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        <title>SE - recent papers</title>


    <link rel="self" href="https://se.copernicus.org/articles/"/>
    <id>https://se.copernicus.org/articles/</id>
    <updated>2026-06-11T18:16:57+02:00</updated>
    <author>
        <name>Copernicus Publications</name>
    </author>
        <entry>
            <id>https://doi.org/10.5194/se-17-803-2026</id>
            <title type="html">Statistical characteristics of non-volcanic tremor distributions along the Mexican Subduction Zone
            </title>
            <link href="https://doi.org/10.5194/se-17-803-2026"/>
            <summary type="html">
                &lt;b&gt;Statistical characteristics of non-volcanic tremor distributions along the Mexican Subduction Zone&lt;/b&gt;&lt;br&gt;
                Quetzalcoatl Rodríguez-Pérez, Víctor Hugo Márquez-Ramírez, and Francisco Ramón Zúñiga&lt;br&gt;
                    Solid Earth, 17, 803&#8211;824, https://doi.org/10.5194/se-17-803-2026, 2026&lt;br&gt;
                We studied the statistical properties of weak signals known as non-volcanic tremors along the Mexican coast to understand how the earth moves deep underground. By analyzing the timing and size of these faint tremors, we discovered they behave similarly to regular earthquakes but follow complex, persistent patterns. Our findings suggest these movements are influenced by underground fluids and nonlinear forces. This work clarifies how energy builds up, improving our grasp of earthquake risks.
            </summary>
            <content type="html">
                &lt;b&gt;Statistical characteristics of non-volcanic tremor distributions along the Mexican Subduction Zone&lt;/b&gt;&lt;br&gt;
                Quetzalcoatl Rodríguez-Pérez, Víctor Hugo Márquez-Ramírez, and Francisco Ramón Zúñiga&lt;br&gt;
                    Solid Earth, 17, 803&#8211;824, https://doi.org/10.5194/se-17-803-2026, 2026&lt;br&gt;
                <p>We analyze the statistical characteristics of non-volcanic tremor (NVT) sequences in the Mexican subduction zone. To this end, we employ various techniques, including the Gutenberg&amp;#8211;Richter relationship, non-extensive statistics, and multifractal detrended moving-average analysis, to extract information on magnitude and interevent-time distributions. The <span class="inline-formula"><i>b</i></span>-value results reveal that <span class="inline-formula"><i>b</i></span&gt; ranges from 1.25 to 2.42, with the highest values occurring in the down-dip portion of the plate interface. In contrast, the <span class="inline-formula"><i>q</i></span>-value shows an inverse behavior, reaching its highest values in the interplate coupling region. Similar to tectonic earthquakes, NVT sequences exhibit a multifractal structure in both magnitude and interevent-time series. The multifractality analysis suggests that this behavior is associated with long-term correlations, the probability distribution of the data, and nonlinear dynamics. Both apparent and intrinsic multifractality are identified, with the former being dominant. Our estimates of the Hurst exponent (<span class="inline-formula"><i>H</i></span>) range from 0.65 to 1.06; most sequences indicate strong persistence (<span class="inline-formula"><i>H</i>>0.95</span>), while values exceeding unity suggest a transition toward non-stationary behavior. These high temporal correlations may reflect localized fluid-perturbed regions, although this interpretation remains speculative. Regarding the distribution that best describes interevent sequences, we find that most sequences are well described by a Lognormal distribution and, to a lesser extent, by a Gamma distribution. Finally, observations of tectonic tremor duration exhibit substantial scatter, resulting in low coefficients of determination in scaling relationships. The source of this variability may be related to the NVT generation mechanism or to detection and characterization processes.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-05-28T18:16:57+02:00</published>
            <updated>2026-05-28T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-789-2026</id>
            <title type="html">Basic Earth Parameters from VLBI observations using Bayesian inversions in the time domain: updated insights of the Earth's interior
            </title>
            <link href="https://doi.org/10.5194/se-17-789-2026"/>
            <summary type="html">
                &lt;b&gt;Basic Earth Parameters from VLBI observations using Bayesian inversions in the time domain: updated insights of the Earth's interior&lt;/b&gt;&lt;br&gt;
                Yuting Cheng, Véronique Dehant, Attilio Rivoldini, Jérémy Rekier, and Christian Bizouard&lt;br&gt;
                    Solid Earth, 17, 789&#8211;801, https://doi.org/10.5194/se-17-789-2026, 2026&lt;br&gt;
                By analyzing 45 years of Very Long Baseline Interferometry data, we found that the liquid outer core and solid mantle are more strongly coupled than expected, likely due to topography at their boundary. The solid inner core is also less rigidly connected to the outer core. These results challenge current models of Earth's deep interior, core dynamics, and magnetic field generation, with implications for geophysics and space navigation.
            </summary>
            <content type="html">
                &lt;b&gt;Basic Earth Parameters from VLBI observations using Bayesian inversions in the time domain: updated insights of the Earth's interior&lt;/b&gt;&lt;br&gt;
                Yuting Cheng, Véronique Dehant, Attilio Rivoldini, Jérémy Rekier, and Christian Bizouard&lt;br&gt;
                    Solid Earth, 17, 789&#8211;801, https://doi.org/10.5194/se-17-789-2026, 2026&lt;br&gt;
                <p>We present updated estimates of Basic Earth Parameters (BEP) from VLBI Celestial Pole Offset (CPO) time series spanning 1980-2025 using an ensemble Markov Chain Monte Carlo (MCMC) Bayesian inversion. Building upon <span class="cit" id="xref_text.1"><a href="#bib1.bibx19">Koot et&amp;#160;al.</a&gt; (<a href="#bib1.bibx19">2008</a>)</span>, we incorporate recent advances in ocean tidal modeling <span class="cit" id="xref_paren.2">(<a href="#bib1.bibx5">Cheng and Bizouard</a>,&amp;#160;<a href="#bib1.bibx5">2025</a>)</span&gt; and update several aspects of the algorithm. Key improvements include: (1) implementation of a cubic spline representation for Free Core Nutation (FCN) amplitude variations, which significantly reduces multimodality in FCN-related parameter in MCMC sampling compared to a linear representation; (2) integration of updated Ocean Tidal Angular Momentum (OTAM) values from FES2014 ocean tidal atlas <span class="cit" id="xref_paren.3">(<a href="#bib1.bibx22">Lyard et&amp;#160;al.</a>,&amp;#160;<a href="#bib1.bibx22">2021</a>)</span>, without the empirical 0.7 scaling factor previously applied in the construction of the last adopted nutation model MHB2000; and (3) utilization of five diverse CPO series from different analysis centers spanning up to 45&amp;#160;years of observations.</p&gt;        <p>Our estimated mean values of the parameters show good consistency across different CPO series, with values of the Earth's dynamical ellipticity at the edge of the <span class="inline-formula">1<i>&amp;#963;</i></span&gt; range of MHB2000 <span class="cit" id="xref_paren.4">(<a href="#bib1.bibx24">Mathews et&amp;#160;al.</a>,&amp;#160;<a href="#bib1.bibx24">2002</a>; <a href="#bib1.bibx2">Buffett et&amp;#160;al.</a>,&amp;#160;<a href="#bib1.bibx2">2002</a>; <a href="#bib1.bibx16">Herring et&amp;#160;al.</a>,&amp;#160;<a href="#bib1.bibx16">2002</a>)</span>. Notable findings include a larger absolute value for the imaginary part of the core-mantle boundary (CMB) coupling constant (<span class="inline-formula"><i>K</i><sup>CMB</sup></span>), approaching the <span class="inline-formula">2<i>&amp;#963;</i></span&gt; boundary of <span class="cit" id="xref_text.5"><a href="#bib1.bibx24">Mathews et&amp;#160;al.</a&gt; (<a href="#bib1.bibx24">2002</a>)</span>, which may reflect contributions from other coupling mechanisms in addition to electromagnetic coupling, including possible topographic coupling through &amp;#8220;form drag&amp;#8221; effect caused by wave interactions with irregular boundaries <span class="cit" id="xref_paren.6">(<a href="#bib1.bibx31">Rekier et&amp;#160;al.</a>,&amp;#160;<a href="#bib1.bibx31">2025</a>)</span>. The real part of the Inner Core Boundary (ICB) coupling constant (<span class="inline-formula"><i>K</i><sup>ICB</sup></span>) is approximately half the MHB2000 value, potentially indicating the need to revisit hydrostatic assumptions for the inner core given recent seismic evidence of viscous deformation <span class="cit" id="xref_paren.7">(<a href="#bib1.bibx37">Wang et&amp;#160;al.</a>,&amp;#160;<a href="#bib1.bibx37">2024</a>; <a href="#bib1.bibx36">Vidale et&amp;#160;al.</a>,&amp;#160;<a href="#bib1.bibx36">2025</a>)</span>. Compliance estimates suggest that frequency extrapolation methods from seismic to nutation bands may be considered unchanged in the mantle, but should be revised at the ICB.  The enhanced FCN free-mode modeling captures amplitude variations that differ from empirical models, particularly after 2000, although the physical interpretation of these differences requires further investigation.</p&gt;        <p>The systematic discrepancies across multiple parameters suggest that current nutation theory needs substantial updates to incorporate more realistic models of core-mantle coupling and inner-core&amp;#8211;outer-core coupling.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-05-22T18:16:57+02:00</published>
            <updated>2026-05-22T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-763-2026</id>
            <title type="html">Distributed right-lateral strain at the northern boundary of the Quito-Latacunga microblock
            </title>
            <link href="https://doi.org/10.5194/se-17-763-2026"/>
            <summary type="html">
                &lt;b&gt;Distributed right-lateral strain at the northern boundary of the Quito-Latacunga microblock&lt;/b&gt;&lt;br&gt;
                Nicolas Harrichhausen, Léo Marconato, Laurence Audin, Pierre Lacan, Stéphane Baize, Hervé Jomard, Alexandra Alvarado, James Hollingsworth, Pierre-Henri Blard, Patricia Ann Mothes, Frédérique Rolandone, and Iván Dario Ortiz Martin&lt;br&gt;
                    Solid Earth, 17, 763&#8211;787, https://doi.org/10.5194/se-17-763-2026, 2026&lt;br&gt;
                Tectonic plates can be broken into smaller blocks with deformation concentrated at their boundaries. We use remote sensing and field studies to investigate how faulting accommodates deformation at the northern boundary of the Quito-Latacunga microblock (Ecuador & Colombia). We show this boundary is a wide zone characterized by several parallel faults capable of hosting moderate to large (<M7) earthquakes, such as the one in 2022, and which may be influenced by nearby volcanism.
            </summary>
            <content type="html">
                &lt;b&gt;Distributed right-lateral strain at the northern boundary of the Quito-Latacunga microblock&lt;/b&gt;&lt;br&gt;
                Nicolas Harrichhausen, Léo Marconato, Laurence Audin, Pierre Lacan, Stéphane Baize, Hervé Jomard, Alexandra Alvarado, James Hollingsworth, Pierre-Henri Blard, Patricia Ann Mothes, Frédérique Rolandone, and Iván Dario Ortiz Martin&lt;br&gt;
                    Solid Earth, 17, 763&#8211;787, https://doi.org/10.5194/se-17-763-2026, 2026&lt;br&gt;
                <p>Remote sensing and field data suggest distributed right-lateral faulting at the northern edge of the Quito-Latacunga microblock in northern Ecuador and southern Colombia. Off the west coast of Ecuador and Colombia, oblique subduction of the Nazca Plate beneath the South America plate induces NE-motion of the Northern Andean Sliver relative to stable South America. Recent geodetic studies show this sliver comprises several independent microblocks, with strain accommodated at each of their boundaries. The Quito-Latacunga microblock, located in the densely populated Inter-Andean valley, shows approximately 3&amp;#8201;mm&amp;#8201;yr<span class="inline-formula"><sup>&amp;#8722;1</sup></span&gt; of right-lateral strain at its northern boundary. However, which structures accommodate this deformation is unclear. Using available digital terrain models (DTMs), local DTMs derived from Pleiades satellite stereo-imagery, InSAR, Google Earth imagery, and field surveys, we demonstrate deformation at the northern boundary is distributed across several NE-striking right-lateral faults in Ecuador and Colombia. InSAR shows that a recent 2022 <span class="inline-formula"><i>M</i>&amp;#8197;5.6</span&gt; earthquake resulted in line-of-sight displacement of 5 to 13&amp;#8201;cm along one of the ENE-striking, right-lateral faults. Offset sediments and glacial features indicate recent earthquakes on two other faults (the Reservoir and Polylepis faults) north of and subparallel with this rupture. Displaced glacial landforms along the Reservoir fault show slip rates between 0.8 and 6.1&amp;#8201;mm&amp;#8201;yr<span class="inline-formula"><sup>&amp;#8722;1</sup></span>, suggesting geologic slip rates that could be higher than geodetic ones. Exposures of the Reservoir fault also show evidence for at least three surface rupturing earthquakes with magnitudes between <span class="inline-formula"><i>M</i>&amp;#8197;6.3</span&gt; and <span class="inline-formula"><i>M</i>&amp;#8197;7.0</span>. Inflation at the nearby Chile-Cerro Negro volcano may influence earthquakes on these faults, enhancing slip and earthquake rates. The Polylepis, Reservoir, and 25 July earthquake faults all overlap with the proposed area for the 15 August 1868, <span class="inline-formula"><i>M</i>&amp;#8197;6.4</span>&amp;#8211;6.8 El Angel earthquake, indicating they could be associated with this damaging event.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-05-21T18:16:57+02:00</published>
            <updated>2026-05-21T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-747-2026</id>
            <title type="html">Persistent deformation in a post-collisional stable continental region: insights from 20 years of cGPS in Romania
            </title>
            <link href="https://doi.org/10.5194/se-17-747-2026"/>
            <summary type="html">
                &lt;b&gt;Persistent deformation in a post-collisional stable continental region: insights from 20 years of cGPS in Romania&lt;/b&gt;&lt;br&gt;
                Alexandra Muntean, Laura Petrescu, Boudewijn Ambrosius, Felix Borleanu, Eduard Ilie Nastase, and Ioan Munteanu&lt;br&gt;
                    Solid Earth, 17, 747&#8211;762, https://doi.org/10.5194/se-17-747-2026, 2026&lt;br&gt;
                We utilize two decades of continuous GPS data to investigate crustal deformation in Romania, a region that has long been regarded as tectonically stable. Despite the end of major collisions millions of years ago, subcrustal earthquakes and active faults indicate ongoing strain. We estimate horizontal and vertical velocities, strain rates, and dominant deformation styles. Our results reveal localized uplift and extension in the foreland, linked to slab dynamics beneath the southeast Carpathians.
            </summary>
            <content type="html">
                &lt;b&gt;Persistent deformation in a post-collisional stable continental region: insights from 20 years of cGPS in Romania&lt;/b&gt;&lt;br&gt;
                Alexandra Muntean, Laura Petrescu, Boudewijn Ambrosius, Felix Borleanu, Eduard Ilie Nastase, and Ioan Munteanu&lt;br&gt;
                    Solid Earth, 17, 747&#8211;762, https://doi.org/10.5194/se-17-747-2026, 2026&lt;br&gt;
                <p>The Carpathian Region, located at the edge of the East European Platform, presents a unique tectonic setting where major deformation associated with subduction and collision appears to have ceased around 8 million years ago. Yet vertical movements and seismicity continued afterward till the present day, suggesting ongoing crustal deformation and challenging our understanding of intraplate earthquakes and the processes driving these phenomena in an area considered a stable continental interior. In this study, we analyze over two decades of continuous GPS (cGPS) data from 143 permanent stations to estimate both horizontal and vertical crustal motions, constructing the most accurate model of crustal deformation in the region to date. The estimated velocity field indicates a southward drift of the South Carpathians and Moesia relative to Eurasia, with velocities ranging from 0.5 to 2&amp;#8201;mm&amp;#8201;yr<span class="inline-formula"><sup>&amp;#8722;1</sup></span>. We detect a more complex pattern of vertical uplift and subsidence in the foredeep, challenging a previously held view that this region is solely subsiding. This pattern may reflect localized uplift in response to processes such as the Vrancea Slab break-off beneath the South-East Carpathians. Crustal-scale active faults accommodate the observed differential motion, fragmenting the foreland. Furthermore, using a regularized horizontal velocity vector field, we estimate strain rate variations, maximum shear strain, and dilatation patterns across Romania, which align with observed stress regimes and earthquake mechanisms. This agreement validates our results and indicates an influence of surface plate kinematics on the observed seismicity, in addition to the deep Vrancea Slab dynamics. Our findings provide insights into the causes of crustal deformation at the transition between active collision zones and stable continental platforms, enhancing our understanding of intraplate seismicity in regions traditionally considered tectonically stable.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-05-19T18:16:57+02:00</published>
            <updated>2026-05-19T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-711-2026</id>
            <title type="html">Deciphering the crustal structure of the Lerma Valley (NW Argentina): a multi-method seismic investigation
            </title>
            <link href="https://doi.org/10.5194/se-17-711-2026"/>
            <summary type="html">
                &lt;b&gt;Deciphering the crustal structure of the Lerma Valley (NW Argentina): a multi-method seismic investigation&lt;/b&gt;&lt;br&gt;
                Emilio J. M. Criado-Sutti, Andrés Olivar-Castaño, Frank Krüger, Carolina Montero-López, Germán Aranda-Viana, Martin Zeckra, and Sebastian Heimann&lt;br&gt;
                    Solid Earth, 17, 711&#8211;733, https://doi.org/10.5194/se-17-711-2026, 2026&lt;br&gt;
                We studied the deep structure beneath the Lerma Valley in northwestern Argentina to better understand how the Earth's crust behaves in this active but little-studied region of the Andes. Using data from local and teleseismic earthquakes, we mapped layers within the crust and found major contrasts between the northern and southern areas. Our results shed new light on how this region formed and evolved, offering important insights into earthquake risks and mountain-building processes.
            </summary>
            <content type="html">
                &lt;b&gt;Deciphering the crustal structure of the Lerma Valley (NW Argentina): a multi-method seismic investigation&lt;/b&gt;&lt;br&gt;
                Emilio J. M. Criado-Sutti, Andrés Olivar-Castaño, Frank Krüger, Carolina Montero-López, Germán Aranda-Viana, Martin Zeckra, and Sebastian Heimann&lt;br&gt;
                    Solid Earth, 17, 711&#8211;733, https://doi.org/10.5194/se-17-711-2026, 2026&lt;br&gt;
                <p>We investigated the crustal structure beneath the Lerma Valley in northwestern Argentina using data from a local seismic network deployed between 2017 and 2018. This geologically complex transition zone between the Eastern Cordillera and the Santa B&amp;#225;rbara system is characterized by moderate to high seismicity, yet remains largely understudied despite its strategic location within the Andean orogen. Its passive orogenic setting and evidence of inherited structures make it a natural laboratory for exploring intraplate deformation and foreland basin evolution.  We combined local and teleseismic receiver functions with ambient noise tomography (ANT), jointly inverting Rayleigh wave phase velocities to obtain 1D shear-wave velocity profiles. The results reveal a stratified crust with four main discontinuities at <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M1" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>&amp;#8764;</mo><mn mathvariant="normal">53</mn><mo>-</mo><mn mathvariant="normal">43</mn></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="48pt" height="10pt" class="svg-formula" dspmath="mathimg" md5hash="aeb3a2e406490af51efede6e1acf27a7"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="se-17-711-2026-ie00001.svg" width="48pt" height="10pt" src="se-17-711-2026-ie00001.png"/></svg:svg></span></span>, 35&amp;#8211;30, 10&amp;#8211;8, and 1.5&amp;#8211;1.2&amp;#8201;km, corresponding to the Moho, mid- and lower-crustal boundaries, and the sedimentary basin base. A southward-dipping Moho is evident from CCP migration and T-component phase shifts. Velocity profiles also show a north&amp;#8211;south contrast: lower velocities (1&amp;#8211;2.5&amp;#8201;<span class="inline-formula">km&amp;#8201;s<sup>&amp;#8722;1</sup></span>) in the south indicate thicker, less consolidated sediments, while the north exhibits more competent crust (up to 3.5&amp;#8201;<span class="inline-formula">km&amp;#8201;s<sup>&amp;#8722;1</sup></span>). The final model comprises five layers, including three sedimentary and two crystalline crustal units. We also introduced a layer-dependent <span class="inline-formula"><i>&amp;#954;</i></span&gt; correction, revealing a trend from 1.65 at the Moho to 2 in the upper layers. These results provide new geophysical constraints on the crustal architecture and tectonic evolution of this underexplored Andean region.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-05-12T18:16:57+02:00</published>
            <updated>2026-05-12T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-735-2026</id>
            <title type="html">Patterns of contemporary horizontal stress orientation in the Earth's crust derived from the World Stress Map Database 2025
            </title>
            <link href="https://doi.org/10.5194/se-17-735-2026"/>
            <summary type="html">
                &lt;b&gt;Patterns of contemporary horizontal stress orientation in the Earth's crust derived from the World Stress Map Database 2025&lt;/b&gt;&lt;br&gt;
                Oliver Heidbach and Mojtaba Rajabi&lt;br&gt;
                    Solid Earth, 17, 735&#8211;745, https://doi.org/10.5194/se-17-735-2026, 2026&lt;br&gt;
                The World Stress Map project provides the only open-access database of crustal stress information. The new global database has been substantially updated, and now contains more than twice the number of data on the orientation of maximum horizontal stress (S<sub>Hmax</sub>). As data are clustered, we provide mean S<sub>Hmax</sub&gt; orientations on different global grids. The results reveal for intraplate areas that the earlier hypothesis that plate boundary forces control the S<sub>Hmax</sub&gt; orientation needs to be revised.
            </summary>
            <content type="html">
                &lt;b&gt;Patterns of contemporary horizontal stress orientation in the Earth's crust derived from the World Stress Map Database 2025&lt;/b&gt;&lt;br&gt;
                Oliver Heidbach and Mojtaba Rajabi&lt;br&gt;
                    Solid Earth, 17, 735&#8211;745, https://doi.org/10.5194/se-17-735-2026, 2026&lt;br&gt;
                <p>Knowledge of the present-day stress field of the Earth's crust is essential for understanding geodynamic processes, as well as for the exploration and management of geo-reservoirs. The World Stress Map (WSM) project provides the only open-access global database of crustal stress information. To mark the project's 40th anniversary, the WSM database has been substantially updated, and now contains more than twice the number of data records on the orientation of maximum horizontal stress (<span class="inline-formula"><i>S</i><sub>Hmax</sub></span>) in comparison to the previous release in 2016. The new database includes 100&amp;#8201;842 quality-ranked data records documenting the <span class="inline-formula"><i>S</i><sub>Hmax</sub></span&gt; orientation in the Earth's crust. As stress data records are clustered around plate boundaries and in sedimentary basins, we provide mean <span class="inline-formula"><i>S</i><sub>Hmax</sub></span&gt; orientation estimates on regular global grids of 2, 1, 0.5 and 0.2&amp;#176; using search radii between 50   and 500&amp;#8201;km to facilitate the analysis of stress patterns. The results reveal that in intraplate regions, where stress data density has increased significantly, the earlier hypothesis that plate boundary forces and relative plate motion primarily control the <span class="inline-formula"><i>S</i><sub>Hmax</sub></span&gt; orientation needs to be revised. The <span class="inline-formula"><i>S</i><sub>Hmax</sub></span&gt; orientation rotates in some areas by more than 50&amp;#176; over spatial scales of 50&amp;#8211;500&amp;#8201;km. Two notable examples include an <span class="inline-formula">&amp;#8764;</span>&amp;#8201;50&amp;#176; rotation of the <span class="inline-formula"><i>S</i><sub>Hmax</sub></span&gt; orientation in the Alpine foreland, from N&amp;#8211;S in the East to NW&amp;#8211;SE in the West, and <span class="inline-formula"><i>S</i><sub>Hmax</sub></span&gt; orientation rotations&amp;#8201;<span class="inline-formula"><i>></i></span>&amp;#8201;50&amp;#176; over distances of less than&amp;#160;100&amp;#8201;km in eastern Australia.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-05-12T18:16:57+02:00</published>
            <updated>2026-05-12T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-689-2026</id>
            <title type="html">Enhancing 2D deep seismic reflection imaging using shot domain regularization: a case study from the Jiangnan Orogenic Belt, South China
            </title>
            <link href="https://doi.org/10.5194/se-17-689-2026"/>
            <summary type="html">
                &lt;b&gt;Enhancing 2D deep seismic reflection imaging using shot domain regularization: a case study from the Jiangnan Orogenic Belt, South China&lt;/b&gt;&lt;br&gt;
                Hui Zhang, Jiayong Yan, Zhendong Liu, Jianguang Han, Hao Wang, and Jiahao Liu&lt;br&gt;
                    Solid Earth, 17, 689&#8211;709, https://doi.org/10.5194/se-17-689-2026, 2026&lt;br&gt;
                This study compares four regularization methods for deep seismic reflection data from the Jiangnan Orogenic Belt, South China. The optimal method regularizes and interpolates shot gathers at 100-meter intervals, improving&amp;#160;signal-to-noise ratio&amp;#160;and resolution, reducing artifacts, and yielding clearer seismic images. Results show data regularization is critical in deep seismic imaging for reliable geological interpretation and accurate mineral deposit detection.
            </summary>
            <content type="html">
                &lt;b&gt;Enhancing 2D deep seismic reflection imaging using shot domain regularization: a case study from the Jiangnan Orogenic Belt, South China&lt;/b&gt;&lt;br&gt;
                Hui Zhang, Jiayong Yan, Zhendong Liu, Jianguang Han, Hao Wang, and Jiahao Liu&lt;br&gt;
                    Solid Earth, 17, 689&#8211;709, https://doi.org/10.5194/se-17-689-2026, 2026&lt;br&gt;
                <p>Deep seismic reflection is a key method for investigating plate tectonics, as it enables detailed imaging of lithospheric structures &amp;#8211; particularly within the crust and upper mantle. It plays a crucial role in understanding crustal evolution and identifying mineral enrichment zones. However, during data acquisition, deviations from the planned shot and receiver locations often occur due to surface constraints or other logistical challenges. These deviations result in irregular seismic data that can introduce significant migration artifacts during processing, ultimately reducing data quality and hindering the interpretation of deep geological structures. To address this issue, we evaluated four data regularization strategies based on anti-aliasing Matching Pursuit Fourier Interpolation using a 2D deep seismic reflection dataset from the central Jiangnan Orogenic Belt. Among these, the method that involves regularizing and infilling shot gathers at 100&amp;#8201;m intervals produced the most effective results. Compared to legacy contractor-processed data, this method achieved a higher signal-to-noise ratio and improved seismic resolution. The superiority of that method was further confirmed through enhanced imaging in the pre-stack time migration results. These findings highlight the importance of shot domain regularization prior to migration in deep seismic reflection surveys.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-04-23T18:16:57+02:00</published>
            <updated>2026-04-23T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-665-2026</id>
            <title type="html">First tomographic imaging of mid-crustal doubling at the Abruzzi outer thrust front, central-southern Italy
            </title>
            <link href="https://doi.org/10.5194/se-17-665-2026"/>
            <summary type="html">
                &lt;b&gt;First tomographic imaging of mid-crustal doubling at the Abruzzi outer thrust front, central-southern Italy&lt;/b&gt;&lt;br&gt;
                Rita de Nardis, Donato Talone, Luca De Siena, Maria Adelaide Romano, Francesco Brozzetti, and Giusy Lavecchia&lt;br&gt;
                    Solid Earth, 17, 665&#8211;687, https://doi.org/10.5194/se-17-665-2026, 2026&lt;br&gt;
                The Outer Thrust System (OTS) in coastal Abruzzi (Italy) remains debated in terms of its geometry, seismic activity, and deformation style. This study presents a new seismic tomography of the Abruzzi Arc basal thrust, revealing mid-crustal doubling at depths of 14&amp;#8211;24 km. The conceptual 3D model highlights deep compressive tectonics influencing the crustal structure. If the thrust is seismogenic, it could have significant implications for regional geodynamics and seismic hazard assessment.
            </summary>
            <content type="html">
                &lt;b&gt;First tomographic imaging of mid-crustal doubling at the Abruzzi outer thrust front, central-southern Italy&lt;/b&gt;&lt;br&gt;
                Rita de Nardis, Donato Talone, Luca De Siena, Maria Adelaide Romano, Francesco Brozzetti, and Giusy Lavecchia&lt;br&gt;
                    Solid Earth, 17, 665&#8211;687, https://doi.org/10.5194/se-17-665-2026, 2026&lt;br&gt;
                <p>The geometry, deep structural style, and seismotectonic setting of the outer Abruzzi thrust system are less understood than those of other segments of Italy's Late Pliocene&amp;#8211;Quaternary contractional belt. This knowledge gap arises from the region's complex surface geology, low seismicity rates, and the limited resolution of existing geophysical data.</p&gt;        <p>Here, we present a local earthquake tomography of a large and previously unexplored area that encompasses the Abruzzi thrust system and spans from the Apennine extensional province in the west to the foreland strike-slip province in the east. The model is based on the inversion of 42&amp;#8201;176 P-wave and 29&amp;#8201;045 S-wave arrival times from earthquakes with <span class="inline-formula"><i>M</i><sub>L</sub></span&gt; ranging from 0.2 to 5.5.</p&gt;        <p>Our results show low seismic velocities at upper crustal levels in the western sectors, correlating with continental basins of the extensional domain. In contrast, marked <span class="inline-formula"><i>V</i><sub><i>p</i></sub></span&gt; inversions (decrease in velocity with depth) at mid- to lower-crustal depths in the eastern sector delineate a crustal doubling.</p&gt;        <p>We interpret the tomographic results in the context of geological, geophysical, and seismological data to construct a 3D conceptual model of the region. This includes the geometric reconstruction of the Abruzzi Arc basal thrust, an eastward convex arcuate structure extending <span class="inline-formula">&amp;#8764;170</span>&amp;#8201;km and reaching depths of <span class="inline-formula">&amp;#8764;24</span>&amp;#8201;km. The model also incorporates strike-slip faults in the footwall and east-dipping normal faults to the west.</p&gt;        <p>The structural affinity between the Abruzzi Arc basal thrust and other seismogenic structures of the Padan&amp;#8211;Adriatic belt, located in the same structural position, suggests potential seismogenic behavior, although slow deformation rates and long recurrence intervals obscure its seismic expression. This conceptual model provides new insights into regional geodynamics and has significant implications for seismic hazard assessment in the central&amp;#8211;southern Apennine transition zone.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-04-20T18:16:57+02:00</published>
            <updated>2026-04-20T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-643-2026</id>
            <title type="html">Geological factors and fracture distribution in deep and ultra-deep sandstones in Kuqa Depression, Tarim Basin, China
            </title>
            <link href="https://doi.org/10.5194/se-17-643-2026"/>
            <summary type="html">
                &lt;b&gt;Geological factors and fracture distribution in deep and ultra-deep sandstones in Kuqa Depression, Tarim Basin, China&lt;/b&gt;&lt;br&gt;
                Yang Su, Jin Lai, Wenle Dang, Xinjian Zhao, Chuang Han, Yongjia Zhang, Zhongrui Wang, Lei Wang, and Guiwen Wang&lt;br&gt;
                    Solid Earth, 17, 643&#8211;664, https://doi.org/10.5194/se-17-643-2026, 2026&lt;br&gt;
                This study integrates geological and geophysical data to examine controls of sedimentary factors, earth stress, and tectonic structure on fracture distribution in deep and ultra-deep sandstones in Kuqa Depression. Key findings show fracture density increases with sandbody thickness and paleostress magnitude, is higher near faults and fold hinges, and is favored by thinner sand-mud interbeds. Increased horizontal stress differences contributes to reduced fracture apertures.
            </summary>
            <content type="html">
                &lt;b&gt;Geological factors and fracture distribution in deep and ultra-deep sandstones in Kuqa Depression, Tarim Basin, China&lt;/b&gt;&lt;br&gt;
                Yang Su, Jin Lai, Wenle Dang, Xinjian Zhao, Chuang Han, Yongjia Zhang, Zhongrui Wang, Lei Wang, and Guiwen Wang&lt;br&gt;
                    Solid Earth, 17, 643&#8211;664, https://doi.org/10.5194/se-17-643-2026, 2026&lt;br&gt;
                <p>Deep (<span class="inline-formula"><i>></i></span>&amp;#8201;4500&amp;#8201;m) and ultra-deep (<span class="inline-formula"><i>></i></span>&amp;#8201;6000&amp;#8201;m) sandstone reservoirs hold great potential for hydrocarbon resources, yet complex geological challenges hinder the successful exploitation of oil and gas. Fractures in deep and ultra-deep sandstones are prevalent and significantly enhance rock permeability, and critically impact fluid flow and hydrocarbon productivity. Relationships between geological factors and fracture distribution in deep sandstone reservoirs, despite its significance, have remained poorly understood. This study utilizes core, thin section, acoustic emission tests and geophysical well logs to elucidate the interplay between geological elements and fracture occurrences in tight sandstones of the Kuqa Depression, which is a tectonically active foreland basin. The controls of sedimentation, sandbody distribution and earth stress on fracture distribution are analyzed. The research then unravels the effects of lithology units, earth stress fields, and broader tectonic context on fracture distribution patterns. Geological factors, including sedimentary factors (lithology, sandbody thickness and sandbody distribution), earth stress, and tectonic structure are integrated to comprehensively evaluate the fracture distributions in Kuqa Depression. The different lithologies are identified, and fractures in different lithologies are characterized. High-angle fractures and vertical fractures are the main fracture types in Bozi-Dabei area. Fracture density exhibits an inverse relationship with sandbody thickness. The presence of thinner sandstones in conjunction with thin mud layers facilitates the formation of fractures. Paleostress affects the generation of natural fractures, and high fracture density is associated with high paleostress magnitudes. In situ stress affects the subsequent modification of natural fractures. However, some filled fractures with wider aperture oriented at high angles to <span class="inline-formula"><i>S</i><sub>Hmax</sub></span&gt; reveal cement-stress interactions jointly controlling apertures, not stress dominance.</p&gt;        <p>Structure factors including the position at folds and the proximity to faults are crucial for the fracture distribution. Fractures are more abundant in the hinge areas of anticlines compared to the limb areas, and fracture density above the neutral planes is notably higher. In addition, fracture density is higher in the formation adjacent to the fault due to the effect of the regional stress field. This study helps unravel the geological controlling factors and distribution of fractures by integrating geological and geophysical data, and has implications for hydrocarbon resource exploration in deep and ultra-deep sandstones.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-04-15T18:16:57+02:00</published>
            <updated>2026-04-15T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-617-2026</id>
            <title type="html">Interpreting the cause of bound earthquakes at underground injection experiments
            </title>
            <link href="https://doi.org/10.5194/se-17-617-2026"/>
            <summary type="html">
                &lt;b&gt;Interpreting the cause of bound earthquakes at underground injection experiments&lt;/b&gt;&lt;br&gt;
                Ryan Schultz, Linus Villiger, Valentin Gischig, and Stefan Wiemer&lt;br&gt;
                    Solid Earth, 17, 617&#8211;642, https://doi.org/10.5194/se-17-617-2026, 2026&lt;br&gt;
                We use statistical tests to infer M<sub>MAX</sub&gt; (maximum possible magnitude) from an earthquake catalogue and focus on data from three underground laboratories with controlled injection experiments. There, we find clear evidence for M<sub>MAX</sub&gt; bounds and corroborate interpretations of fracture growth against other geophysical studies. Unbound sequences occur when stimulation is directed towards pre-existing faults. The validation of our methods against well-studied cases is encouraging and will help validate future interpretations.
            </summary>
            <content type="html">
                &lt;b&gt;Interpreting the cause of bound earthquakes at underground injection experiments&lt;/b&gt;&lt;br&gt;
                Ryan Schultz, Linus Villiger, Valentin Gischig, and Stefan Wiemer&lt;br&gt;
                    Solid Earth, 17, 617&#8211;642, https://doi.org/10.5194/se-17-617-2026, 2026&lt;br&gt;
                <p>Constraining the maximum possible magnitude (<span class="inline-formula"><i>M</i><sub>MAX</sub></span>) of an induced earthquake sequence is a challenging process with important implications for managing risks. CAP-tests are a suite of statistical tests that can infer, quantify, and select best-fitting <span class="inline-formula"><i>M</i><sub>MAX</sub></span&gt; models via an earthquake catalogue's magnitudes. We use CAP-tests to discern between bound/unbound earthquake sequences at underground laboratories, where high-resolution and near-field geophysical observations are abundant. There, we find clear evidence for bound sequences, where magnitude growth was restricted during stimulation. Furthermore, bound sequences tend to be associated with stimulations that occurred within intact rock. On the other hand, unbound sequences tended to be associated with stimulations where hydraulic fractures interacted with relatively large pre-existing faults/fractures. We further examine bound sequences by fitting magnitude growth to a generalized family of <span class="inline-formula"><i>M</i><sub>MAX</sub></span&gt; functions. This process appears to be able to aggregate bound sequences into categories consistent with theoretical considerations (e.g., tectonic, tensile-crack, or shear-crack). These results provide a basis for validating and interpreting bound sequences in controlled experiments, which is important for extrapolating to larger-scale observations. Overall, CAP-tests appear to be a promising avenue for constraining <span class="inline-formula"><i>M</i><sub>MAX</sub></span&gt; from earthquake catalogue data.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-04-10T18:16:57+02:00</published>
            <updated>2026-04-10T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-601-2026</id>
            <title type="html">High-pressure behaviour and elastic constants of 1<i>M</i> and 2<i>M</i><sub>1</sub> polytypes of phlogopite KMg<sub>3</sub>Si<sub>3</sub>AlO<sub>10</sub>(OH)<sub>2</sub>
            </title>
            <link href="https://doi.org/10.5194/se-17-601-2026"/>
            <summary type="html">
                &lt;b&gt;High-pressure behaviour and elastic constants of 1M and 2M1 polytypes of phlogopite KMg3Si3AlO10(OH)2&lt;/b&gt;&lt;br&gt;
                Gianfranco Ulian, Francesca Ranellucci, and Giovanni Valdrè&lt;br&gt;
                    Solid Earth, 17, 601&#8211;616, https://doi.org/10.5194/se-17-601-2026, 2026&lt;br&gt;
                Layer silicates (phyllosilicates) are important minerals because of their ubiquity on the Earth&amp;#8217;s crust and due to their ability to release water in the mantle. The present study focuses on the elastic properties of a specific phyllosilicate known as phlogopite [KMg<sub>3</sub>Si<sub>3</sub>AlO<sub>10</sub>(OH)<sub>2</sub>], which were characterised using first-principles methods. The results show the mineral's anisotropic mechanical behaviour, which also depends on how the mineral layers are stacked in the crystal structure.
            </summary>
            <content type="html">
                &lt;b&gt;High-pressure behaviour and elastic constants of 1M and 2M1 polytypes of phlogopite KMg3Si3AlO10(OH)2&lt;/b&gt;&lt;br&gt;
                Gianfranco Ulian, Francesca Ranellucci, and Giovanni Valdrè&lt;br&gt;
                    Solid Earth, 17, 601&#8211;616, https://doi.org/10.5194/se-17-601-2026, 2026&lt;br&gt;
                <p>In the present work, the elastic properties of both <span class="inline-formula">1<i>M</i></span&gt; and <span class="inline-formula">2<i>M</i><sub>1</sub></span&gt; phlogopite polytypes, KMg<span class="inline-formula"><sub>3</sub></span>Si<span class="inline-formula"><sub>3</sub></span>AlO<span class="inline-formula"><sub>10</sub></span>(OH)<span class="inline-formula"><sub>2</sub></span&gt; (monoclinic crystal system) were investigated from PV equation of state fitting and by analysis of the fourth-rank elastic tensor. The analysis was performed within the Density Functional Theory framework, using all-electron Gaussian-type orbitals basis sets and the B3LYP functional corrected a posteriori to include long-range interactions (B3LYP-D*). In general, the elastic properties of the two polytypes were strongly anisotropic, with the axial moduli ratio <span class="inline-formula"><i>M</i>(<i>a</i>)</span>&amp;#8201;:&amp;#8201;<span class="inline-formula"><i>M</i>(<i>b</i>)</span>&amp;#8201;:&amp;#8201;<span class="inline-formula"><i>M</i>(<i>c</i>)</span&gt; being close to <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M18" display="inline" overflow="scroll" dspmath="mathml"><mrow><mn mathvariant="normal">4</mn><mo>:</mo><mn mathvariant="normal">4</mn><mo>:</mo><mn mathvariant="normal">1</mn></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="36pt" height="10pt" class="svg-formula" dspmath="mathimg" md5hash="45e4d051053debce880c8869e43cb13e"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="se-17-601-2026-ie00001.svg" width="36pt" height="10pt" src="se-17-601-2026-ie00001.png"/></svg:svg></span></span>. The volume-integrated third-order Birch-Murnaghan equation of state fitting parameters at 0&amp;#8201;K were <span class="inline-formula"><i>K</i><sub>0</sub>=57.9(2)</span>&amp;#8201;GPa, <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M20" display="inline" overflow="scroll" dspmath="mathml"><mrow><msup><mi>K</mi><mo>&amp;#8242;</mo></msup><mo>=</mo><mn mathvariant="normal">8.29</mn><mo>(</mo><mn mathvariant="normal">7</mn><mo>)</mo></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="61pt" height="13pt" class="svg-formula" dspmath="mathimg" md5hash="2cf397aca0163ae1ead9a4e618b6d40b"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="se-17-601-2026-ie00002.svg" width="61pt" height="13pt" src="se-17-601-2026-ie00002.png"/></svg:svg></span></span&gt; and <span class="inline-formula"><i>V</i><sub>0</sub>=489.82(3)</span>&amp;#8201;&amp;#197;<span class="inline-formula"><sup>3</sup></span&gt; for phlogopite-<span class="inline-formula">1<i>M</i></span>, which were very close to those of the <span class="inline-formula">2<i>M</i><sub>1</sub></span&gt; polytype, i.e., <span class="inline-formula"><i>K</i><sub>0</sub>=58.3(1)</span>&amp;#8201;GPa, <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M26" display="inline" overflow="scroll" dspmath="mathml"><mrow><msup><mi>K</mi><mo>&amp;#8242;</mo></msup><mo>=</mo><mn mathvariant="normal">8.71</mn><mo>(</mo><mn mathvariant="normal">8</mn></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="58pt" height="13pt" class="svg-formula" dspmath="mathimg" md5hash="8c1ed069226e24d4e5df3977cafcaf07"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="se-17-601-2026-ie00003.svg" width="58pt" height="13pt" src="se-17-601-2026-ie00003.png"/></svg:svg></span></span>) and <span class="inline-formula"><i>V</i><sub>0</sub>=978.96(9)</span>&amp;#8201;&amp;#197;<span class="inline-formula"><sup>3</sup></span>. The monoclinic elastic tensors obtained for the two polytypes of phlogopite, which have never been experimentally reported for both minerals so far, were in line with the PV behaviour of the mineral, providing further data related to the directional dependence of the elastic properties and seismic wave propagation. The elastic properties from both PV hydrostatic compression and from the elastic moduli tensor were discussed against the available experimental and theoretical data in the scientific literature, extending the knowledge on this important trioctahedral phyllosilicate.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-04-02T18:16:57+02:00</published>
            <updated>2026-04-02T18:16:57+02:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-573-2026</id>
            <title type="html">On the criticality of return flows in viscous accretionary wedges and its implications for deep-crustal exhumation in subduction zones
            </title>
            <link href="https://doi.org/10.5194/se-17-573-2026"/>
            <summary type="html">
                &lt;b&gt;On the criticality of return flows in viscous accretionary wedges and its implications for deep-crustal exhumation in subduction zones&lt;/b&gt;&lt;br&gt;
                Ayan Patsa and Nibir Mandal&lt;br&gt;
                    Solid Earth, 17, 573&#8211;600, https://doi.org/10.5194/se-17-573-2026, 2026&lt;br&gt;
                Accretionary wedges are the prime locations of exhumed high-pressure (HP) and low-temperature (LT) metamorphic rocks. Previous tectonic models invoked the corner flow theory with a premise of slab-parallel motion to explain the upward return flow of buried metasediments. In this study, we develop a generalized corner flow model with additional kinematic and rheological factors and evaluate the limiting conditions in which a wedge can set in significant return flows.
            </summary>
            <content type="html">
                &lt;b&gt;On the criticality of return flows in viscous accretionary wedges and its implications for deep-crustal exhumation in subduction zones&lt;/b&gt;&lt;br&gt;
                Ayan Patsa and Nibir Mandal&lt;br&gt;
                    Solid Earth, 17, 573&#8211;600, https://doi.org/10.5194/se-17-573-2026, 2026&lt;br&gt;
                <p>In subduction zones, the accretionary wedges play a vital role in mediating the burial processes of incoming oceanic sediments and eventually their return pathways to the surface. A direction of the previous tectonic models invoked the standard corner flow theory, assuming a slab-parallel shear and a rigid, fixed overriding plate, to elucidate the crustal recycling processes in tectonic wedges. To deal with more complex subduction-collisional settings, where they have deformable overriding plates, and associate a horizontal slab migration (advance or rollback) component during subduction, we develop a generalized corner flow model to revisit the problem of return flow mechanics, providing a criticality analysis of the return flows as a function of the geometric, kinematic, and rheological conditions in accretionary wedges. A new set of analytical solutions is presented to evaluate the limiting conditions in which a wedge can set in significant return flows, leading to focused exhumation of the deep-crustal materials. The theoretical results suggest that, for moderate wedge-taper angles (<span class="inline-formula">&amp;#8764;30</span>&amp;#176;), the viscosity ratios (<span class="inline-formula"><i>&amp;#956;</i><sub>r</sub></span>) between the overriding plate and the wedge <span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M3" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>&amp;#8805;</mo><mo>&amp;#8764;</mo><msup><mn mathvariant="normal">10</mn><mn mathvariant="normal">3</mn></msup></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="37pt" height="14pt" class="svg-formula" dspmath="mathimg" md5hash="a56e87bfc11b706d2a8d6ced5b59cfa9"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="se-17-573-2026-ie00001.svg" width="37pt" height="14pt" src="se-17-573-2026-ie00001.png"/></svg:svg></span></span&gt; provide favourable tectonic settings for the return flow kinematics in accretionary wedges. Decrease in <span class="inline-formula"><i>&amp;#956;</i><sub>r</sub></span>, or addition of slab roll back weakens the return flows, whereas slab advance greatly strengthens the return flows. The analytical solutions are also utilized to demonstrate reversals in the shear-sense patterns across the wedge. We expand this study by incorporating results from scaled laboratory experiments to evaluate applicability of the generalized theoretical model. It is shown from the theoretical model that the total pressure in the accretionary wedge dynamics becomes close to the lithostatic value when the rheological setting has low-viscosity (10<span class="inline-formula"><sup>19</sup></span>&amp;#8201;Pa&amp;#8201;s) wedge materials.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-25T18:16:57+01:00</published>
            <updated>2026-03-25T18:16:57+01:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-555-2026</id>
            <title type="html">Fatbox: the Fault Analysis Toolbox
            </title>
            <link href="https://doi.org/10.5194/se-17-555-2026"/>
            <summary type="html">
                &lt;b&gt;Fatbox: the Fault Analysis Toolbox&lt;/b&gt;&lt;br&gt;
                Pauline Gayrin, Thilo Wrona, Sascha Brune, Derek Neuharth, Nicolas Molnar, Alessandro La Rosa, and John Naliboff&lt;br&gt;
                    Solid Earth, 17, 555&#8211;572, https://doi.org/10.5194/se-17-555-2026, 2026&lt;br&gt;
                When in extension, the Earth's crust accommodates deformation by breaking. Through time, faults grow into an intricate network that can be detected by changes in topography, or through modelling (numerical or analogue). This study demonstrates how the Python library Fatbox, the Fault Analysis Toolbox, can extract the network pattern automatically from said datasets and measure the geometry and kinematics of the fault network.
            </summary>
            <content type="html">
                &lt;b&gt;Fatbox: the Fault Analysis Toolbox&lt;/b&gt;&lt;br&gt;
                Pauline Gayrin, Thilo Wrona, Sascha Brune, Derek Neuharth, Nicolas Molnar, Alessandro La Rosa, and John Naliboff&lt;br&gt;
                    Solid Earth, 17, 555&#8211;572, https://doi.org/10.5194/se-17-555-2026, 2026&lt;br&gt;
                <p>Analysing the spatial arrangement, connectivity, and evolutionary history of complex fault networks is essential for quantifying strain distribution in active deformational zones, and evaluating associated geohazard and resource potentials. The structure and evolution of fault networks are commonly investigated using a range of methods, including the analysis of topographic data derived from satellite imagery, numerical modelling, as well as physical experiments. The high density and intrinsic complexity of fault systems in many study areas or models pose significant challenges for automated analysis, often necessitating time-intensive manual interpretation. Here, we present Fatbox, the Fault Analysis Toolbox, an open-source Python library that integrates semi-automated fault extraction with automated geometric and kinematic analysis of fault networks. The toolbox capabilities are demonstrated through three case studies on normal fault systems, each drawing on a different data type: (1)&amp;#160;fault extraction and geometric characterization using GLO-30 topographic data in the Magadi-Natron basin in East Africa; (2)&amp;#160;spatio-temporal tracking of fault development in vertical cross-sections of a forward numerical rift model; and (3)&amp;#160;surface fault mapping and geometric evolution of a physical rifting experiment. Fatbox represents fault networks as topological graphs, comprising nodes (i.e., points) and edges (i.e., lines) connecting the nodes. In time-dependent models, the toolbox enables temporal tracking of faults, providing detailed insights into their geometric evolution and facilitating high-resolution measurements of fault kinematics. Fatbox offers a versatile and scalable framework that enhances the efficiency, reproducibility, and precision of fault system analysis &amp;#8211; opening new avenues for tectonic research.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-24T18:16:57+01:00</published>
            <updated>2026-03-24T18:16:57+01:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-537-2026</id>
            <title type="html">Impact of differential stress on fracture due to volume increasing hydration
            </title>
            <link href="https://doi.org/10.5194/se-17-537-2026"/>
            <summary type="html">
                &lt;b&gt;Impact of differential stress on fracture due to volume increasing hydration&lt;/b&gt;&lt;br&gt;
                Jeremiah J. McElwee, Ikuko Wada, Kazuki Yoshida, Hiroyuki Shimizu, and Atsushi Okamoto&lt;br&gt;
                    Solid Earth, 17, 537&#8211;554, https://doi.org/10.5194/se-17-537-2026, 2026&lt;br&gt;
                The volume increase associated with many hydration reactions can fracture the surrounding rock, creating new fluid pathways that impact the distribution of fluids and hydration. However, it is unclear how this process is impacted by the background stress state, which varies across tectonic settings. We ran simulations that indicate the fracture pattern is sensitive to the background stress state, suggesting that it may be a key factor guiding hydration in the lithosphere.
            </summary>
            <content type="html">
                &lt;b&gt;Impact of differential stress on fracture due to volume increasing hydration&lt;/b&gt;&lt;br&gt;
                Jeremiah J. McElwee, Ikuko Wada, Kazuki Yoshida, Hiroyuki Shimizu, and Atsushi Okamoto&lt;br&gt;
                    Solid Earth, 17, 537&#8211;554, https://doi.org/10.5194/se-17-537-2026, 2026&lt;br&gt;
                <p>The volume increase that accompanies many hydration reactions can stress and fracture the surrounding rock, a process commonly called reaction-induced fracturing. Reaction-induced fracturing accelerates the rate of hydration by creating new pathways for fluids to migrate into reactive rock and by generating new reactive surface areas. The evolution of reaction-induced fractures also depends on the background stress state, which varies among different tectonic environments. We investigate the impact of tectonic stresses on reaction-induced fracturing using 2-D hydraulic-chemical-mechanical distinct element models. The results indicate that the general pattern of reaction-induced fractures depends on the orientation of background tectonic stresses relative to fluid-supplying channels. A spalling fracture pattern characterized by short cracks parallel to and along fluid-supplying channels occurs when the maximum principal tectonic stress is parallel to the channels whereas a branching fracture pattern characterized by long tensile cracks that propagate in a hierarchical manner into unreacted parts of the rock is expected when the tectonic stress is hydrostatic or when the maximum principal tectonic stress is normal to fluid-supplying channels. Spalling localizes hydration and fluid flow along the channels whereas branching promotes spatially extensive hydration and fluid flow away from the fluid supply. The results indicate tectonic stresses may guide the hydration distribution in the oceanic lithosphere at mid-ocean ridges and outer rises and in the cold mantle wedge corner in subduction zones.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-23T18:16:57+01:00</published>
            <updated>2026-03-23T18:16:57+01:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-513-2026</id>
            <title type="html">TCSEIS-1D: An Interactive 1D Code for temperature and composition modelling of the crust and mantle from seismological data
            </title>
            <link href="https://doi.org/10.5194/se-17-513-2026"/>
            <summary type="html">
                &lt;b&gt;TCSEIS-1D: An Interactive 1D Code for temperature and composition modelling of the crust and mantle from seismological data&lt;/b&gt;&lt;br&gt;
                Mariano S. Arnaiz-Rodríguez and Javier Fullea&lt;br&gt;
                    Solid Earth, 17, 513&#8211;535, https://doi.org/10.5194/se-17-513-2026, 2026&lt;br&gt;
                <span data-olk-copy-source="MessageBody">We introduce TCSEIS-1D, a new open-source software that connects the physical and chemical structure of the Earth&amp;#8217;s crust and mantle with seismic observations. This relationship is often difficult to model, but TCSEIS-1D simplifies the process using geophysical and thermodynamic principles. It allows scientists to explore how variations in temperature and composition influence surface wave dispersion and receiver functions, helping to interpret what seismic data reveals about Earth's interior.</span>
            </summary>
            <content type="html">
                &lt;b&gt;TCSEIS-1D: An Interactive 1D Code for temperature and composition modelling of the crust and mantle from seismological data&lt;/b&gt;&lt;br&gt;
                Mariano S. Arnaiz-Rodríguez and Javier Fullea&lt;br&gt;
                    Solid Earth, 17, 513&#8211;535, https://doi.org/10.5194/se-17-513-2026, 2026&lt;br&gt;
                <p>We present TCSEIS-1D, a software to model the Earth's thermochemical and geophysical structure from the surface down to the core-mantle boundary (CMB). The code is designed to estimate geophysical parameters of the Earth's crust and mantle from petrological and thermal information within a thermodynamically consistent framework and to perform forward 1D coupled geophysical-petrological modelling of the structure of the Earth. Developed in Julia Language, the open-source code is intended to be an easy-to-use, flexible, and fast. TCSEIS-1D includes tools to exploit the large repertoire of 1D seismological data available, namely: surface wave dispersion curves (of fundamental and higher modes of Rayleigh and Love waves) and receiver functions (of P, S, and SKS waves). Surface heat flow and isostatic topography can also be modelled. Four simple examples that illustrate the capabilities of the code are presented to show the sensitivity of Rayleigh wave phase velocity curves and P-to-S receiver functions to compositional and temperature variations.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-19T18:16:57+01:00</published>
            <updated>2026-03-19T18:16:57+01:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-485-2026</id>
            <title type="html">The influence of burial history on physical rock properties: a case study of Lower Jurassic claystones from the Hils and Sack Synclines (Germany)
            </title>
            <link href="https://doi.org/10.5194/se-17-485-2026"/>
            <summary type="html">
                &lt;b&gt;The influence of burial history on physical rock properties: a case study of Lower Jurassic claystones from the Hils and Sack Synclines (Germany)&lt;/b&gt;&lt;br&gt;
                Raphael Burchartz, Timo Seemann, Garri Gaus, Lisa Winhausen, Mohammadreza Jalali, Brian Mutuma Mbui, Sebastian Grohmann, Linda Burnaz, Marlise Colling Cassel, Jochen Erbacher, Ralf Littke, and Florian Amann&lt;br&gt;
                    Solid Earth, 17, 485&#8211;512, https://doi.org/10.5194/se-17-485-2026, 2026&lt;br&gt;
                In Germany, claystones are studied for their suitability as host-rocks for the disposal of high-level radioactive waste. The MATURITY project systematically investigates how gradual burial affects physical properties in the Lower Jurassic Amaltheenton Formation of the Lower Saxony Basin (Germany). Understanding these changes helps assess claystone suitability for long-term waste isolation, improving site selection for deep geological repositories.
            </summary>
            <content type="html">
                &lt;b&gt;The influence of burial history on physical rock properties: a case study of Lower Jurassic claystones from the Hils and Sack Synclines (Germany)&lt;/b&gt;&lt;br&gt;
                Raphael Burchartz, Timo Seemann, Garri Gaus, Lisa Winhausen, Mohammadreza Jalali, Brian Mutuma Mbui, Sebastian Grohmann, Linda Burnaz, Marlise Colling Cassel, Jochen Erbacher, Ralf Littke, and Florian Amann&lt;br&gt;
                    Solid Earth, 17, 485&#8211;512, https://doi.org/10.5194/se-17-485-2026, 2026&lt;br&gt;
                <p>The search for a suitable host rock for the deep geological disposal of high-level radioactive waste is a major societal challenge of our time. In Germany, clay-bearing formations are under investigation to potentially host a repository for high-level radioactive waste (alongside rock salt and crystalline rock). Their intrinsic properties such as low permeability, self-sealing efficiency with respect to fractures, and sorption capacity provide promising conditions for long-term waste containment. However, these properties are dependent on numerous factors such as mineralogical composition, temperature and stress conditions, and water content. Among these factors, the burial history and thus compaction affect mineralogy, porosity, permeability, and mechanical properties. Within the framework of the MATURITY project, the impact of the burial history on these properties is investigated based on a combination of different laboratory and field methods. For this purpose, a Lower Jurassic claystone formation (the Amaltheenton-Formation, Fm) which was subjected to variable maximum depth and subsequent uplift during its burial history was chosen as target formation. At five locations, in the margin area of the Lower Saxony Basin (Germany) shallow boreholes were drilled through the formation where varying degrees of maturation indicate substantial differences in maximum burial depth.</p&gt;        <p>In this contribution, we present the first results of initial project steps that show (a)&amp;#160;a similar clay-dominated mineralogical composition of the Amaltheenton-Fm across the borehole locations, (b)&amp;#160;an increase of max. burial temperatures (83&amp;#8211;169&amp;#8201;<span class="inline-formula">&amp;#176;C</span>) over a lateral distance of <span class="inline-formula">&amp;#8764;</span>&amp;#8201;50&amp;#8201;<span class="inline-formula">km</span&gt; within the investigation area, (c)&amp;#160;a gradual increase in bulk density accompanied by a reduction in porosity and permeability for normally-compacted Amaltheenton-Fm sequences along increasing max. burial temperatures, (d)&amp;#160;a reverse trend of those parameters for a potentially undercompacted Amaltheenton-Fm sequence, and (e)&amp;#160;hydraulic conductivity determined from in-situ hydraulic tests that significantly differs from laboratory derived equivalents and span two orders of magnitude (10<span class="inline-formula"><sup>&amp;#8722;5</sup></span&gt; to 10<span class="inline-formula"><sup>&amp;#8722;7</sup></span>&amp;#8201;<span class="inline-formula">m&amp;#8201;s<sup>&amp;#8722;1</sup></span>).</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-18T18:16:57+01:00</published>
            <updated>2026-03-18T18:16:57+01:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-465-2026</id>
            <title type="html">Constraining the wavefield of volcano-seismic events on Mt. Etna, Italy through a rotational sensor and seismic array observations
            </title>
            <link href="https://doi.org/10.5194/se-17-465-2026"/>
            <summary type="html">
                &lt;b&gt;Constraining the wavefield of volcano-seismic events on Mt. Etna, Italy through a rotational sensor and seismic array observations&lt;/b&gt;&lt;br&gt;
                Nele Inken Käte Vesely, Eva Patricia Silke Eibl, Gilda Currenti, Mariangela Sciotto, Giuseppe Di Grazia, Matthias Ohrnberger, and Philippe Jousset&lt;br&gt;
                    Solid Earth, 17, 465&#8211;484, https://doi.org/10.5194/se-17-465-2026, 2026&lt;br&gt;
                We compare seismometers with the 6C method, which combines rotational and seismometer data, determining signal directions and wave velocities for short and continuous low-frequency volcanic signals at Mt. Etna. Either the cluster or the rotational sensor reliably detect continuous signal directions, aligning with the observatory data. For short signals, 6C directions deviate more, likely due to a complex underground. Combining both methods' velocity results improves understanding volcanic waves.
            </summary>
            <content type="html">
                &lt;b&gt;Constraining the wavefield of volcano-seismic events on Mt. Etna, Italy through a rotational sensor and seismic array observations&lt;/b&gt;&lt;br&gt;
                Nele Inken Käte Vesely, Eva Patricia Silke Eibl, Gilda Currenti, Mariangela Sciotto, Giuseppe Di Grazia, Matthias Ohrnberger, and Philippe Jousset&lt;br&gt;
                    Solid Earth, 17, 465&#8211;484, https://doi.org/10.5194/se-17-465-2026, 2026&lt;br&gt;
                <p>Long-period (LP) events and tremor are characteristic seismic signals of active volcanoes, offering insight into underlying fluid-driven processes. However, their emergent wavefield is complex and challenging to characterise. Here we decipher the LP event and tremor wavefield composition using a seismic array combined with a rotational sensor co-located with a seismometer (6C station). This study analyses and compares directional and phase velocity estimates by processing a 25&amp;#8201;d long dataset from a rotational sensor and an array of seven broadband stations deployed at Mt. Etna, Italy, in August&amp;#8211;September 2019. We derive the back azimuths (BAz) of LP events and tremor from both the seismometer array and the 6C station, and we compare these estimates with a reference BAz obtained from the network locations from the Istituto Nazionale di Geofisica e Vulcanologia-Osservatorio Etneo (INGV-OE) on Mt. Etna.</p&gt;        <p>Volcanic tremor occurs in distinct phases with varying seismic and surface activity. Depending on the phase, either the array or the 6C method provides reliable tremor BAz estimates, agreeing well with the INGV-OE reference. We find that BAz estimates of both methods are shifted southward relative to the reference location for the LP events. We attribute the larger southward deviation observed in the 6C results to local heterogeneities which exert a stronger influence on the 6C station than on the array.</p&gt;        <p>Based on the array derived slownesses we infer that the tremor and LP events mainly consist of surface waves. Further, the rotational sensor recordings suggest a wavefield dominated by SH-type waves. In combination with the observed temporal evolution of the 6C phase velocity in narrow frequency bands, we infer Love-wave dominance. This study highlights the value of a rotational sensor to constrain the wavefield in a deterministic way in a complex volcanic environment.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-16T18:16:57+01:00</published>
            <updated>2026-03-16T18:16:57+01:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-453-2026</id>
            <title type="html">Offshore crustal thickness variation along the Palu&#8211;Koro strike&#8211;slip fault in the Sulawesi region from OBS receiver function analysis
            </title>
            <link href="https://doi.org/10.5194/se-17-453-2026"/>
            <summary type="html">
                &lt;b&gt;Offshore crustal thickness variation along the Palu–Koro strike–slip fault in the Sulawesi region from OBS receiver function analysis&lt;/b&gt;&lt;br&gt;
                Tingwei Yang, ChuanChuan Lü, Tianyao Hao, Nicholas Rawlinson, Tao Xu, Pepen Supendi, Sri Widiyantoro, Muhammad Taufiq Rafie, Alfian Alfian, and David Prambudi Sahara&lt;br&gt;
                    Solid Earth, 17, 453&#8211;464, https://doi.org/10.5194/se-17-453-2026, 2026&lt;br&gt;
                We studied the crust beneath Celebes Sea and Makassar Strait in East Indonesia to better understand how the region formed and moves today. Using ocean-bottom and land-based seismometers, we discovered significant differences in crust thickness and unusual underground structures associated with major faults. These findings help explain past tectonic activity and may improve understanding of earthquake hazards in the area.
            </summary>
            <content type="html">
                &lt;b&gt;Offshore crustal thickness variation along the Palu–Koro strike–slip fault in the Sulawesi region from OBS receiver function analysis&lt;/b&gt;&lt;br&gt;
                Tingwei Yang, ChuanChuan Lü, Tianyao Hao, Nicholas Rawlinson, Tao Xu, Pepen Supendi, Sri Widiyantoro, Muhammad Taufiq Rafie, Alfian Alfian, and David Prambudi Sahara&lt;br&gt;
                    Solid Earth, 17, 453&#8211;464, https://doi.org/10.5194/se-17-453-2026, 2026&lt;br&gt;
                <p>The North Sulawesi Subduction Zone is one of the youngest active subduction systems in the western Pacific. In western Sulawesi, the Palu&amp;#8211;Koro strike&amp;#8211;slip fault connects with the westward-extending North Sulawesi Trench, forming a distinctive subduction&amp;#8211;transform fault system. Understanding the crustal structure beneath the Celebes Sea and the geometry of the Palu&amp;#8211;Koro fault is crucial for assessing regional deformation, rupture dynamics, and seismic hazards. In this study, we analyse data from nine ocean bottom seismometers (OBSs) deployed across the Palu&amp;#8211;Koro fault using the receiver function <span class="inline-formula"><i>H</i></span>&amp;#8211;<span class="inline-formula"><i>&amp;#954;</i></span&gt; stacking method to estimate crustal thickness. Our results reveal a shallow Moho (<span class="inline-formula">&amp;#8764;8</span>&amp;#8201;km depth) beneath the Celebes Sea, in contrast to significantly greater depths (<span class="inline-formula">&amp;#8764;25</span>&amp;#8201;km) beneath eastern Kalimantan and northern Sulawesi. Sharp variations in Moho depth near the Palu&amp;#8211;Koro fault suggest the juxtaposition of two distinct crustal blocks. Combining S-wave velocity structures and local seismicity catalogue, we infer that the Palu&amp;#8211;Koro fault is a left-lateral, through-going strike&amp;#8211;slip fault extending into the Celebes Sea. These findings provide new geophysical constraints on the interplay between strike&amp;#8211;slip faulting and subduction retreat, with implications for the generation of tsunamis by submarine earthquakes in this tectonically complex region.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-12T18:16:57+01:00</published>
            <updated>2026-03-12T18:16:57+01:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-429-2026</id>
            <title type="html">Where curling stones collide with rock mechanics: cyclical damage accumulation and fatigue in granitoids
            </title>
            <link href="https://doi.org/10.5194/se-17-429-2026"/>
            <summary type="html">
                &lt;b&gt;Where curling stones collide with rock mechanics: cyclical damage accumulation and fatigue in granitoids&lt;/b&gt;&lt;br&gt;
                Derek D. V. Leung, Florian Fusseis, and Ian B. Butler&lt;br&gt;
                    Solid Earth, 17, 429&#8211;452, https://doi.org/10.5194/se-17-429-2026, 2026&lt;br&gt;
                Curling stones often collide with each other during a game. Over time, these collisions cause damage in the striking bands on the sides of the stones. We determined experimentally how hard these stones collide into one another. We then looked at old curling stones to understand how damage builds up in these rocks. We found that early, fast impacts produce fractures until the striking band is saturated in fractures. Repeated impacts after this stage make fractures grow.
            </summary>
            <content type="html">
                &lt;b&gt;Where curling stones collide with rock mechanics: cyclical damage accumulation and fatigue in granitoids&lt;/b&gt;&lt;br&gt;
                Derek D. V. Leung, Florian Fusseis, and Ian B. Butler&lt;br&gt;
                    Solid Earth, 17, 429&#8211;452, https://doi.org/10.5194/se-17-429-2026, 2026&lt;br&gt;
                <p>Fatigue and damage accumulation in granitoids are classical, but poorly characterised, rock mechanics problems. We explore these phenomena by examining curling stone impacts. Curling stones are slid on ice and made to collide along a circumferential striking band. This well constrained scenario involves uniaxial compression of convex surfaces (i.e., Hertzian contacts). Conservatively, each stone experiences about 2900 impacts per season, over a lifespan of 10&amp;#8211;15&amp;#160;years before refurbishment, providing a unique opportunity to study fatigue and damage accumulation under dynamic cyclic loading.</p&gt;        <p>Here, we first determine the stress magnitudes of head-on curling stone impacts using on-ice experiments involving a high-speed camera and pressure-sensitive films. We then characterise the damage observed in aged stones using photogrammetry, microtomography, and microscopy. For high-velocity impacts (<span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M1" display="inline" overflow="scroll" dspmath="mathml"><mrow><mn mathvariant="normal">2.93</mn><mo>&amp;#177;</mo><mn mathvariant="normal">0.15</mn><mspace linebreak="nobreak" width="0.125em"/><mrow class="unit"><mi mathvariant="normal">m</mi><mspace linebreak="nobreak" width="0.125em"/><msup><mi mathvariant="normal">s</mi><mrow><mo>-</mo><mn mathvariant="normal">1</mn></mrow></msup></mrow></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="83pt" height="14pt" class="svg-formula" dspmath="mathimg" md5hash="7f100d4c948a282ee7f1135ea89d0647"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="se-17-429-2026-ie00001.svg" width="83pt" height="14pt" src="se-17-429-2026-ie00001.png"/></svg:svg></span></span>), a curling stone is locally and momentarily stressed to 300&amp;#8211;680&amp;#8201;MPa, exceeding its quasi-static unconfined compressive strength and exceeding the threshold for fatigue damage for repeated dynamic loadings. Curling stone impacts are dynamic in nature, as evidenced by (1)&amp;#160;high strain rates (<span class="inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" id="M2" display="inline" overflow="scroll" dspmath="mathml"><mrow><mn mathvariant="normal">24</mn><mo>&amp;#177;</mo><mn mathvariant="normal">4</mn><mspace linebreak="nobreak" width="0.125em"/><mrow class="unit"><msup><mi mathvariant="normal">s</mi><mrow><mo>-</mo><mn mathvariant="normal">1</mn></mrow></msup></mrow></mrow></math><span><svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="49pt" height="14pt" class="svg-formula" dspmath="mathimg" md5hash="6a2e3883fac6e54cdd6fe73f0b9496e9"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="se-17-429-2026-ie00002.svg" width="49pt" height="14pt" src="se-17-429-2026-ie00002.png"/></svg:svg></span></span>) that lie below those of co-seismic rock pulverization; (2)&amp;#160;ejection of rock powder during collisions and the presence of potential spalling microcracks; and (3)&amp;#160;presence of striations on crescent-shaped fractures, which resemble mirror-mist-hackle patterns indicative of dynamic microcrack propagation. In the striking band, damage is confined to macroscopic Hertzian cone fractures and their immediate collet zones, and does not appear to extend beyond about 3&amp;#8211;5&amp;#8201;cm into the stones (radially). The circumferential density of cone fractures is limited to about 2&amp;#8211;2.5&amp;#8201;<span class="inline-formula">cm<sup>&amp;#8722;1</sup></span>.</p&gt;        <p>We propose that (1)&amp;#160;early, high-velocity impacts initiate cone fractures up to a specific spatial density, and (2)&amp;#160;with subsequent collisions in the same regions of the striking band, cone fractures progressively propagate and coarsen. This concentrates and channels the accumulated damage, shielding the rest of the stone from reaching critical stress levels for damage. Our findings are significant for applications where rocks are exposed to repetitive, high-stress impacts and suggest that narrow damage zones can dissipate high-impact stresses.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-05T18:16:57+01:00</published>
            <updated>2026-03-05T18:16:57+01:00</updated>
        </entry>
        <entry>
            <id>https://doi.org/10.5194/se-17-407-2026</id>
            <title type="html">Feldspar alteration by disequilibrium CO<sub>2</sub>-H<sub>2</sub>O fluids in reservoir sandstones: implications for CCS
            </title>
            <link href="https://doi.org/10.5194/se-17-407-2026"/>
            <summary type="html">
                &lt;b&gt;Feldspar alteration by disequilibrium CO2-H2O fluids in reservoir sandstones: implications for CCS&lt;/b&gt;&lt;br&gt;
                Natalie J. C. Farrell, Lining Yang, Michael J. Flowerdew, Chris Mark, Buhari Ardo, Kevin G. Taylor, Nico Bigaroni, Michael Pointon, Lewis Hughes, John Waters, and Lee Paul&lt;br&gt;
                    Solid Earth, 17, 407&#8211;427, https://doi.org/10.5194/se-17-407-2026, 2026&lt;br&gt;
                Contrary to current CCS (Carbon Capture and Storage) models, reaction experiments conducted at subsurface stress and temperature conditions reveal that feldspars, common, reactive grains in sandstone reservoirs, can undergo significant chemical and mechanical changes when exposed to CO&amp;#8322; enriched water. These chemo-mechanical processes, including grain fracturing, dissolution, and clay precipitation, can modify fluid pathways and rock strength, potentially reducing reservoir productivity and increasing leakage risk.
            </summary>
            <content type="html">
                &lt;b&gt;Feldspar alteration by disequilibrium CO2-H2O fluids in reservoir sandstones: implications for CCS&lt;/b&gt;&lt;br&gt;
                Natalie J. C. Farrell, Lining Yang, Michael J. Flowerdew, Chris Mark, Buhari Ardo, Kevin G. Taylor, Nico Bigaroni, Michael Pointon, Lewis Hughes, John Waters, and Lee Paul&lt;br&gt;
                    Solid Earth, 17, 407&#8211;427, https://doi.org/10.5194/se-17-407-2026, 2026&lt;br&gt;
                <p>Understanding how the minerals in reservoir rocks respond to <span class="inline-formula">CO<sub>2</sub></span>&amp;#160;injection is vital for the success and safety of Carbon Capture and Storage (CCS) projects. Feldspars are the most common mineral in the Earth's crust and act as primary framework grains in sandstones. Compared to quartz, feldspars are mechanically weak and chemically reactive. Dissolved feldspars can re-precipitate as clays, which in CCS reservoirs could impact fluid-flow. While caprock mineral stability is well studied, reservoir mineral reactivity, particularly of feldspars, remains understudied. To address this knowledge gap, we present microstructural and geochemical data from batch experiments that reacted <span class="inline-formula">CO<sub>2</sub></span>-enriched fluids with feldspar-bearing sandstone sampled from the Captain Sandstone Member, the primary reservoir for the Acorn CCS Project (UK).</p&gt;        <p>Experiments were conducted in a hydrostatic pressure vessel at 70&amp;#8201;<span class="inline-formula">MPa</span&gt; confining pressure, 50&amp;#8201;<span class="inline-formula">MPa</span&gt; pore pressure, and temperatures ranging from 80&amp;#160;to 550&amp;#8201;<span class="inline-formula">&amp;#176;C</span>, using <span class="inline-formula">CO<sub>2</sub></span>-enriched water to simulate reservoir conditions. Pre- and post-reaction samples were analysed using XRD, SEM-EDS, and XCT to assess microstructural and mineralogical changes. Results show that <span class="inline-formula">CO<sub>2</sub>:feldspar</span&gt; interactions differ significantly from control experiments involving water alone. At reservoir-relevant temperatures (80&amp;#8201;<span class="inline-formula">&amp;#176;C</span>), incongruent dissolution of K-feldspar weakened grains which led to microfracturing. At 250&amp;#8201;<span class="inline-formula">&amp;#176;C</span>, <span class="inline-formula">CO<sub>2</sub></span&gt; fluids caused total dissolution of calcite grains and cement and selective leaching of calcium from oligoclase, enriching the pore fluid with <span class="inline-formula">Ca<sup>2+</sup></span>. Above 400&amp;#8201;<span class="inline-formula">&amp;#176;C</span>, coupled dissolution&amp;#8211;precipitation processes were observed, including congruent K-feldspar dissolution, secondary porosity development, and localised precipitation of Ca-aluminosilicates and K-bearing phases around dissolving K-feldspars. These transformations could alter reservoir flow pathways and induce mechanical risks, i.e. destabilising nearby faults or initiating reservoir collapse. Given feldspars' prevalence in crustal rocks and CCS sandstone reservoirs, their reactive behaviour under in-situ conditions and in the presence of aggressive fluids demands greater attention.</p>
            </content>
            <author>
                <name>Copernicus Electronic Production Support Office</name>
            </author>
            <published>2026-03-05T18:16:57+01:00</published>
            <updated>2026-03-05T18:16:57+01:00</updated>
        </entry>
</feed>