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<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "https://jats.nlm.nih.gov/nlm-dtd/publishing/3.0/journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0" article-type="research-article">
  <front>
    <journal-meta><journal-id journal-id-type="publisher">NHESS</journal-id><journal-title-group>
    <journal-title>Natural Hazards and Earth System Sciences</journal-title>
    <abbrev-journal-title abbrev-type="publisher">NHESS</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Nat. Hazards Earth Syst. Sci.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1684-9981</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/nhess-26-4611-2026</article-id><title-group><article-title>Reliability analysis method for soil slopes permanent displacement under mainshock–aftershock sequences</article-title><alt-title>Reliability analysis method for soil slopes permanent displacement under MAS</alt-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Wang</surname><given-names>Tianyi</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff3">
          <name><surname>Zhang</surname><given-names>Chengda</given-names></name>
          <email>zcd_geo@163.com</email>
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff4">
          <name><surname>Zhang</surname><given-names>Jiangwei</given-names></name>
          <email>zhangjiangwei@tsinghua.edu.cn</email>
        <ext-link>https://orcid.org/0000-0002-3459-5343</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff5">
          <name><surname>Chen</surname><given-names>Su</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff6">
          <name><surname>Dai</surname><given-names>Zhijun</given-names></name>
          <email>dzj@cea-igp.ac.cn</email>
        </contrib>
        <aff id="aff1"><label>1</label><institution>School of Earth Sciences, Hebei GEO University, Shijiazhuang, 052161, China</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Key Laboratory of Intelligent Detection and Equipment for Underground Space of Beijing-Tianjin-Hebei Urban Agglomeration, Ministry of Natural Resources, Shijiazhuang, 052161, China</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>519 Team of North China Geological Exploration Bureau, Tianjin North China Geological Exploration Bureau, Baoding, 071051, China</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>State Key Laboratory of Hydroscience and Engineering, Tsinghua University, Beijing, 100084, China</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Key Laboratory of Urban Security and Disaster Engineering of the Ministry of Education, Beijing University of Technology, Beijing, 100124, China</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Institute of Geophysics, China Earthquake Administration, Beijing, 100081, China</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Chengda Zhang (zcd_geo@163.com), Jiangwei Zhang (zhangjiangwei@tsinghua.edu.cn), and Zhijun Dai (dzj@cea-igp.ac.cn)</corresp></author-notes><pub-date><day>28</day><month>September</month><year>2026</year></pub-date>
      
      <volume>26</volume>
      <issue>9</issue>
      <fpage>4611</fpage><lpage>4619</lpage>
      <history>
        <date date-type="received"><day>4</day><month>February</month><year>2026</year></date>
           <date date-type="rev-request"><day>17</day><month>April</month><year>2026</year></date>
           <date date-type="rev-recd"><day>1</day><month>September</month><year>2026</year></date>
           <date date-type="accepted"><day>1</day><month>September</month><year>2026</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2026 Tianyi Wang et al.</copyright-statement>
        <copyright-year>2026</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026.html">This article is available from https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026.html</self-uri><self-uri xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026.pdf">The full text article is available as a PDF file from https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026.pdf</self-uri>
      <abstract><title>Abstract</title>

      <p id="d2e159">After a primary seismic event, subsequent aftershocks frequently induce progressive damage to slopes. Evaluating the response of slopes to mainshock–aftershock sequences (MAS) from a probabilistic perspective is crucial for disaster prevention and mitigation. Current research primarily focuses on single mainshock events, and commonly adopts peak ground acceleration (PGA), with limited consideration of the cumulative aftershock effects. This study proposes a PDEM-based reliability framework for soil slopes subjected to MAS. First, the random input field of the MAS is first constructed by integrating theoretical models with real data. Then, considering the peak, cumulative, and spectral characteristics of the MAS, correlation analysis is conducted to identify cumulative absolute velocity (CAV) as the controlling parameter for the soil slope response among the 21 candidate parameters. Finally, based on the probability density evolution method (PDEM), a reliability assessment framework for soil slope behavior under MAS is constructed. Compared with existing methods, the proposed approach more effectively incorporates the effects of aftershocks and enables more accurate reliability assessment of slope permanent displacement under MAS. This study provides a probabilistic framework and methodological approaches for assessing slope stability under MAS.</p>
  </abstract>
    
<funding-group>
<award-group id="gs1">
<funding-source>National Natural Science Foundation of China</funding-source>
<award-id>51908176</award-id>
<award-id>62273315</award-id>
<award-id>52192675</award-id>
</award-group>
</funding-group>
</article-meta>
  </front>
<body>
      

      
<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d2e173">Major seismic events are commonly followed by a series of aftershocks, whose effects on slope stability should not be underestimated. Observations of earthquake-induced damage indicate that aftershocks often act as the final trigger for slope failure (Xu and Huang, 2008; Yin, 2008). As the safety requirements for engineering structures become increasingly stringent, slope stability under MAS has attracted considerable interest from both researchers and engineering practitioners. Li et al. (2009) developed and improved the PDEM framework for analyzing stochastic dynamic systems, providing a systematic approach to nonlinear stochastic dynamic analysis and reliability assessment of large-scale and complex engineering structures. The framework has been widely applied to stochastic dynamic analyses of slopes (Li and Chen, 2017). Building on this work, Pang et al. (2021, 2024) introduced an enhanced generalized-PDEM approach for reliability analysis of complex slopes. Their methodology considers multiple slope parameters and ground motion uncertainties. Additionally, accounting for the spatial variation in soil strength properties, a reliability assessment methodology integrating the Newmark method and PDEM is developed to evaluate the effects of aftershocks and spatial heterogeneity on slope dynamic reliability (Newmark, 1965; Zhou et al., 2023; Wang et al., 2022; Xu et al., 2025). Most existing studies use peak ground acceleration (PGA) as the primary measure of ground motion intensity. Nevertheless, intensity measures based only on peak values may not adequately capture the overall characteristics of MAS ground motions (Ruiz-Garcia and Negrete-Manriquez, 2011; Amiri et al., 2022).</p>
      <p id="d2e176">For characterizing the ground motion random field of the MAS, the Monte Carlo method is a well-established and effective approach (Metropolis and Ulam, 1949; Hu et al., 2018; Nithin et al., 2020; Kim and Sitar, 2013). However, it requires a large number of samples and incomplete probability information of the sample set (Jiang et al., 2021). The random function-dimension reduction simulation technique generates MAS time histories with associated probabilities, thereby forming a complete probabilistic set. These time histories can then be coupled with the PDEM to conduct sophisticated dynamic response and reliability analyses for complex engineering structures subjected to MAS (Liu and Liu, 2017; Liu et al., 2019, 2022).</p>
      <p id="d2e179">Current reliability analysis methods for seismic slopes are predominantly developed for single-mainshock scenarios and therefore may not adequately assess slope reliability under MAS. Moreover, existing studies on sequential ground motions predominantly use PGA as the intensity measure, which may not adequately capture the cumulative damage effect contributed by aftershocks. To address these limitations, this study adopts cumulative absolute velocity (CAV) as the intensity measure for MAS ground motions and develops a reliability analysis framework for the permanent displacement of soil slopes based on the PDEM. The proposed method accounts for the effects of aftershocks and provides a basis for stability assessment and disaster prevention of soil slopes subjected to MAS.</p>

      <fig id="F1" specific-use="star"><label>Figure 1</label><caption><p id="d2e185">Geometric dimensions and mesh division of the slope model.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f01.png"/>

      </fig>

<table-wrap id="T1" specific-use="star"><label>Table 1</label><caption><p id="d2e197">Parameters of the slope.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Soil layer</oasis:entry>
         <oasis:entry colname="col2">Density</oasis:entry>
         <oasis:entry colname="col3">Bulk modulus</oasis:entry>
         <oasis:entry colname="col4">Shear modulus</oasis:entry>
         <oasis:entry colname="col5">Cohesion</oasis:entry>
         <oasis:entry colname="col6">Internal friction angle</oasis:entry>
         <oasis:entry colname="col7">Shear strength</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">(<inline-formula><mml:math id="M1" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kg</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M2" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">MPa</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M3" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">MPa</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M4" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kPa</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6">(°)</oasis:entry>
         <oasis:entry colname="col7"><inline-formula><mml:math id="M5" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kPa</mml:mi></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Soft soil</italic></oasis:entry>
         <oasis:entry colname="col2">1900</oasis:entry>
         <oasis:entry colname="col3">70</oasis:entry>
         <oasis:entry colname="col4">37</oasis:entry>
         <oasis:entry colname="col5">34</oasis:entry>
         <oasis:entry colname="col6">24</oasis:entry>
         <oasis:entry colname="col7">4.2</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>Hardpan</italic></oasis:entry>
         <oasis:entry colname="col2">2000</oasis:entry>
         <oasis:entry colname="col3">875</oasis:entry>
         <oasis:entry colname="col4">560</oasis:entry>
         <oasis:entry colname="col5">120</oasis:entry>
         <oasis:entry colname="col6">42</oasis:entry>
         <oasis:entry colname="col7">120</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Model</title>
      <p id="d2e383">This investigation employs a two-layer slope model to investigate slope response under MAS. Figure 1 shows the double-layer slope model established by referring to Wang et al. (2021). The model is 150 <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> long and 30 <inline-formula><mml:math id="M7" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> high. The grid size <inline-formula><mml:math id="M8" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>L</mml:mi></mml:mrow></mml:math></inline-formula> range from 0.5 to 1.8 <inline-formula><mml:math id="M9" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, with a finer resolution of approximately 0.5 <inline-formula><mml:math id="M10" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> in the potential sliding zone. The soil consists of clay from southwestern China (Yang et al., 2022; Ma et al., 2023; Zhang et al., 2024), and its properties are listed in Table 1.</p>
      <p id="d2e428">This investigation utilizes the finite-difference platform FLAC3D, with soil mechanical behavior characterized through a Mohr–Coulomb constitutive model with a tensile cutoff. Local damping is adopted in this study. Its implementation is given by Eq. (1) (Li and Yang, 2006). Because FLAC3D does not require the assembly of a global stiffness matrix, it is computationally efficient for nonlinear dynamic analysis. This feature makes FLAC3D suitable for simulating the nonlinear dynamic response of slopes. (Hu et al., 2017; Puthanpurayil et al., 2018; Yan et al., 2011).

            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M11" display="block"><mml:mrow><mml:mi mathvariant="italic">ξ</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="italic">π</mml:mi><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e447">Within Eq. (1), the coefficient <inline-formula><mml:math id="M12" display="inline"><mml:mi mathvariant="italic">ξ</mml:mi></mml:math></inline-formula> quantifies localized damping intensity, <inline-formula><mml:math id="M13" display="inline"><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> designates the critical damping fraction, while <inline-formula><mml:math id="M14" display="inline"><mml:mi mathvariant="italic">π</mml:mi></mml:math></inline-formula> maintains its conventional value of 3.14.</p>
      <p id="d2e475">This investigation adopts a 5 % critical damping fraction to replicate energy dissipation characteristics during seismic wave transmission through soil media (Qu et al., 2015), yielding a local damping coefficient of 0.157 according to Eq. (1).</p>

      <fig id="F2" specific-use="star"><label>Figure 2</label><caption><p id="d2e481">Correlation coefficient of MAS ground motion parameters (PGA: peak ground acceleration; PGV: peak ground velocity; PGD: peak ground displacement; <inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mtext>sq</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: squared acceleration; <inline-formula><mml:math id="M16" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mtext>sq</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: squared velocity; <inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mtext>sq</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: squared displacement; <inline-formula><mml:math id="M18" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mtext>rs</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: root square acceleration; <inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mtext>rs</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: root square velocity; <inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mtext>rs</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: root square displacement; <inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mi>A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>: Arias intensity; <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>: significant duration; CAV: cumulative absolute velocity; CAD: cumulative absolute displacement; CAI: cumulative absolute impulse; <inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mtext>rms</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: root-mean-square acceleration; <inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mtext>rms</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: root-mean-square velocity; <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mtext>rms</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: root-mean-square displacement; <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>: characteristic intensity; <inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:msub><mml:mtext>Sa</mml:mtext><mml:mtext>Ts</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: response spectral acceleration at natural vibration period <inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mtext>Sa</mml:mtext><mml:mtext>1.5Ts</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>: response spectral acceleration at 1.5 <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">s</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>; ASI: acceleration spectral intensity.).</p></caption>
          <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f02.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>Reliability analysis method of slope under MAS</title>
      <p id="d2e676">Based on the principle of probability conservation, generalized density evolution equations can be derived for the analysis of stochastic dynamic systems. By combining these equations with the virtual stochastic process method, the probability characteristics of stochastic systems can be modeled. Furthermore, based on the PDEM, the reliability analysis of the permanent displacement of the slope under the MAS action is realized (Li and Chen, 2008; Liu and Liu, 2017; Jiang et al., 2021). The main steps are as follows: <list list-type="custom"><list-item><label>1.</label>
      <p id="d2e681">The measured data of the MAS were statistically analyzed to obtain the frequency-domain energy distribution function curves for each ground motion. Employing optimal square approximation criteria, we determine the parameter vector <inline-formula><mml:math id="M31" display="inline"><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:math></inline-formula> defining each evolving power spectral density function. The MAS dataset in this research is modeled as zero-mean, fully non-stationary processes characterized by an evolutionary power spectral density (EPSD) model. The discrete representative points of each ground motion are expressed as <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">q</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">q</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">q</mml:mi></mml:mrow></mml:msub><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="italic">θ</mml:mi><mml:mrow><mml:mi>s</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">q</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M33" display="inline"><mml:mi>q</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M34" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">96</mml:mn></mml:mrow></mml:math></inline-formula>), with the corresponding probabilities given in Eq. (2):<disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M36" display="block"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>q</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mo>∫</mml:mo><mml:mrow><mml:mi>V</mml:mi><mml:mi>q</mml:mi></mml:mrow></mml:msub><mml:mi>p</mml:mi><mml:mi mathvariant="normal">Θ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:math></disp-formula></p></list-item><list-item><label>2.</label>
      <p id="d2e814">Within the framework of reliability analysis based on PDEM, it is essential to identify a ground-motion parameter that exhibits the strongest correlation with slope displacement responses under MAS. We have demonstrated that among the 21 parameters considered in three categories – namely, peak types (PGA, PGV, PGD), spectral characteristics (<inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:msub><mml:mtext>Sa</mml:mtext><mml:mtext>Ts</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mtext>Sa</mml:mtext><mml:mtext>1.5Ts</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, ASI), and cumulative types (<inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mtext>sq</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mtext>sq</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mtext>sq</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mtext>rs</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mtext>rs</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mtext>rs</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mi mathvariant="normal">A</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, CAV, CAD, CAI, <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mtext>rms</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M47" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mtext>rms</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi>d</mml:mi><mml:mtext>rms</mml:mtext></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mi mathvariant="normal">c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M50" display="inline"><mml:mrow><mml:msub><mml:mi>t</mml:mi><mml:mi mathvariant="normal">d</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) – CAV showed the highest correlation coefficient (<inline-formula><mml:math id="M51" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M52" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.872) with the permanent displacement, and more effectively captured the characteristics of aftershocks, as shown in Fig. 2 (Zhang et al., 2024). Consequently, CAV is adopted as the primary intensity measure for slope displacement response under MAS and combined with the PDEM for reliability assessment.</p>
      <p id="d2e987">Based on trial calculations, 96 sets of MAS were scaled to three CAV levels: 12, 28, and 40 <inline-formula><mml:math id="M53" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>. Using the FLAC3D, the slope response under MAS, denoted as <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>X</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">Θ</mml:mi><mml:mi>q</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M55" display="inline"><mml:mi>j</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M56" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M57" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">96</mml:mn></mml:mrow></mml:math></inline-formula>.</p></list-item><list-item><label>3.</label>
      <p id="d2e1069">Based on the above two steps to get assigned to probability <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">q</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and slope of the response results <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>X</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">Θ</mml:mi><mml:mi mathvariant="normal">q</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> probability density evolution Eq. (3):<disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M60" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:mi>X</mml:mi><mml:mi mathvariant="normal">Θ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mover accent="true"><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>m</mml:mi></mml:msubsup><mml:mover accent="true"><mml:mrow><mml:msub><mml:mi>X</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow><mml:mo mathvariant="normal">˙</mml:mo></mml:mover></mml:mrow><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">Θ</mml:mi><mml:mi mathvariant="normal">q</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>×</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:mi>X</mml:mi><mml:mi mathvariant="normal">Θ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">3</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">96</mml:mn></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d2e1263">Within this formulation, <inline-formula><mml:math id="M61" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula> designates system response quantities, <inline-formula><mml:math id="M62" display="inline"><mml:mi mathvariant="normal">Θ</mml:mi></mml:math></inline-formula> encompasses the ensemble of random variables exclusive of initial conditions. <inline-formula><mml:math id="M63" display="inline"><mml:mrow><mml:mi mathvariant="normal">Θ</mml:mi><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi>X</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>,</mml:mo><mml:mover accent="true"><mml:mi mathvariant="normal">Θ</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> represents the vector comprising all stochastic variables within the system; <inline-formula><mml:math id="M64" display="inline"><mml:mrow><mml:mi>X</mml:mi><mml:mo>=</mml:mo><mml:mi>H</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Θ</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> indicates the physical response of <inline-formula><mml:math id="M65" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula>; <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:mi>X</mml:mi><mml:mi mathvariant="normal">Θ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mi mathvariant="italic">θ</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> signifies the joint probability density function (PDF) for <inline-formula><mml:math id="M67" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M68" display="inline"><mml:mi mathvariant="normal">Θ</mml:mi></mml:math></inline-formula>.</p>
      <p id="d2e1372">When <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, the following initial condition is as shown in Eq. (3):<disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M70" display="block"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:mi>X</mml:mi><mml:mi mathvariant="normal">Θ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi mathvariant="normal">|</mml:mi><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">Θ</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1459">In this expression, <inline-formula><mml:math id="M71" display="inline"><mml:mi mathvariant="italic">δ</mml:mi></mml:math></inline-formula> denotes the Dirac delta function, while <inline-formula><mml:math id="M72" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> corresponds to the <inline-formula><mml:math id="M73" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula> value <inline-formula><mml:math id="M74" display="inline"><mml:mrow><mml:mi>t</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>t</mml:mi><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. The PDF of <inline-formula><mml:math id="M75" display="inline"><mml:mi>X</mml:mi></mml:math></inline-formula> at any given time can be derived by summing the contributions from all discrete numerical solutions, as expressed in Eq. (4):<disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M76" display="block"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi>X</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mo movablelimits="false">∫</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mrow><mml:mi>X</mml:mi><mml:mi mathvariant="normal">Θ</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1561">Probability density evolution equations require numerical methods for their solution. Deriving a direct analytical solution to Eq. (4) is mathematically challenging. Conventional practice uses finite-difference schemes to solve the equation.<disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M77" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi>a</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>p</mml:mi><mml:mo>(</mml:mo><mml:mi>z</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1628">First-order Taylor series expansion of Eq. (5), yields approximate differential expressions:<disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M78" display="block"><mml:mrow><mml:msub><mml:mfenced open="[" close="]"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1698">For spatial coordinate <inline-formula><mml:math id="M79" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula>, analogous treatment produces:<disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M80" display="block"><mml:mrow><mml:msub><mml:mfenced close="]" open="["><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∂</mml:mo><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mo>∂</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>z</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula></p>
      <p id="d2e1775">Substitute Eqs. (6) and (7) into Eq. (5):<disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M81" display="block"><mml:mtable class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>-</mml:mo><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:msup><mml:mi>a</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:mfenced open="[" close="]"><mml:mrow><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>p</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mfenced><mml:mtext> or </mml:mtext><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>+</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:msup><mml:mi>a</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:mo>)</mml:mo><mml:msubsup><mml:mi>p</mml:mi><mml:mi>j</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:mi mathvariant="bold-italic">λ</mml:mi><mml:msup><mml:mi>a</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup><mml:msubsup><mml:mi>p</mml:mi><mml:mrow><mml:mi>j</mml:mi><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mi>k</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula></p>
      <p id="d2e1953">Equation (9) is the one-sided difference scheme. Substitute <inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>X</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mi>j</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">Θ</mml:mi><mml:mi mathvariant="normal">q</mml:mi></mml:msub><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> obtained from <inline-formula><mml:math id="M83" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>X</mml:mi><mml:mo mathvariant="normal">˙</mml:mo></mml:mover><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> into Eq. (3), and solve the partial differential equation using the L-W or TVD format of the finite difference method.</p></list-item><list-item><label>4.</label>
      <p id="d2e1998">The PDF of slope displacement response <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi>X</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is obtained numerically through cumulative summation of the joint PDF <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mi mathvariant="italic">_</mml:mi><mml:mi>X</mml:mi><mml:mi mathvariant="normal">Θ</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mi mathvariant="italic">θ</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:mi>q</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>,</mml:mo><mml:mn mathvariant="normal">96</mml:mn></mml:mrow></mml:math></inline-formula>. Subsequently, both PDF and cumulative distribution function (CDF) graphs for slope displacement are developed. These PDF and CDF curves are then used to characterize the statistical distribution of slope displacement and evaluate slope reliability.</p></list-item></list></p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Stochastic simulations of MAS</title>
      <p id="d2e2078">Empirical MAS recordings provide more realistic representations of structural damage and cumulative degradation (Yang et al., 2022). This study uses a diverse set of real earthquake records to reduce the bias associated with specific ground motion types. Through iterative parameter identification based on evolutionary power spectral density modeling, this study combines theoretical models with data-driven methods to construct stochastic seismic inputs. These inputs provide a stochastic loading basis for investigating the effects of MAS on slope reliability.</p>
      <p id="d2e2081">This study selected 96 recorded mainshock–aftershock pairs from 15 seismic events in the NGA-West2 strong-motion database maintained by the Pacific Earthquake Engineering Research Center (PEER). We selected records based on five criteria (Bray and Macedo, 2019; Yeznabad et al., 2022; Yeznabad et al., 2026): (1) the mainshock and its aftershock must belong to the same seismic event, with the aftershock defined as the largest-magnitude event occurring within 12 months after the mainshock; (2) both events have a <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M88" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 5.0 and a PGA <inline-formula><mml:math id="M89" display="inline"><mml:mo>≥</mml:mo></mml:math></inline-formula> 0.05 <inline-formula><mml:math id="M90" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula>; (3) both records are taken from the same component of the same station; (4) the station has an average shear-wave velocity in the upper 30 <inline-formula><mml:math id="M91" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> (Vs30) between 100 and 700 <inline-formula><mml:math id="M92" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>; and (5) the rupture distance of each event does not exceed 80 <inline-formula><mml:math id="M93" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">km</mml:mi></mml:mrow></mml:math></inline-formula>. The 96 MAS records selected according to the above criteria encompass a broad range of sequence-type ground-motion characteristics. However, as these records are derived from the NGA-West2 database and primarily represent shallow crustal earthquakes, the applicability of the results is primarily limited to MAS ground motions from shallow crustal earthquakes.</p>

      <fig id="F3"><label>Figure 3</label><caption><p id="d2e2153">Typical acceleration time history of a MAS.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f03.png"/>

      </fig>

      <fig id="F4" specific-use="star"><label>Figure 4</label><caption><p id="d2e2165">The identification effect of the parameter vector <inline-formula><mml:math id="M94" display="inline"><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:math></inline-formula>. <bold>(a)</bold> The fitting results of the mainshock. <bold>(b)</bold> The fitting results of the aftershock.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f04.png"/>

      </fig>

      <p id="d2e2187">Each MAS adopted a “mainshock <inline-formula><mml:math id="M95" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> 20 <inline-formula><mml:math id="M96" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">s</mml:mi></mml:mrow></mml:math></inline-formula> temporal gap <inline-formula><mml:math id="M97" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> aftershock” configuration to preserve comprehensive non-stationary sequence characteristics (Wang et al., 2022). Figure 3 displays a typical mainshock–aftershock acceleration record from the Whittier Narrows event, with the mainshock and aftershock numbered 589 and 707, respectively, in the NGA-West2 database. In the sensitivity analysis of the 21 MAS ground-motion parameters, the original ground-motion records were used without amplitude scaling. Subsequently, when calculating the permanent displacement of the slope at different CAV levels, the ground-motion amplitudes were scaled to better represent practical engineering conditions.</p>

<table-wrap id="T2"><label>Table 2</label><caption><p id="d2e2215">Identification results of MAS.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Earthquake</oasis:entry>
         <oasis:entry colname="col2">Damping</oasis:entry>
         <oasis:entry colname="col3">Superior</oasis:entry>
         <oasis:entry colname="col4">Time<inline-formula><mml:math id="M98" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>frequency</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">type</oasis:entry>
         <oasis:entry colname="col2">ratio</oasis:entry>
         <oasis:entry colname="col3">circular</oasis:entry>
         <oasis:entry colname="col4">modulation</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">frequency</oasis:entry>
         <oasis:entry colname="col4">function</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><italic>mainshock</italic></oasis:entry>
         <oasis:entry colname="col2">0.32</oasis:entry>
         <oasis:entry colname="col3">14.09</oasis:entry>
         <oasis:entry colname="col4">0.64</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>aftershock</italic></oasis:entry>
         <oasis:entry colname="col2">0.37</oasis:entry>
         <oasis:entry colname="col3">14.64</oasis:entry>
         <oasis:entry colname="col4">0.71</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d2e2320">For the mainshock–aftershock sequences constructed above, frequency-domain energy distribution analysis is performed using an evolutionary power spectrum model for fully non-stationary ground motion processes (Priestley, 1965; Liu and Liu, 2017). The best square approximation criterion and the least square method are adopted to fit the energy distribution curve in the frequency domain. The parameter vector <inline-formula><mml:math id="M99" display="inline"><mml:mi mathvariant="bold-italic">λ</mml:mi></mml:math></inline-formula> is further obtained through inversion and regression. In the process, considering the site damping ratio <inline-formula><mml:math id="M100" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ξ</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> excellence, site soil circular frequency <inline-formula><mml:math id="M101" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ω</mml:mi><mml:mi mathvariant="normal">f</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the influence of a frequency modulation function parameter. The identification results are shown in Fig. 4, and the corresponding data are listed in Table 2. The constructed ground motions can be regarded as zero-mean, real-valued, non-stationary ground motion processes generated by the evolutionary power spectral density function model.</p>

      <fig id="F5" specific-use="star"><label>Figure 5</label><caption><p id="d2e2354">Displacement response distribution of slopes under MAS. The horizontal axis (Ground motioN ID) represents the serial number of ground motion records (ID <inline-formula><mml:math id="M102" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 1–96).</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f05.png"/>

      </fig>


</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Results and analysis</title>
      <p id="d2e2381">To assess slope reliability based on permanent displacement responses, it is necessary to define critical displacement thresholds. Jibson and Michael (2009) classified slope displacement into four ranges for seismic landslide risk evaluation: displacements of 0–1 <inline-formula><mml:math id="M103" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> indicate low risk, 1–5 <inline-formula><mml:math id="M104" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> indicate medium risk, 5–15 <inline-formula><mml:math id="M105" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> indicate high risk, and those exceeding 15 <inline-formula><mml:math id="M106" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">cm</mml:mi></mml:mrow></mml:math></inline-formula> indicate very high risk. For permanent displacement, Ozkan (1998) suggests that the control standard for seismic sliding deformation is 1 <inline-formula><mml:math id="M107" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>. In this study, based on the actual engineering requirements, three slope displacement thresholds of 0.05, 0.25, and 0.50 <inline-formula><mml:math id="M108" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> were selected, corresponding to low-, medium-, and high-level failure states, respectively, to systematically evaluate slope reliability under MAS.</p>

      <fig id="F6"><label>Figure 6</label><caption><p id="d2e2435">Upper bounds of permanent displacement at different CAV and PGA levels.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f06.png"/>

      </fig>

      <p id="d2e2444">Figure 5 shows the distribution of slope permanent displacement under MAS. The distribution is widely dispersed, and the slope displacement response increases with increasing ground motion intensity. When the CAV of the MAS was 12, 28 and 40 <inline-formula><mml:math id="M109" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, respectively, the corresponding average slope permanent displacements were 0.067, 0.328 and 0.633 <inline-formula><mml:math id="M110" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, respectively, which are comparable to the slope displacement results when the PGA of the MAS was 0.4, 0.5 and 0.6 <inline-formula><mml:math id="M111" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula> in reference (Wang et al., 2022). Figure 6 compares the upper bounds of the permanent displacement ranges obtained at three corresponding CAV and PGA levels. It can be observed that, compared with PGA, the use of CAV leads to a more concentrated distribution of permanent displacement results, with the overall dispersion reduced by approximately 40 % on average. These results demonstrate that CAV provides a more concentrated representation of permanent displacement responses. Therefore, CAV is more suitable than the commonly used PGA for characterizing MAS ground motions in the reliability analysis of slope permanent displacement.</p>
      <p id="d2e2481">Nevertheless, even with the use of CAV as the MAS ground-motion intensity measure, the obtained slope displacement responses remain somewhat scattered. This suggests that additional ground-motion parameters – including frequency content and duration – also influence slope permanent displacement (Rathje and Saygili, 2008, 2009; Yeznabad et al.,2022). Given the current lack of a single comprehensive ground-motion parameter that can effectively predict slope displacement responses, the PDEM framework propagates this inherent variability into the reliability estimate, thus rendering a probabilistic treatment indispensable. Building on previous studies, this study develops a reliability probabilistic analysis method based on the PDEM.</p>

      <fig id="F7" specific-use="star"><label>Figure 7</label><caption><p id="d2e2486">Statistical analysis of slope permanent displacement probability under MAS. Probability Density Function (PDF), describing the probability density of permanent displacement, and Cumulative Distribution Function (CDF), representing the cumulative probability of permanent displacement.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f07.png"/>

      </fig>

      <p id="d2e2495">Figure 7 presents the PDF and CDF curves of slope permanent displacement. The PDF curves show the distribution characteristics and main concentration ranges of slope permanent displacement, while the CDF curves provide the cumulative probability at different displacement levels for evaluating slope reliability based on the specified displacement thresholds. The PDF curves shown in Fig. 7a exhibit bimodal or multimodal characteristics, making them difficult to describe using standard distributions such as the normal or lognormal distribution. Under the MAS action of different intensities, the displacements of slopes have diverse distribution patterns, and their probabilities are also not the same. When the CAV is 12 <inline-formula><mml:math id="M112" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, slope permanent displacement ranges from 0 to 0.25 <inline-formula><mml:math id="M113" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, and the slope reliability is 48.5 % at the displacement threshold of 0.05 <inline-formula><mml:math id="M114" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> corresponding to the low failure state. At a CAV of 28 <inline-formula><mml:math id="M115" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, the displacement range expands to 0–1.00 <inline-formula><mml:math id="M116" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, and the slope reliability is 45.5 % at the displacement threshold of 0.25 <inline-formula><mml:math id="M117" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> corresponding to the medium failure state. At a CAV of 40 <inline-formula><mml:math id="M118" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, the displacement range further expands to 0–2.00 <inline-formula><mml:math id="M119" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>, and the slope reliability decreases to 31.7 % at the displacement threshold of 0.50 <inline-formula><mml:math id="M120" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> corresponding to the high failure state.</p>

      <fig id="F8"><label>Figure 8</label><caption><p id="d2e2600">Slope permanent displacement at a CDF of 50 %.</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f08.png"/>

      </fig>

      <p id="d2e2609">Figures 8 and 9 compares the CDF of slope permanent displacement obtained using CAV and PGA. The CAV-based CDF curves show an overall leftward shift relative to the corresponding PGA-based curves, indicating smaller displacement values at the same cumulative probability. At a cumulative probability of 50 %, the slope permanent displacements are approximately 0.07, 0.32, and 0.55 <inline-formula><mml:math id="M121" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> for CAV <inline-formula><mml:math id="M122" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 12, 28, and 40 <inline-formula><mml:math id="M123" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, respectively, compared with approximately 0.20, 0.50, and 0.70 <inline-formula><mml:math id="M124" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula> for PGA <inline-formula><mml:math id="M125" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.4, 0.5, and 0.6 <inline-formula><mml:math id="M126" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi></mml:mrow></mml:math></inline-formula>. The difference becomes more evident at higher cumulative probabilities. The PGA-based CDF exhibit more pronounced large-displacement tails and greater dispersion, whereas the CAV-based CDF show more concentrated displacement distributions. Overall, CAV better captures the cumulative effects of MAS on slope permanent displacement and therefore provides a more comprehensive intensity measure for slope reliability analysis under MAS.</p>

      <fig id="F9"><label>Figure 9</label><caption><p id="d2e2672">Compared with the reliability results of slope displacement response in reference (Wang et al., 2022).</p></caption>
        <graphic xlink:href="https://nhess.copernicus.org/articles/26/4611/2026/nhess-26-4611-2026-f09.png"/>

      </fig>

</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d2e2689">By identifying the intensity measure of MAS and integrating it with the PDEM, this study develops a reliability analysis method for slope permanent displacement under MAS. The main conclusions are as follows: <list list-type="custom"><list-item><label>1.</label>
      <p id="d2e2694">Among the 21 MAS ground-motion parameters considered, CAV showed the strongest correlation with slope permanent displacement (<inline-formula><mml:math id="M127" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M128" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> 0.872) and best represents the cumulative effects of MAS. Therefore, CAV can be used as the intensity measure to assess the response of soil slopes under MAS.</p></list-item><list-item><label>2.</label>
      <p id="d2e2712">By incorporating the dynamic calculation results, the slope permanent displacement gradually increases as CAV increases from 12 to 40 <inline-formula><mml:math id="M129" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">m</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">s</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, while the displacement results still exhibit a degree of scatter. This variability highlights the need for probabilistic analysis when evaluating slope reliability under MAS.</p></list-item><list-item><label>3.</label>
      <p id="d2e2733">By incorporating the characteristics of MAS into the PDEM framework and adopting CAV as the intensity measure, a methodology for evaluating the reliability of slope permanent displacement under MAS is developed. Compared with the conventional PGA-based method, the proposed method effectively reduces the dispersion of slope permanent displacement responses and improves the estimation of slope reliability at different displacement thresholds, demonstrating its theoretical and practical value.</p></list-item></list></p>
      <p id="d2e2736">This study focuses on clayey soil slopes in southwestern China and examines the feasibility of the proposed reliability analysis method for soil slope responses under shallow-crustal MAS. The effects of soil-parameter variability and slope geometric variability are not considered. The principal contribution of this study lies in the proposed methodological framework, which integrates CAV as the intensity measure for MAS with the PDEM for efficient reliability analysis. Further consideration of soil-parameter variability is expected to improve the applicability of the proposed method to practical engineering problems.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability"><title>Code and data availability</title>

      <p id="d2e2744">The MAS ground motions in this study was based on the NGA-West2 strong-motion database from the Pacific Earthquake Engineering Research Center (Chengda Zhang, zcd_geo@163.com).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d2e2751">JZ and CZ designed the research and optimized the overall structure of this paper. TW and CZ completed most of the main work, including the programming, debugging of parameters, and final drafting of the article. SC and ZD contributed some important algorithm ideas and completed the work of the comparison part. JZ and ZD provided the original algorithm ideas and framework for this study and provides valuable suggestions for program optimization and parameter adjustment.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d2e2757">The contact author has declared that none of the authors has any competing interests.</p>
  </notes><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d2e2763">Views and opinions expressed are, however, those of the author(s) only and do not necessarily reflect those of the European Union or REA. Neither the European Union nor the granting authority can be held responsible for them.Publisher's note: Copernicus Publications remains neutral with regard to jurisdictional claims made in the text, published maps, institutional affiliations, or any other geographical representation in this paper. The authors bear the ultimate responsibility for providing appropriate place names. Views expressed in the text are those of the authors and do not necessarily reflect the views of the publisher.</p>
  </notes><ack><title>Acknowledgements</title><p id="d2e2773">The authors gratefully acknowledge the financial support of the National Natural Science Foundation of China.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d2e2779">This work was supported by the financial support from the National Natural Science Foundation of China (grant nos. 51908176, 62273315 and 52192675).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d2e2786">This paper was edited by Seda Yolsal-Çevikbilen and reviewed by Tuncay Taymaz and Ali Fallah Yeznabad.</p>
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