p>The SERCA pump rate can be taken as an instantaneous function of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> by using a Hill-type kinetic model (<xref ref-type="bibr" rid="B70">Ullah et al., 2006</xref>):</p>
<disp-formula id="S2.E10">
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<mml:mo>,</mml:mo>
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</disp-formula>
<p>where <italic>v<sub>3</sub></italic> represents the maximum SERCA pump flux and <italic>k<sub>3</sub></italic> is the dissociation constant of Ca<sup>2+</sup> to SERCA.</p>
<p>To model RyR, we modified the previous model (<xref ref-type="bibr" rid="B32">Friel, 1995</xref>) by increasing the effect of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and took the following form:</p>
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</mml:mrow>
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</mml:mrow>
<mml:mo>]</mml:mo>
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<mml:mrow>
<mml:mi>E</mml:mi>
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<mml:msub>
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<mml:mn>2</mml:mn>
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</mml:mrow>
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</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>k<sub>0</sub></italic> is the zero calcium concentration level leak. This parameter is usually used to ensure a physiologically meaningful resting Ca<sup>2+</sup> level (<xref ref-type="bibr" rid="B29">Dupont et al., 2016</xref>). Furthermore, <italic>k<sub>2</sub></italic> is the maximal rate of the channel, <italic>k<sub>d</sub></italic> corresponds to the RyR channel sensitivity for the CICR.</p>
<p>The leakage flux from the ER is assumed to be proportional to the Ca<sup>2+</sup> gradient across the ER membrane by <italic>v<sub>2</sub></italic>, the maximal rate of Ca<sup>2+</sup> leakage (<xref ref-type="bibr" rid="B70">Ullah et al., 2006</xref>).</p>
<disp-formula id="S2.E12">
<label>(12)</label>
<mml:math id="M12">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
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<mml:mi>J</mml:mi>
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</mml:msub>
</mml:mpadded>
<mml:mo rspace="5.8pt">=</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>v</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mo>&#x2062;</mml:mo>
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<mml:mo stretchy="false">(</mml:mo>
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</mml:mrow>
</mml:mrow>
</mml:mrow>
<mml:mo>.</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>Finally, we considered Ca<sup>2+</sup> extrusion flux as described (<xref ref-type="bibr" rid="B70">Ullah et al., 2006</xref>):</p>
<disp-formula id="S2.E13">
<label>(13)</label>
<mml:math id="M13">
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</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>k<sub>1</sub></italic> is the rate constant of calcium extrusion.</p>
</sec>
<sec id="S2.SS1.SSS2">
<title>Generation/Degradation of Cytosolic IP<sub>3</sub></title>
<p>IP<sub>3</sub> is the second messenger involved in G protein-coupled receptor-mediated signal transduction. In astrocytes, IP<sub>3</sub> is produced by hydrolysis of phosphatidylinositol 4,5-bisphosphate by two phosphoinositide-specific phospholipase C (PLC) isoenzymes, PLC&#x03B2; and PLC&#x03B4; (<xref ref-type="bibr" rid="B55">Rebecchi and Pentyala, 2000</xref>). Therefore, the IP<sub>3</sub> dynamic is described as:</p>
<disp-formula id="S2.E14">
<label>(14)</label>
<mml:math id="M14">
<mml:mrow>
<mml:mrow>
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</mml:mrow>
<mml:mo>/</mml:mo>
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</mml:mrow>
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<mml:mo>&#x2062;</mml:mo>
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<mml:mrow>
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<mml:mo stretchy="false">]</mml:mo>
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</mml:mrow>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>J</italic><sub><italic>PLC&#x03B2;</italic></sub> and <italic>J</italic><sub><italic>PLC&#x03B4;</italic></sub> are PLC&#x03B2;- and PLC&#x03B4;-dependent IP<sub>3</sub> production, respectively. <italic>k</italic><sub><italic>deg</italic></sub> represents the rate of IP<sub>3</sub> degradation.</p>
<p>PLC&#x03B2; is primarily controlled by external glutamate stimulation (<xref ref-type="bibr" rid="B23">De Pitt&#x00E0; et al., 2009</xref>). So <italic>J</italic><sub><italic>PLC&#x03B2;</italic></sub> can be modeled as follows (<xref ref-type="bibr" rid="B23">De Pitt&#x00E0; et al., 2009</xref>):</p>
<disp-formula id="S2.E15">
<label>(15)</label>
<mml:math id="M15">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
<mml:msub>
<mml:mi>J</mml:mi>
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<mml:mo>&#x2062;</mml:mo>
<mml:mi mathvariant="normal">&#x03B2;</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mpadded>
<mml:mo rspace="5.8pt">=</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>v</mml:mi>
<mml:mi mathvariant="normal">&#x03B2;</mml:mi>
</mml:msub>
<mml:mo>&#x2062;</mml:mo>
<mml:mfrac>
<mml:msup>
<mml:mi>g</mml:mi>
<mml:mn>0.7</mml:mn>
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<mml:mrow>
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<mml:mi>g</mml:mi>
<mml:mn>0.7</mml:mn>
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<mml:mo>+</mml:mo>
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</mml:mrow>
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<mml:mo>+</mml:mo>
<mml:msub>
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<mml:mi mathvariant="normal">&#x03C0;</mml:mi>
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</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mn>0.7</mml:mn>
</mml:msup>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>v</italic><sub>&#x03B2;</sub> is the maximal PLC&#x03B2; rate, <italic>g</italic> is the concentration of glutamate, we set this value to be <italic>g</italic> = 1 &#x03BC;M. <italic>k<sub>R</sub></italic> is glutamate affinity and <italic>k<sub>P</sub></italic> is the Ca<sup>2+</sup>/PLC-dependent inhibition factor and <italic>k</italic><sub>&#x03C0;</sub> controls Ca<sup>2+</sup> affinity of PLC.</p>
<p>In contrast, PLC&#x03B4; is essentially activated by increased intracellular Ca<sup>2+</sup> levels (<xref ref-type="bibr" rid="B57">Rhee and Bae, 1997</xref>) and is written as (<xref ref-type="bibr" rid="B24">De Young and Keizer, 1992</xref>):</p>
<disp-formula id="S2.E16">
<label>(16)</label>
<mml:math id="M16">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
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</mml:mpadded>
<mml:mo rspace="5.8pt">=</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>v</mml:mi>
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</mml:mrow>
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</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>v<sub>4</sub></italic> is the maximum rate of IP<sub>3</sub> production, and <italic>k<sub>4</sub></italic> is the dissociation constant for Ca<sup>2+</sup> stimulation of IP<sub>3</sub> production. Here &#x03B1; is used to investigate the relative effect of Ca<sup>2+</sup> stimulation of PLC&#x03B4; on IP<sub>3</sub> production. For example, if &#x03B1; = 0, the IP<sub>3</sub> production rate is <italic>v<sub>4</sub></italic>, which is independent of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub>.</p>
</sec>
</sec>
<sec id="S2.SS2">
<title>A&#x03B2; Assumption</title>
<p>Exposure of astrocytes to A&#x03B2; was reported to trigger [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> transients and [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> oscillations (<xref ref-type="bibr" rid="B3">Alberdi et al., 2013</xref>). Such effects may involve various Ca<sup>2+</sup> entry pathways as well as Ca<sup>2+</sup> release from ER (<xref ref-type="bibr" rid="B1">Abramov et al., 2003</xref>; <xref ref-type="bibr" rid="B3">Alberdi et al., 2013</xref>). These experimental findings have provided useful insights for us to make our A&#x03B2; assumption. However, in the real condition, the accumulation of A&#x03B2; can occur over months, years, and even decades which does not match the short timescale of changes in Ca<sup>2+</sup>. To solve this issue, we assumed a fixed level of A&#x03B2; concentration in our model using the parameter <italic>a</italic> which corresponds to the certain stage of the progression of AD. For example, a small value of <italic>a</italic> may reflect a low level of A&#x03B2; representing the early stage of the disease. By changing <italic>a</italic>, we can easily investigate the effect of A&#x03B2; on different progressions of AD.</p>
<p>A study has demonstrated that L-type channels might be activated by A&#x03B2;, and increased expression of L-type channels is associated with A&#x03B2;-positive plaques (<xref ref-type="bibr" rid="B4">Alves et al., 2019</xref>). To do this, we altered the original form of <italic>I</italic><sub><italic>Ca,L</italic></sub>:</p>
<disp-formula id="S2.E17">
<label>(17)</label>
<mml:math id="M17">
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<mml:mi>h</mml:mi>
<mml:mi>L</mml:mi>
</mml:msub>
<mml:mo>&#x2062;</mml:mo>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
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<mml:mi>V</mml:mi>
<mml:mi>m</mml:mi>
</mml:msub>
<mml:mo>-</mml:mo>
<mml:msub>
<mml:mi>E</mml:mi>
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<mml:mi>C</mml:mi>
<mml:mo>&#x2062;</mml:mo>
<mml:mi>a</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>k</italic><sub><italic>VGCC</italic></sub> controls the strength of the effect of A&#x03B2; on the channels.</p>
<p>Besides, A&#x03B2;-formed channels on the plasma membrane can also trigger additional Ca<sup>2+</sup> influx into the cytoplasm (<xref ref-type="bibr" rid="B26">Demuro et al., 2010</xref>). In order to incorporate the possible influence, we included another term in<italic>J</italic><sub><italic>in</italic></sub>:</p>
<disp-formula id="S2.E18">
<label>(18)</label>
<mml:math id="M18">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
<mml:msub>
<mml:mi>J</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x2062;</mml:mo>
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</mml:mrow>
</mml:msub>
</mml:mpadded>
<mml:mo rspace="5.8pt">=</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>v</mml:mi>
<mml:mn>5</mml:mn>
</mml:msub>
<mml:mo>+</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>k</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x2062;</mml:mo>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2062;</mml:mo>
<mml:msup>
<mml:mi>a</mml:mi>
<mml:mi>k</mml:mi>
</mml:msup>
</mml:mrow>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>k</italic><sub><italic>in</italic></sub> represents a rate constant (<xref ref-type="bibr" rid="B22">De Caluw&#x00E9; and Dupont, 2013</xref>), or, in other words, the strength of A&#x03B2; in this study, and <italic>k</italic> is the cooperativity coefficient.</p>
<p>Although some studies have elucidated the role of RyRs in regulating Ca<sup>2+</sup> disruption in AD (<xref ref-type="bibr" rid="B62">Stutzmann et al., 2006</xref>; <xref ref-type="bibr" rid="B34">Goussakov et al., 2010</xref>; <xref ref-type="bibr" rid="B15">Briggs et al., 2013</xref>), data on the contributions of Ca<sup>2+</sup> flux through the RyR in the presence of A&#x03B2; are minimal. Given that A&#x03B2; can increase the channel open probability, we decided to revise the expression as follows:</p>
<disp-formula id="S2.E19">
<label>(19)</label>
<mml:math id="M19">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
<mml:msub>
<mml:mi>J</mml:mi>
<mml:mrow>
<mml:mi>R</mml:mi>
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<mml:mo>&#x2062;</mml:mo>
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</mml:msub>
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<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>k</mml:mi>
<mml:mn>0</mml:mn>
</mml:msub>
<mml:mo>+</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mi>k</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:mo>&#x2062;</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mo stretchy="false">[</mml:mo>
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<mml:mo>+</mml:mo>
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</mml:msup>
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<mml:mo stretchy="false">]</mml:mo>
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<mml:mi>i</mml:mi>
<mml:mn>3</mml:mn>
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<mml:msub>
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<mml:mo>+</mml:mo>
</mml:mrow>
</mml:msup>
</mml:mrow>
<mml:mo>]</mml:mo>
</mml:mrow>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>k</italic><sub><italic>RyR</italic></sub> represents the strength of A&#x03B2;.</p>
<p>In addition to the direct effect on Ca<sup>2+</sup> fluxes, A&#x03B2; can also alter IP<sub>3</sub> levels. On the one hand, A&#x03B2; up-regulates the expression of astroglial mGluR<sub>5</sub>, therefore, affects downstream IP<sub>3</sub> production (<xref ref-type="bibr" rid="B56">Renner et al., 2010</xref>). On the other hand, intracellular A&#x03B2; oligomers induce Ca<sup>2+</sup> liberation from the ER via IP<sub>3</sub>Rs by stimulating PLC-mediated IP<sub>3</sub> production (<xref ref-type="bibr" rid="B25">Demuro and Parker, 2013</xref>). Based on these findings, we adapted equations (15) and (16), assuming that the glutamate- and Ca<sup>2+</sup>-dependent IP<sub>3</sub> production would take the following forms:</p>
<disp-formula id="S2.E20">
<label>(20)</label>
<mml:math id="M20">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
<mml:msub>
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<mml:mi>a</mml:mi>
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<mml:mo stretchy="false">]</mml:mo>
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<mml:mi>i</mml:mi>
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<mml:mrow>
<mml:mn>2</mml:mn>
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</mml:mrow>
</mml:msup>
</mml:mrow>
<mml:mo stretchy="false">]</mml:mo>
</mml:mrow>
<mml:mi>i</mml:mi>
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<mml:mo>+</mml:mo>
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</mml:mfrac>
</mml:mrow>
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<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
<mml:mn>0.7</mml:mn>
</mml:msup>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<disp-formula id="S2.E21">
<label>(21)</label>
<mml:math id="M21">
<mml:mrow>
<mml:mrow>
<mml:mpadded width="+3.3pt">
<mml:msub>
<mml:mi>J</mml:mi>
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</mml:mrow>
</mml:msub>
</mml:mpadded>
<mml:mo rspace="5.8pt">=</mml:mo>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>v</mml:mi>
<mml:mn>4</mml:mn>
</mml:msub>
<mml:mo>+</mml:mo>
<mml:mrow>
<mml:msub>
<mml:mi>k</mml:mi>
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</mml:mrow>
<mml:mo>&#x2062;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msup>
<mml:mtext>[Ca</mml:mtext>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mo>+</mml:mo>
</mml:mrow>
</mml:msup>
<mml:mo stretchy="false">]</mml:mo>
<mml:msub>
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<mml:mo>+</mml:mo>
<mml:mo stretchy="false">(</mml:mo>
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<mml:mi mathvariant="normal">&#x03B1;</mml:mi>
<mml:mo stretchy="false">)</mml:mo>
<mml:mi>k</mml:mi>
<mml:msub>
<mml:mi/>
<mml:mn>4</mml:mn>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msup>
<mml:mtext>[Ca</mml:mtext>
<mml:mrow>
<mml:mn>2</mml:mn>
<mml:mo>+</mml:mo>
</mml:mrow>
</mml:msup>
<mml:mo stretchy="false">]</mml:mo>
<mml:msub>
<mml:mi/>
<mml:mrow>
<mml:mtext>i</mml:mtext>
</mml:mrow>
</mml:msub>
<mml:mo>+</mml:mo>
<mml:mi>k</mml:mi>
<mml:msub>
<mml:mi/>
<mml:mn>4</mml:mn>
</mml:msub>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where the parameters <italic>k</italic><sub><italic>PLC&#x03B2;</italic></sub> and <italic>k</italic><sub><italic>PLC&#x03B4;</italic></sub> control the strength of the linear influence of A&#x03B2; on each term, respectively.</p>
<p>All the parameters used in our model can be found in <xref ref-type="table" rid="T2">Table 2</xref>. In simulations, parameters are chosen under the principle that the oscillations obtained agree qualitatively with the experimental data. More details of the model can be found in the associated MATLAB code (R2020a, MathWorks; see in the Supporting Material).</p>
<table-wrap position="float" id="T2">
<label>TABLE 2</label>
<caption><p>Parameters used in the model.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left">Parameter</td>
<td valign="top" align="left">Description</td>
<td valign="top" align="left">Value</td>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left"><italic>a</italic></td>
<td valign="top" align="left">A fixed level of A&#x03B2; concentration</td>
<td valign="top" align="left">&#x2265; 0</td>
</tr>
<tr>
<td valign="top" align="left"><italic>c<sub>1</sub></italic></td>
<td valign="top" align="left">The ratio of ER volume to the cytoplasmic volume</td>
<td valign="top" align="left">0.185</td>
</tr>
<tr>
<td valign="top" align="left"><italic>z</italic></td>
<td valign="top" align="left">Valence of Ca<sup>2+</sup></td>
<td valign="top" align="left">2</td>
</tr>
<tr>
<td valign="top" align="left"><italic>z<sub>K</sub></italic></td>
<td valign="top" align="left">Valence of K<sup>+</sup></td>
<td valign="top" align="left">1</td>
</tr>
<tr>
<td valign="top" align="left"><italic>F</italic></td>
<td valign="top" align="left">Faraday constant</td>
<td valign="top" align="left">96,485 C/mole</td>
</tr>
<tr>
<td valign="top" align="left"><italic>R</italic></td>
<td valign="top" align="left">Ideal gas constant</td>
<td valign="top" align="left">8.31 J/(moleK)</td>
</tr>
<tr>
<td valign="top" align="left"><italic>T</italic></td>
<td valign="top" align="left">Temperature</td>
<td valign="top" align="left">293 K</td>
</tr>
<tr>
<td valign="top" align="left"><italic>V</italic><sub>ast</sub></td>
<td valign="top" align="left">The volume of an astrocyte</td>
<td valign="top" align="left">3.49&#x002A;10<sup>&#x2013;13</sup> L</td>
</tr>
<tr>
<td valign="top" align="left"><italic>v<sub>1</sub></italic></td>
<td valign="top" align="left">Max Ca<sup>2+</sup> channel flux</td>
<td valign="top" align="left">6 s<sup>&#x2013;1</sup></td>
</tr>
<tr>
<td valign="top" align="left"><italic>v<sub>2</sub></italic></td>
<td valign="top" align="left">Ca<sup>2+</sup> leak flux constant</td>
<td valign="top" align="left">0.11 s<sup>&#x2013;1</sup></td>
</tr>
<tr>
<td valign="top" align="left"><italic>v<sub>3</sub></italic></td>
<td valign="top" align="left">Maximum SERCA pump flux</td>
<td valign="top" align="left">2.2 &#x03BC;M/s</td>
</tr>
<tr>
<td valign="top" align="left"><italic>v<sub>4</sub></italic></td>
<td valign="top" align="left">Maximum rate of IP<sub>3</sub> production</td>
<td valign="top" align="left">0.5 &#x03BC;M/s</td>
</tr>
<tr>
<td valign="top" align="left"><italic>v<sub>5</sub></italic></td>
<td valign="top" align="left">Transmembrane leak flux</td>
<td valign="top" align="left">0.036 &#x03BC;M/s</td>
</tr>
<tr>
<td valign="top" align="left"><italic>v</italic><sub>&#x03B2;</sub></td>
<td valign="top" align="left">Maximal rate of IP<sub>3</sub> production by PLC&#x03B2;</td>
<td valign="top" align="left">0.05 &#x03BC;M/s</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k<sub>0</sub></italic></td>
<td valign="top" align="left">Zero calcium concentration level leak from RyRs</td>
<td valign="top" align="left">0.013 s<sup>&#x2013;1</sup></td>
</tr>
<tr>
<td valign="top" align="left"><italic>k<sub>1</sub></italic></td>
<td valign="top" align="left">Rate constant of calcium extrusion</td>
<td valign="top" align="left">0.5 s<sup>&#x2013;1</sup></td>
</tr>
<tr>
<td valign="top" align="left"><italic>k<sub>2</sub></italic></td>
<td valign="top" align="left">Maximal rate of the RyRs</td>
<td valign="top" align="left">0.18 s<sup>&#x2013;1</sup></td>
</tr>
<tr>
<td valign="top" align="left"><italic>k<sub>3</sub></italic></td>
<td valign="top" align="left">Dissociation constant of Ca<sup>2+</sup> to SERCA</td>
<td valign="top" align="left">0.05 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k<sub>4</sub></italic></td>
<td valign="top" align="left">Dissociation constant for Ca<sup>2+</sup> stimulation of IP<sub>3</sub> production</td>
<td valign="top" align="left">1.1 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k<sub>d</sub></italic></td>
<td valign="top" align="left">RyR sensitivity for the CICR</td>
<td valign="top" align="left">0.13 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k<sub>R</sub></italic></td>
<td valign="top" align="left">Glutamate affinity</td>
<td valign="top" align="left">1.3 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k<sub>P</sub></italic></td>
<td valign="top" align="left">The Ca<sup>2+</sup>/PLC-dependent inhibition factor</td>
<td valign="top" align="left">10 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k</italic><sub>&#x03C0;</sub></td>
<td valign="top" align="left">Ca<sup>2+</sup> affinity of PLC</td>
<td valign="top" align="left">0.6 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k</italic><sub><italic>deg</italic></sub></td>
<td valign="top" align="left">Rate of IP<sub>3</sub> degradation</td>
<td valign="top" align="left">1 s<sup>&#x2013;1</sup></td>
</tr>
<tr>
<td valign="top" align="left"><italic>d<sub>1</sub></italic></td>
<td valign="top" align="left">Dissociation constant for IP3</td>
<td valign="top" align="left">0.13 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>d<sub>2</sub></italic></td>
<td valign="top" align="left">Inactivation dissociation constant of Ca<sup>2+</sup></td>
<td valign="top" align="left">1.049 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>d<sub>3</sub></italic></td>
<td valign="top" align="left">Inactivation dissociation constant of IP<sub>3</sub></td>
<td valign="top" align="left">0.9434 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>d<sub>5</sub></italic></td>
<td valign="top" align="left">Ca<sup>2+</sup> activation constant</td>
<td valign="top" align="left">0.08234 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left"><italic>a<sub>2</sub></italic></td>
<td valign="top" align="left">Ca<sup>2+</sup> inhibition constant</td>
<td valign="top" align="left">0.2 s<sup>&#x2013;1</sup></td>
</tr>
<tr>
<td valign="top" align="left"><italic>k</italic></td>
<td valign="top" align="left">The cooperativity coefficient</td>
<td valign="top" align="left">4</td>
</tr>
<tr>
<td valign="top" align="left"><italic>g</italic></td>
<td valign="top" align="left">Concentration of glutamate</td>
<td valign="top" align="left">1 &#x03BC;M</td>
</tr>
<tr>
<td valign="top" align="left">&#x03B1;</td>
<td valign="top" align="left">The relative effect of Ca<sup>2+</sup> stimulation of PLC&#x03B4; on IP<sub>3</sub> production</td>
<td valign="top" align="left">0.8</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k</italic><sub><italic>VGCC</italic></sub></td>
<td valign="top" align="left">The strength of the influence of A&#x03B2; on VGCCs</td>
<td valign="top" align="left">10</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k</italic><sub><italic>in</italic></sub></td>
<td valign="top" align="left">The strength of the influence of A&#x03B2; on A&#x03B2; channels</td>
<td valign="top" align="left">1</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k</italic><sub><italic>RyR</italic></sub></td>
<td valign="top" align="left">The strength of the influence of A&#x03B2; on RyRs</td>
<td valign="top" align="left">0.2</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k</italic><sub><italic>PLC&#x03B2;</italic></sub></td>
<td valign="top" align="left">The strength of the influence of A&#x03B2; on glutamate-dependent IP<sub>3</sub> production</td>
<td valign="top" align="left">0.05</td>
</tr>
<tr>
<td valign="top" align="left"><italic>k</italic><sub><italic>PLC&#x03B4;</italic></sub></td>
<td valign="top" align="left">The strength of the influence of A&#x03B2; on Ca<sup>2+</sup>-dependent IP<sub>3</sub> production</td>
<td valign="top" align="left">0.5</td>
</tr>
<tr>
<td valign="top" align="left">[<italic>K</italic><sup>+</sup>]<sub><italic>o</italic></sub></td>
<td valign="top" align="left">Extracellular K<sup>+</sup> concentration</td>
<td valign="top" align="left">3&#x2013;5 mM</td>
</tr>
<tr>
<td valign="top" align="left">[<italic>K</italic><sup>+</sup>]<sub><italic>i</italic></sub></td>
<td valign="top" align="left">Intracellular K<sup>+</sup> concentration</td>
<td valign="top" align="left">130 mM</td>
</tr>
<tr>
<td valign="top" align="left">&#x03B5;</td>
<td valign="top" align="left">Modulation factor</td>
<td valign="top" align="left">17 mV</td>
</tr>
<tr>
<td valign="top" align="left"><italic>g<sub>T</sub></italic></td>
<td valign="top" align="left">Steady conductance of T-type channel</td>
<td valign="top" align="left">0.06 pS</td>
</tr>
<tr>
<td valign="top" align="left"><italic>g<sub>L</sub></italic></td>
<td valign="top" align="left">Steady conductance of L-type channel</td>
<td valign="top" align="left">3.5 pS</td>
</tr>
<tr>
<td valign="top" align="left"><italic>g<sub>N</sub></italic></td>
<td valign="top" align="left">Steady conductance of N-type channel</td>
<td valign="top" align="left">0.39 pS</td>
</tr>
<tr>
<td valign="top" align="left"><italic>g<sub>R</sub></italic></td>
<td valign="top" align="left">Steady conductance of R-type channel</td>
<td valign="top" align="left">0.2225 pS</td>
</tr>
<tr>
<td valign="top" align="left">[<italic>Ca</italic><sup>2 +</sup>]<sub><italic>o</italic></sub></td>
<td valign="top" align="left">Extracellular Ca<sup>2+</sup> concentration</td>
<td valign="top" align="left">1.5 mM</td>
</tr>
</tbody>
</table></table-wrap>
</sec>
<sec id="S2.SS3">
<title>Sensitivity and Robustness Analysis</title>
<p>Robustness characterizes the ability to maintain performance in the face of perturbations while sensitivity characterizes the ability of living organisms to adequately react to certain stimulus. The two concepts are interlinked. In deterministic modeling, robustness is usually quantified by calculating sensitivity, e.g., period and amplitude sensitivity in quantifying robustness of circadian rhythms (<xref ref-type="bibr" rid="B28">Dubitzky et al., 2013</xref>). In this study, our model is highly sensitive to certain parameters and the oscillatory responses presented here only occur under certain scenarios. Therefore, a simple local sensitivity analysis was performed to assess the sensitivity of the model output, i.e., [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and frequency, to variation in parameters determining the contribution of various fluxes and those representing the effect of therapy. We followed the Morris screening method in which only one input parameter <italic>x<sub>i</sub></italic> is modified between two successive runs of the model. The change of the output induced onto the model objective function <italic>y</italic>(<italic>x</italic>)=(<italic>x</italic><sub>1</sub>,<italic>x</italic><sub>2</sub>,,<italic>x</italic><sub><italic>n</italic></sub>), can then be unambiguously attributed to such a modification of <italic>x<sub>i</sub></italic>. Therefore, the sensitivity <italic>S</italic> of an oscillatory amplitude and frequency to changes in model parameters <italic>P</italic> can be quantified by:</p>
<disp-formula id="S2.Ex2">
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<p>where &#x25B3;<italic>Output</italic> represents the changes of the model output induced by the changes in input parameters, and &#x25B3;<italic>P</italic><sub><italic>change</italic></sub> is the changes in input parameters between two runs of the model. Each parameter was allowed to vary around its control value and the model was solved for each parameter change.</p>
</sec>
</sec>
<sec sec-type="results" id="S3">
<title>Results</title>
<p>Our simulations show that A&#x03B2; can trigger disruptions of cytosolic Ca<sup>2+</sup> levels through interactions between various mechanisms, or, the single components. Each pathway exhibits different characteristics with the influence of A&#x03B2;. Changes in astrocyte resting membrane potential (RMP) were considered and incorporated into our model. With the intention of restoring dysregulated calcium signals, some therapeutic measures were tested, and the multi-pathway involved &#x201C;combination therapy&#x201D; gained effective recovery.</p>
<sec id="S3.SS1">
<title>A&#x03B2; Impairs Ca<sup>2+</sup> Homeostasis in Astrocytes</title>
<p>Calcium oscillations in astrocytes are crucial signaling pathways with multiple roles in several brain functions (<xref ref-type="bibr" rid="B59">Riera et al., 2011a</xref>). <xref ref-type="bibr" rid="B19">Charles et al. (1991)</xref> have reported the [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> oscillations in glial cells with the peak amplitude of 0.6&#x2013;0.8 &#x03BC;M induced by mechanical and glutamate stimulations. <xref ref-type="bibr" rid="B52">Parri and Crunelli (2001)</xref> found a subset of spontaneously active thalamic astrocytes exhibits [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> oscillations with an average frequency of 0.019 Hz. Here, our model produced typical calcium oscillations of approximately 0.6 &#x03BC;M in amplitude and 0.03 Hz in frequency without A&#x03B2; (<xref ref-type="fig" rid="F2">Figure 2</xref>) which is consistent with the experimental data suggesting the physiological agreement of our biophysical model.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption><p>The effect of A&#x03B2; on cytosolic Ca<sup>2+</sup> dynamics. <bold>(A)</bold> The time course of Ca<sup>2+</sup> dynamics at different A&#x03B2; levels (0, 0.2, 0.4, 0.6, and 0.8). <bold>(B)</bold> Bifurcation diagram of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> plotted against the A&#x03B2; level, <italic>a</italic>. <bold>(C)</bold> The frequency of Ca<sup>2+</sup> oscillations plotted against the A&#x03B2; level, <italic>a</italic>.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-767892-g002.tif"/>
</fig>
<p>A&#x03B2; has been shown to impair intracellular Ca<sup>2+</sup> homeostasis in our simulations. <xref ref-type="fig" rid="F2">Figure 2A</xref> describes the cytosolic Ca<sup>2+</sup> with different A&#x03B2; levels. We can clearly observe the increasing amplitude and frequency with elevated A&#x03B2;. The intracellular calcium signals would change into a high steady state if there is excessive A&#x03B2;. In <xref ref-type="fig" rid="F2">Figures 2B,C</xref>, we performed analyses on bifurcation features and variations of frequency to study the dynamical influence of A&#x03B2; on Ca<sup>2+</sup>. At a low level of A&#x03B2;, that is, 0 &#x003C; <italic>a</italic> &#x003C; 0.3, which we assumed to represent an early or milder state of the disease, the oscillation amplitude increases while the frequency changes little. At a middle A&#x03B2; level (0.3 &#x003C; <italic>a</italic> &#x003C; 0.6), the oscillation frequency has a rapid increase. For a higher level of A&#x03B2; (<italic>a</italic> &#x003E; 0.6), which represents a later or more severe stage of the disease, astrocytic Ca<sup>2+</sup> dynamics become the high steady state in which the calcium concentration has an explosive increase.</p>
<p>Since A&#x03B2; has such significant effects, we continued to test parameters representing the strength of A&#x03B2; on each pathway. Illustrated in <xref ref-type="fig" rid="F3">Figures 3A&#x2013;E</xref> are bifurcation analysis for this purpose. Regardless of the level of A&#x03B2;, the effect on VGCCs is minimal because both amplitude and frequency show good robustness against <italic>k</italic><sub><italic>VGCC</italic></sub> (<xref ref-type="fig" rid="F3">Figure 3A</xref>). Nevertheless, A&#x03B2; channels makes an obvious influence with increasing A&#x03B2;. Both [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and frequency markedly vary in oscillation or steady state (<xref ref-type="fig" rid="F3">Figure 3B</xref>). <xref ref-type="fig" rid="F3">Figure 3C</xref> displays the effect of <italic>k</italic><sub><italic>RyR</italic></sub>, showing that [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> is relatively robust against large <italic>k</italic><sub><italic>RyR</italic></sub> whereas the frequency is quite the opposite. On balance, <italic>k</italic><sub><italic>RyR</italic></sub> induced alterations are minor. <xref ref-type="fig" rid="F3">Figures 3D,E</xref> are the effects of parameters related to IP<sub>3</sub> production and their influence is essentially similar. Increasing IP<sub>3</sub> can make elevated frequency but slightly decreased [Ca<sup>2+</sup>]<sub><italic>i</italic></sub>. They both do not affect the steady state. Besides, we also considered other indirect parameters. Their sensitivities which are calculated for parameter variations of &#x00B1; 10% are shown in <xref ref-type="fig" rid="F3">Figures 3F,G</xref>. A small change in <italic>k<sub>2</sub></italic> can cause a significant decrease in [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and increase in frequency, while the rate of ER leakage (<italic>v<sub>2</sub></italic>) acts as the same role but is less sensitive than <italic>k<sub>2</sub></italic>. Another leak flux <italic>J</italic><sub><italic>in</italic></sub> has a positive effect on both sides. Some other parameters here with low sensitivity are not discussed further.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption><p>The effect of various parameters on cytosolic Ca<sup>2+</sup> dynamics. <bold>(A&#x2013;E)</bold> Bifurcation diagrams of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> plotted against the strength of A&#x03B2; acting on different pathways. <bold>(F)</bold> Amplitude sensitivity of Ca<sup>2+</sup> dynamics. The sensitivities are calculated for parameter variations of &#x00B1; 10%. <bold>(G)</bold> Frequency sensitivity of Ca<sup>2+</sup> dynamics. The sensitivities are calculated for parameter variations of &#x00B1; 10%.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-767892-g003.tif"/>
</fig>
<p>In general, various results suggest that A&#x03B2; triggers aberrant calcium signals by increasing [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and frequency. In particular, high levels of A&#x03B2; are more hazardous and can be fatal. These disruptions of calcium oscillations make calcium signaling abnormal and raise the possibility of calcium intoxication (<xref ref-type="bibr" rid="B48">Mattson and Chan, 2003</xref>).</p>
</sec>
<sec id="S3.SS2">
<title>Contribution of A&#x03B2; on Ca<sup>2+</sup> Dynamics Through Different Pathways</title>
<p>The above results have revealed how the multiple A&#x03B2;-affected pathways interact and collectively contribute to Ca<sup>2+</sup> dysregulation. However, we remained curious about the alterations in these pathways, and therefore, we next separated these pathways and examined, in isolation, how A&#x03B2; alters these pathways and causes abnormalities in cytosolic Ca<sup>2+</sup>. So, we denoted whether A&#x03B2; affects calcium flux by changing the strength of the effect of A&#x03B2; on the individual pathways (i.e., <italic>k</italic><sub><italic>VGCC</italic></sub>, <italic>k</italic><sub><italic>in</italic></sub>, <italic>k</italic><sub><italic>RyR</italic></sub>, <italic>k</italic><sub><italic>PLC&#x03B2;</italic></sub> and <italic>k</italic><sub><italic>PLC&#x03B4;</italic></sub>) to 0 or 1 and described the dynamics of varying the parameter <italic>a</italic>, meaning how A&#x03B2; acts on a single pathway.</p>
<p>We examined the effect of each pathway on cytosolic Ca<sup>2+</sup> dynamics by analyzing bifurcation and frequency. The results are shown in <xref ref-type="fig" rid="F4">Figure 4</xref>. Diagram indicates that large amounts of A&#x03B2; are required to elicit changes in intracellular Ca<sup>2+</sup> activity when acting on VGCCs; even at steady state, the effects of A&#x03B2; are slow (<xref ref-type="fig" rid="F4">Figure 4A</xref>). This illustrates that [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> are robust to changes in <italic>J</italic><sub><italic>VGCC</italic></sub>. In contrast, slight A&#x03B2; acting on the formed channels is able to disrupt normal astrocytic calcium oscillations and enables [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> at steady state to grow rapidly as well. When <italic>a</italic> &#x003C; 0.3, the frequency essentially exhibits unchanged behavior. Then the frequency increased significantly as A&#x03B2; became larger. <xref ref-type="fig" rid="F4">Figure 4C</xref> illustrates the effect of <italic>J</italic><sub><italic>RyR</italic></sub>. We can observe the increased amplitude of oscillation, stable and unchanged low steady state concentration, and reduced frequency, especially when <italic>a</italic> &#x003E; 0.3, where a sharp decrease in frequency occurs. <xref ref-type="fig" rid="F4">Figure 4D</xref> shows that A&#x03B2;-mediated IP<sub>3</sub> production leads to the decrease of calcium oscillation amplitude and the increase of frequency, but this effect gradually disappears with the increase of the A&#x03B2; level. We analyzed the reason and found that when A&#x03B2; increases to a certain value, both <italic>m</italic> and <italic>n</italic> tend to be constant, resulting in no change of <italic>J</italic><sub><italic>CICR</italic></sub> affected by IP<sub>3</sub>, so the whole dynamics gradually tend to be stable.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption><p>Contribution of A&#x03B2; on cytosolic Ca<sup>2+</sup> dynamics through different pathways. <bold>(A&#x2013;D)</bold> Bifurcation diagrams of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> plotted against the A&#x03B2; level with affected pathways.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-767892-g004.tif"/>
</fig>
<p>On the whole, we considered that A&#x03B2; channels and RyRs play a major role in the regulation of intracellular Ca<sup>2+</sup> under the influence of A&#x03B2;, while the other two pathways have little effect.</p>
</sec>
<sec id="S3.SS3">
<title>The Influence of Resting Membrane Potential</title>
<p>Although astrocytes are non-excitable cells, values of RMP reported in different studies may vary in extension to some ones due differences in outside K<sup>+</sup> concentration (<xref ref-type="bibr" rid="B6">Anderson et al., 1995</xref>). Thus, the changes in extracellular K<sup>+</sup> concentration can depolarize the astrocyte and increase the open probability of VGCCs (<xref ref-type="bibr" rid="B11">Bellot-Saez et al., 2017</xref>). Therefore, we simulated how changes in RMP can affect the <italic>J</italic><sub><italic>VGCC</italic></sub> and intracellular Ca<sup>2+</sup> dynamics.</p>
<p>The hyperpolarized RMP of mature astrocytes is set close to the K<sup>+</sup> Nernst potential, approximately &#x2013;80 mV (<xref ref-type="bibr" rid="B73">Verkhratsky and Nedergaard, 2018</xref>). So, we modeled <italic>V<sub>m</sub></italic> as the following form (<xref ref-type="bibr" rid="B75">Wu et al., 2019</xref>):</p>
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</mml:mrow>
</mml:mrow>
<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
</disp-formula>
<p>where <italic>R</italic> is the ideal gas constant, <italic>T</italic> is the absolute temperature, <italic>z<sub>K</sub></italic> is the valence of K<sup>+</sup>, and <italic>F</italic> is Faraday constant. [K<sup>+</sup>]<sub><italic>o</italic></sub> and [<italic>K</italic>]<sub><italic>i</italic></sub> are the extracellular and intracellular K<sup>+</sup> concentrations, respectively. &#x03B5; is a modulation factor.</p>
<p>Now we can examine the effects of changes to RMP by adjusting [<italic>K</italic>]<sub><italic>o</italic></sub>. The impact of such changes in <italic>V<sub>m</sub></italic> and the resulting Ca<sup>2+</sup> dynamics are shown in <xref ref-type="fig" rid="F5">Figures 5</xref>, <xref ref-type="fig" rid="F6">6</xref>.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption><p>Extracellular K<sup>+</sup> increases the frequency of Ca<sup>2+</sup> oscillations through activation of VGCCs. <bold>(A)</bold> The dependency of the astrocytic RMP <italic>V<sub>m</sub></italic> of different [K<sup>+</sup>]<sub><italic>o</italic></sub>. <bold>(B)</bold> Ca<sup>2+</sup> influx through VGCCs at three different RMPs (&#x2013;78, &#x2013;71, and &#x2013;65 mV). <bold>(C)</bold> Cytosolic Ca<sup>2+</sup> dynamics at three different RMPs (&#x2013;78, &#x2013;71, and &#x2013;65 mV). <bold>(D)</bold> Bifurcation diagram of the [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> in cytosol vs. RMP. <bold>(E)</bold> The frequency of the oscillations vs. RMP.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-767892-g005.tif"/>
</fig>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption><p>The influence of A&#x03B2; on Ca<sup>2+</sup> dynamics with RMP. <bold>(A)</bold> Representative traces of Ca<sup>2+</sup> dynamics within the three different A&#x03B2; levels (0.2, 0.4, and 0.6) at different <italic>V<sub>m</sub></italic>: &#x2013;78, &#x2013;71, and &#x2013;65 mV. <bold>(B)</bold> The frequency of Ca<sup>2+</sup> signals vs. A&#x03B2; levels and RMPs. <bold>(C)</bold> The amplitude of Ca<sup>2+</sup> signals vs. A&#x03B2; levels and RMPs.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-767892-g006.tif"/>
</fig>
<p><xref ref-type="fig" rid="F5">Figure 5A</xref> displays the dependence of <italic>V<sub>m</sub></italic> on [<italic>K</italic>]<sub><italic>o</italic></sub>. We then chose three different values of <italic>V<sub>m</sub></italic> with [<italic>K</italic>]<sub><italic>o</italic></sub> of 3, 4, and 5 mM for our following simulations. <xref ref-type="fig" rid="F5">Figure 5B</xref> shows how RMP significantly affect the <italic>J</italic><sub><italic>VGCC</italic></sub>. Both the amplitude and frequency increase with depolarization. These alterations in <italic>J</italic><sub><italic>VGCC</italic></sub> similarly affected [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> (<xref ref-type="fig" rid="F5">Figure 5C</xref>). Through the bifurcation and frequency diagrams in <xref ref-type="fig" rid="F5">Figures 5D,E</xref>, we could observe that before reaching steady state, [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> is very robust to RMP, but after entering steady state, it increases dramatically. In contrast, the frequency consistently shows an increasing trend.</p>
<p>We induced A&#x03B2; and studied the interactions between the two factors. <xref ref-type="fig" rid="F6">Figure 6A</xref> shows the cytosolic Ca<sup>2+</sup> dynamics vs. three different RMP (&#x2212;78, &#x2212;71, and &#x2212;65 mV) and three different A&#x03B2; levels (0.2, 0.4, and 0.6). In <xref ref-type="fig" rid="F6">Figures 6B,C</xref>, we show the analysis of the frequency and amplitude of cytosolic Ca<sup>2+</sup> dynamics, respectively. For the range where oscillation emerged (about &#x2212;80 to &#x2212;64 mV), the higher the RMP, the more profoundly affected by A&#x03B2;, since only a little A&#x03B2; is required to disrupt the oscillations. However, when at a high A&#x03B2; level, the range rapidly narrowed and eventually disappeared, indicating that the astrocytes will always be in the steady state with a high [Ca<sup>2+</sup>]<sub><italic>i</italic></sub>. In the research scope, increasing A&#x03B2; and RMP will lead to the increase of amplitude and frequency, in which the influence of the two on the amplitude is close while A&#x03B2; has a more significant contribution to the increase of calcium amplitude than the RMP.</p>
</sec>
<sec id="S3.SS4">
<title>Blocking A&#x03B2;-Affected Pathways Benefits the Recovery of Calcium Homeostasis</title>
<p>At present, the treatment of AD remains a challenging research hotspot. There are four FDA-approved prescription drugs (<xref ref-type="bibr" rid="B71">Vaz and Silvestre, 2020</xref>) that show some effectiveness; however, they only relieve symptoms. Here, we tested the effects of blocking channels, receptors and products affected by A&#x03B2; as described above. We characterized the effect of recovery as a function of the blocking ratio of specific parameters and investigated their respective sensitivities at three different A&#x03B2; levels of <italic>a</italic> = 0.2, <italic>a</italic> = 0.4 and <italic>a</italic> = 0.6, which represented different stages of the disease. Results are shown in <xref ref-type="fig" rid="F7">Figure 7</xref>.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption><p>Effect of blocking channels, receptors, and products. <bold>(A&#x2013;D)</bold> The changes in amplitude and frequency after different blocking ratios of related channels, receptors, and products. The green dashed line represents the absence of A&#x03B2;. <bold>(E)</bold> Amplitude sensitivity of recovery effect. The sensitivities are calculated by the slope in <bold>(A&#x2013;D)</bold>. <bold>(F)</bold> Frequency sensitivity of recovery effect. The sensitivities are calculated by the slope in <bold>(A&#x2013;D)</bold>.</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-767892-g007.tif"/>
</fig>
<p>If we blocked VGCCs, as you can see in <xref ref-type="fig" rid="F7">Figure 7A</xref>, therapy of this pathway shows a weak effect to the recovery of [Ca<sup>2+</sup>]<sub><italic>i.</italic></sub> For frequency, this method can restore the frequency to normal at the low level of A&#x03B2; (<italic>a</italic> = 0.2), but when at the high level, even the channel is completely blocked, it fails to do so. Inhibition of membrane leak flux obtains effective results with the ability to reduce the frequency and amplitude of abnormal rise (<xref ref-type="fig" rid="F7">Figure 7B</xref>). Blocking RyRs has a certain effect on the recovery of elevated [Ca<sup>2+</sup>]<sub><italic>i</italic></sub>, but the recovery is not obvious and even has an adverse effect at a higher A&#x03B2; level for frequency (<xref ref-type="fig" rid="F7">Figure 7C</xref>). Reducing the production rate of IP<sub>3</sub> can help to low down the increased frequency. However, this way contributes to decreasing [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> only at high inhibition ratio (<xref ref-type="fig" rid="F7">Figure 7D</xref>). Illustrated in <xref ref-type="fig" rid="F7">Figures 7E,F</xref> are quantitative sensitivity analysis of the recovery of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and frequency, respectively. Overall, targeting <italic>J</italic><sub><italic>in</italic></sub> has the best effect, followed by RyR blockade, and blocking VGCCs has the least effect.</p>
<p>In <xref ref-type="fig" rid="F8">Figure 8</xref>, different strategies based on our sensitivity analysis are applied to restore calcium homeostasis for two different situations (<italic>a</italic> = 0.2 and <italic>a</italic> = 0.6). When <italic>a</italic> = 0.2 representing the early stage of the disease, there exists significant variation in frequency. However, the abnormal signals can recover to some extent by simply inhibited the RyR pathway by 80% (<xref ref-type="fig" rid="F8">Figure 8A</xref>). When <italic>a</italic> = 0.6 representing the advanced stage of the disease in which both frequency and [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> are markedly affected, targeting only one pathway is powerless. With the &#x201C;combination therapy&#x201D;, we can not only get the ideal recovery effect, but also carry out the treatment with more than one strategy (<xref ref-type="fig" rid="F8">Figure 8B</xref>).</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption><p>The cytosolic Ca<sup>2+</sup> dynamics after treatment. <bold>(A)</bold> Effect of single therapy at the early stage of AD. Top, <italic>a</italic> = 0. Middle, <italic>a</italic> = 0.2. Bottom, <italic>a</italic> = 0.2 + single therapy. <bold>(B)</bold> Effect of &#x201C;combination therapy&#x201D; at the advanced stage of AD. Top, <italic>a</italic> = 0. Middle, <italic>a</italic> = 0.6. Bottom, <italic>a</italic> = 0.6 + two different &#x201C;combination therapies.&#x201D;</p></caption>
<graphic mimetype="image" mime-subtype="tiff" xlink:href="fphys-12-767892-g008.tif"/>
</fig>
</sec>
</sec>
<sec sec-type="discussion" id="S4">
<title>Discussion</title>
<p>With a rapidly aging population, AD has become a major public health concern. However, the causation of AD remains unclear. Dysregulation of astrocytic Ca<sup>2+</sup> has been widely regarded as an important component of AD. While controversy still remains, because some researches have not found acute [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> responses to A&#x03B2; (<xref ref-type="bibr" rid="B18">Casley et al., 2009</xref>; <xref ref-type="bibr" rid="B69">Toivari et al., 2011</xref>), this could possibly be attributed to the variability of A&#x03B2; species (monomers, oligomers, fibrils) and astrocyte types (from different brain areas) (<xref ref-type="bibr" rid="B43">Lim et al., 2014</xref>). More experiments reported that A&#x03B2; triggered transient [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> increases or [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> oscillations in astrocytes (<xref ref-type="bibr" rid="B36">Jalonen et al., 1997</xref>; <xref ref-type="bibr" rid="B1">Abramov et al., 2003</xref>; <xref ref-type="bibr" rid="B3">Alberdi et al., 2013</xref>; <xref ref-type="bibr" rid="B43">Lim et al., 2014</xref>). Unfortunately, the interactions of various mechanisms make it difficult to precisely understand how A&#x03B2; impacts cytosolic Ca<sup>2+</sup> levels and individual fluxes. Decoupling various components and integrating their contributions into a full view may help us better understand the complexity of A&#x03B2; mechanisms in intracellular calcium dysregulation.</p>
<p>Computational modeling is a powerful approach that provides great opportunities to study complex mechanisms since it is experimentally difficult to isolate each component for separate studies. Our previous work on bioRxiv (<xref ref-type="bibr" rid="B33">Gao et al., 2020</xref>) has proposed a model related to AD focusing on the effect of A&#x03B2; through four different pathways on cytosolic Ca<sup>2+</sup>. Although we have considered a multi-pathway model, there is still room for more in-depth study of the individual contribution of A&#x03B2; on each pathway and methods of restoring the disrupted signals. There are also some limitations to the model itself. Specifically, for example, our prior study has only included the PLC&#x03B4;-dependent production while IP<sub>3</sub> is regulated by two entirely different pathways in astrocytes. Also, differences in volume of cytosol and ER, and changes in membrane potential were neglected. These all deserve rigorous consideration and continued refinement.</p>
<p>In this paper, we modified and extended the previous studies in conjunction with experimental data and a comprehensive model was proposed. Not only all the issues mentioned are considered, but also the model is more physiologically reasonable. Just as important, the brevity and universality of the modeling method are worth noting. We previously used Lavrentovich&#x2019;s model (<xref ref-type="bibr" rid="B40">Lavrentovich and Hemkin, 2008</xref>) to describe CICR dynamics depended on [IP<sub>3</sub>] and [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> from both the ER and cytosol. However, a form simplified from De Young&#x2019;s model (<xref ref-type="bibr" rid="B24">De Young and Keizer, 1992</xref>) by Li (<xref ref-type="bibr" rid="B41">Li and Rinzel, 1994</xref>) based on the gating of IP<sub>3</sub>R provides good agreement with experimental recordings of channel opening and is more suitable for biophysical modeling. These, then, make a model more compatible with physiological data, providing good foundations for simulation studies of AD-induced dysregulation of astrocytic Ca<sup>2+</sup>.</p>
<p>In the experimental studies, <xref ref-type="bibr" rid="B36">Jalonen et al. (1997)</xref> exposed astrocytes to 1 &#x03BC;M A&#x03B2; and found that transient increase in [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> rose from about 0.6 to 0.9 &#x03BC;M. <xref ref-type="bibr" rid="B65">Takano et al. (2007)</xref> reported that after the injection of A&#x03B2; in both Dutch/Iowa mice and controls, the frequency of astrocytic Ca<sup>2+</sup> oscillations increased significantly and became approximately three times as the control group. In our model, similar results were observed. The [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and frequency are about 0.83 &#x03BC;M and 0.12 Hz when <italic>a</italic> = 0.6, compared to 0.58 &#x03BC;M and 0.034 Hz when <italic>a</italic> = 0. This means that our model has a good physiological agreement. Besides, we also found that the accumulation of A&#x03B2; not only leads to the increase of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and frequency in astrocytes, but also makes a transition from oscillation to a high steady state after exceeding a certain threshold, in which, the intracellular [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> will remain at a very high level, and this level will continue to rise rapidly with the increase of A&#x03B2;. In AD, the high intracellular [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> directly impacts memory formation and consolidation (<xref ref-type="bibr" rid="B12">Berridge, 2014</xref>).</p>
<p>Upregulation of astrocytic VGCCs expression in astrocytes has been indicated in pathological conditions, especially the L-Type in AD. Our model shows that VGCCs may contribute less to the dysregulation of cytosolic Ca<sup>2+</sup> levels. This is because [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> is very robust either under high strength of the effect of A&#x03B2; or a large amount of A&#x03B2;. Even when there is a clear change in frequency, the sensitivity is low relative to the changes in A&#x03B2;. In response to the disruptions, <xref ref-type="bibr" rid="B7">Anekonda et al. (2011)</xref> have demonstrated that L-type Ca<sup>2+</sup> current blockers can protect cells from the inductive effect of A&#x03B2;. We did confirm the efficacy of blocking VGCCs, but the recovery was not significant enough.</p>
<p>A&#x03B2; has been shown to impair the membrane permeability, due to the A&#x03B2;-formed pores resulting in the increase of Ca<sup>2+</sup> influx through the membrane (<xref ref-type="bibr" rid="B26">Demuro et al., 2010</xref>). This additional influx shows damage to astrocytic homeostasis in our simulations. Especially, when oscillations disappear and the astrocyte calcium level is at a high steady state, A&#x03B2; can cause dramatic increases in [Ca<sup>2+</sup>]<sub><italic>i</italic></sub>. In fact, channel formation has been already proposed as a molecular mechanism for A&#x03B2; toxicity in the early 1990s (<xref ref-type="bibr" rid="B8">Arispe et al., 1993</xref>), and our model, in the light of physiology, has well reflected how ionic leakage strongly affects and rapidly disrupts the cellular homeostasis. This intense pathology can be treated with Zn<sup>2+</sup> (<xref ref-type="bibr" rid="B1">Abramov et al., 2003</xref>). We demonstrated that blocking the channel achieves desirable effects and may serve as a promising therapeutic approach.</p>
<p>Although disruptions on the membrane by A&#x03B2; are believed to be an important mechanism, the intracellular signaling pathways also deserve attention. In this study, we reflect the toxic effects of A&#x03B2; by increasing the channel open probability of RyRs. Other studies also suggested that A&#x03B2; can directly increase the RyR expression (<xref ref-type="bibr" rid="B63">Supnet et al., 2006</xref>). The increasing [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> and unchanged low steady state were observed. Unlike the other pathways, A&#x03B2; caused a decrease in frequency, which was more rapid in the presence of large amounts of A&#x03B2; because of the occurrence of mixed oscillations. Research has reported that RyR-mediated Ca<sup>2+</sup> release can be reduced after treatment with RyR inhibitor (<xref ref-type="bibr" rid="B51">Oul&#x00E8;s et al., 2012</xref>). Results showed a significant therapeutic effect on abnormal high [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> in our study.</p>
<p>Accumulated evidence indicates that A&#x03B2; is involved in the regulation of IP<sub>3</sub> production in AD (<xref ref-type="bibr" rid="B25">Demuro and Parker, 2013</xref>; <xref ref-type="bibr" rid="B37">Jensen et al., 2013</xref>). In this paper, we considered both A&#x03B2;-mediated channels or receptors, as well as non-directly acting intermediates such as IP<sub>3</sub>, which embodies the concept of &#x201C;multi-pathway&#x201D; in a true sense and illustrates the complexity of our model. According to the results of the simulation, increasing IP<sub>3</sub> levels can lead to the decrease of [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> but the increase of frequency. The recovery effect is stronger than the blockage of VGCCs but not as effective as the other two pathways. Reducing the intracellular IP<sub>3</sub> level has a certain effect on frequency recovery, but the recovery effect on [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> is not ideal. This may reveal that IP<sub>3</sub> mainly regulates the frequency of intracellular calcium signals.</p>
<p>The RMP of astrocytes is also a contributing factor within our consideration. Compared to their neuronal counterparts, astrocytes display a highly negative RMP (<xref ref-type="bibr" rid="B14">Bolton et al., 2006</xref>). Some studies have shown that [K<sup>+</sup>]<sub><italic>o</italic></sub> is critical in establishing the RMP of astrocytes (<xref ref-type="bibr" rid="B6">Anderson et al., 1995</xref>; <xref ref-type="bibr" rid="B11">Bellot-Saez et al., 2017</xref>). However, defective extracellular K<sup>+</sup> clearance mechanisms have also been observed in AD which led to the loss of astrocyte polarization (<xref ref-type="bibr" rid="B50">Olabarria et al., 2010</xref>). Our model shows that increasing [K<sup>+</sup>]<sub><italic>o</italic></sub> contributes to astrocyte depolarization, which to some extent reflects the impairment of astrocyte polarization by abnormal accumulation of [K<sup>+</sup>]<sub><italic>o</italic></sub> in AD. During the process of depolarization, the amplitude of transmembrane Ca<sup>2+</sup> flow mediated by VGCCs, as well as frequency increases. The affected <italic>J</italic><sub><italic>VGCC</italic></sub>, in turn, will cause further damage to cytosolic Ca<sup>2+</sup> dynamics, manifested primarily by a large increase in [Ca<sup>2+</sup>]<sub><italic>i</italic></sub> at steady state and a marked increase in frequency. This finding suggests that the frequency of Ca<sup>2+</sup> events can be increased by depolarization of astrocytes, through activating of VGCCs. On the other hand, the accumulation of A&#x03B2; can narrow the range of membrane potential where oscillations are triggered. This may indicate the destructive nature of A&#x03B2; to synchronization oscillation of astrocyte network. Besides, astrocyte RMP displays extensive heterogeneity in the central nervous system (<xref ref-type="bibr" rid="B49">McNeill et al., 2021</xref>). To a certain extent, our model also reflects the characteristics of astrocytes with different RMP.</p>
<p>Finding a cure for AD is one of the most urgent and difficult tasks in modern medicine. At present, the drugs that are used to treat AD can only relieve symptoms but cannot slow down or reverse the progression of the disease (<xref ref-type="bibr" rid="B5">Alzheimer&#x2019;s Association, 2020</xref>). The recent development and FDA approval of the AD drug Aducanumab, which targets A&#x03B2;, caused a great controversy (<xref ref-type="bibr" rid="B71">Vaz and Silvestre, 2020</xref>). But there is no doubt that drug research targeting A&#x03B2; or Tau proteins has once fallen into a bottleneck (<xref ref-type="bibr" rid="B20">Congdon and Sigurdsson, 2018</xref>; <xref ref-type="bibr" rid="B31">Foroutan et al., 2019</xref>), so it is advisable to explore feasible therapies from the perspective of Ca<sup>2+</sup> dynamics. Mounting evidence has demonstrated that calcium signals play an indispensable role in AD (<xref ref-type="bibr" rid="B76">Yu et al., 2009</xref>), but Ca<sup>2+</sup>-pathway therapeutics remain undeveloped. Our simulations suggested that therapy targeting a specific receptor, channel or product is efficacious but limited because of multiple targets of A&#x03B2;, particularly in the terminal stages of the disease. Meanwhile, combination therapy can perfectly compensate for the shortage of single therapy. Generally, restoring calcium homeostasis is useful and necessary (<xref ref-type="bibr" rid="B43">Lim et al., 2014</xref>). Memantine, approved for the treatment of AD, has been clinically proven to be effective in preventing NMDAR-mediated calcium flux for decades, and here, we have demonstrated that other Ca<sup>2+</sup> pathways in astrocytes may also be potential therapeutic targets and unraveled which Ca<sup>2+</sup> pathway is effective because it is also likely to bring significant side-effects if the pathway is not carefully chosen.</p>
<p>It is challenging to establish a model of A&#x03B2;-mediated multi-pathway calcium dynamics. Although several mechanisms by which A&#x03B2; affects astrocytes have been experimentally demonstrated, how some of these mechanisms occur remains unclear. But the ubiquitous Ca<sup>2+</sup> regulatory fluxes used in our model make it easily applicable for studying various cell types with spatial components. In fact, astrocytes exhibit a very complex morphology suggesting the spatiotemporal characteristics of Ca<sup>2+</sup> signals in different structures (<xref ref-type="bibr" rid="B61">Semyanov et al., 2020</xref>) while we considered a spatially homogeneous astrocyte for better quantifying. However, even by adopting some simplifications, our model includes a large number of parameters, some of which still lack the effectiveness of the verification experiment. Our deterministic model generated regular calcium oscillations, which is consistent with the situation in some reports (<xref ref-type="bibr" rid="B52">Parri and Crunelli, 2001</xref>; <xref ref-type="bibr" rid="B66">Tashiro et al., 2002</xref>), However, in most cases, the calcium signals observed in the experiments presented clear irregularities which revealed its stochastic nature, meaning that some level of stochasticity may be closer to the physiology. All the deficiencies can be altered in future follow-up work as we continue to improve our understanding of the effects of A&#x03B2; in the astrocytic system. Our codes are publicly available for reproducibility, assisting with fast, convenient, and accurate validation of the model. Moreover, continuous improvement of the model combined with experimental data helps to make the model more useful.</p>
<p>In general, we have presented a hypothetical AD-specific model regarding Ca<sup>2+</sup> dysregulation in astrocytes. The proposed general model incorporates multiple critical individually modeled Ca<sup>2+</sup> mechanisms into a single framework, which obtains a more comprehensive picture compared to present work, especially fewer models are containing VGCCs and RyRs in astrocytes. To our knowledge, this is one of the few computational models to investigate the contribution of various Ca<sup>2+</sup> fluxes to Ca<sup>2+</sup> dynamics including entry and release under the influence of A&#x03B2;. Furthermore, we tested methods of blocking affected pathways. The &#x201C;combination therapy&#x201D; was first proposed and showed the significant effects on restoring calcium homeostasis. This may provide factual predictions for future drug development. Our study can provide an in-depth understanding of AD and pave the way toward the development of much more effective treatment modalities.</p>
</sec>
<sec sec-type="data-availability" id="S5">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="supplementary-material" rid="SM1">Supplementary Material</xref>, further inquiries can be directed to the corresponding author/s.</p>
</sec>
<sec id="S6">
<title>Author Contributions</title>
<p>SC, HG, and AZ conceived and designed the research. LL and HG conducted literature research and wrote MATLAB code. LL, SC, and HG performed simulations and analyzed data and discussed the results and wrote the article with input from AZ. SC supervised the study. LL plotted pictures. All authors contributed to the article and approved the submitted version.</p>
</sec>
<sec sec-type="COI-statement" id="conf1">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="S7">
<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>
</body>
<back>
<sec sec-type="funding-information" id="S8">
<title>Funding</title>
<p>This work was supported by the National Natural Science Foundation of China (Grant No. 91749209), and the Director Fund of WNLO. AZ thanks MRC grant MR/R02524X/1 and the Ministry of Science and Higher Education of the Russian Federation within the framework of state support for the creation and development of World-Class Research Centers &#x201C;Digital biodesign and personalized healthcare&#x201D; No. 075-15-2020-926.</p>
</sec>
<ack>
<p>We would like to thank Dr. Yicheng Xie and Ms. Jinyu Li for helpful suggestions and revisions.</p>
</ack>
<sec id="S9" sec-type="supplementary material"><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/fphys.2021.767892/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fphys.2021.767892/full#supplementary-material</ext-link></p>
<supplementary-material xlink:href="Data_Sheet_1.docx" id="SM1" mimetype="application/vnd.openxmlformats-officedocument.wordprocessingml.document" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
<ref-list>
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