TS3.4 | Across the time scales, from earthquakes to earthquake cycle
Orals |
Fri, 10:45
Fri, 08:30
EDI
Across the time scales, from earthquakes to earthquake cycle
Co-organized by G3/NH14
Convener: Y. Klinger | Co-conveners: Alice-Agnes Gabriel, Harsha Bhat, Magali Rizza
Orals
| Fri, 02 May, 10:45–12:30 (CEST)
 
Room G2
Posters on site
| Attendance Fri, 02 May, 08:30–10:15 (CEST) | Display Fri, 02 May, 08:30–12:30
 
Hall X2
Orals |
Fri, 10:45
Fri, 08:30

Orals: Fri, 2 May | Room G2

10:45–10:50
10:50–11:00
|
EGU25-5630
|
ECS
|
On-site presentation
Jianfeng Cai, Yangmao Wen, Kefeng He, and Caijun Xu

The Ganzi-Yushu fault, striking in a northwest direction with a length of approximately 500 km, delineates the boundary between the Bayan Har block and the Qiangtang block. Due to the ongoing collision between the Indian plate and Eurasia plate and the resultant eastward extrusion process in the Tibetan Plateau, the fault system is characterized by rapid left-lateral strike-slip and frequent major earthquake events. The 2010 MS 7.1 Yushu earthquake ruptured the northwestern segment of the fault, resulting in significant casualties and property losses. Apart from the 2010 Yushu earthquake, this fault has experienced four M > 7.0 earthquakes in the past 300 years, marking it as one of the most seismically active fault systems in the Tibetan Plateau.

In this study, we use Sentinel-1 InSAR data spanning from 2014 to 2023 to derive the interseismic velocity fields along the Ganzi-Yushu fault. Based on the interseismic velocity field, we derive the slip rates and interseismic coupling distribution along the Ganzi-Yushu fault using elastic block model. The results indicate left-lateral slip rates of 4.0~6.5 mm/yr along the Ganzi-Yushu fault. We identify five locked segments along strike, which has good consistency with historical earthquakes.

To assess the earthquake potential along the Ganzi-Yushu fault, we simulate earthquake rupture sequences using quasi-dynamic earthquake cycle model. We set the friction coefficient of the rate- and state-dependent friction law according to the interseismic coupling model, thereby obtaining interseismic slip rates in numerical simulations that align with the kinematic results. Our quasi-dynamic earthquake cycle model generates both single- and multi-segment ruptures with magnitudes approximating those inferred from the historical events. Owing to variations in seismogenic width and slip rate, different segments exhibit distinct recurrence intervals, which is consistent with the results from geological surveys. The locations of nucleation and the slip history on fault determine whether a rupture can propagate across multiple segments and generate a major event. By integrating the kinematic model with the physics-based seismic cycle simulations, our results shed light on the earthquake potential along the Ganzi-Yushu fault.

How to cite: Cai, J., Wen, Y., He, K., and Xu, C.: Seismic rupture and earthquake sequence along the Ganzi-Yushu fault in Eastern Tibet: From kinematics to dynamics, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-5630, https://doi.org/10.5194/egusphere-egu25-5630, 2025.

11:00–11:10
|
EGU25-2504
|
On-site presentation
Junjie Ren, Guangchun Xu, and Xiwei Xu

Surface ruptures associated with large historical earthquakes provide critical insights into earthquake magnitudes and the kinematics of their seismogenic faults. In 1955, a major earthquake occurred along the Zheduotang fault, a segment of the southern Xianshuihe fault zone in eastern Tibet. The magnitude of this earthquake has been a subject of debate, with estimates ranging from M6.6 to M7.5, primarily due to conflicting interpretations of its associated surface ruptures. This study reviews previous research on the surface ruptures of the 1955 Zheduotang earthquake and presents new field data, including unmanned aerial vehicle (UAV)-based topographic surveys, trench excavations, and lichenometry in the epicentral region. Evidence from the freshness of ground ruptures, dating of faulting events from trenching, and lichen size measurements supports a ~55 km long surface rupture zone, corresponding to a moment magnitude (Mw) of ~7.1 for the 1955 earthquake. Analysis of offset glacial interfluves reveals a late Quaternary left-lateral slip rate of ~2.5–3.0 mm/yr in the southern segment of the Zheduotang fault, lower than ~3.4–4.8 mm/yr previously observed in the northern section. Deformed landforms and surface ruptures indicate that the fault trends NWN and exhibits predominantly left-lateral strike-slip motion in its northern section, while the southern segment trends NW and includes a notable normal faulting component. Our findings suggest that the Zheduotang fault delineates the southwestern boundary of the Bamei-Kangding releasing stepover zone within the southern Xianshuihe left-lateral strike-slip fault zone. These results enhance understanding of seismic hazards and the tectonic kinematics along the eastern boundary of the Tibetan Plateau.

How to cite: Ren, J., Xu, G., and Xu, X.: Revisiting surface ruptures of the 1955 Zheduotang earthquake (M ~7.5) in eastern Tibet: kinematic implications on the southern Xianshuihe fault zone, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-2504, https://doi.org/10.5194/egusphere-egu25-2504, 2025.

11:10–11:20
|
EGU25-19215
|
ECS
|
On-site presentation
Nicolas Pinzon Matapi, Yann Klinger, Xiwei Xu, Paul Tapponnier, Jing Liu‐Zeng, Jerome Van Der Woerd, Kang Li, and Mingxing Gao

The understanding of the spatial‐temporal distribution of past earthquakes is essential to assess the event recurrence behavior and to estimate the size of potential earthquakes along active strike‐slip fault systems. However, the scarcity of paleoseismic data remains a major hurdle in this endeavor. This is the case of the longest strike‐slip fault in Asia, the Altyn Tagh Fault (ATF). We documented six very likely large earthquakes that potentially ruptured the Aksay section of the ATF. Employing a Bayesian approach, we present modeled date ranges of 6339–5220 BC, 5296–4563 BC, 3026–2677 BC, 1324–808 BC, 314–632 AD, and 915– 1300 AD. The mean recurrence time is 1,329 ± 588 years with a coefficient of variation (COV) of ∼0.44. In the same fault section, 90 horizontal offsets record an average coseismic slip of 5.1 ± 1.4 m for the last event and suggest four older earthquakes plausibly with a similar slip distribution. Although at the local‐scale the COV indicates quasi‐periodic rupture behavior, the individual interevent times exhibit significant irregularity, a pattern also observed in adjacent fault sections (Xorxoli, Annanba and Tashi sections). We found that such irregularities are a natural consequence of long‐term fault interactions, which allow for synchronized ruptures along the northern and southern strands of the central‐eastern ATF. Our rupture model highlights bursty periods of seismic activity with mean interevent times of 475 ± 108 years separated by long‐lull periods of 1.1–1.6 kyr. Based on this temporal organization and considering the 401‐year elapsed time since the most recent event on the Xorxoli section, there exists a possibility of a forthcoming large earthquake occurring within the next century. 

How to cite: Pinzon Matapi, N., Klinger, Y., Xu, X., Tapponnier, P., Liu‐Zeng, J., Van Der Woerd, J., Li, K., and Gao, M.: Spatiotemporal Clustering of Large Earthquakes Along the Central‐Eastern Sections of the Altyn Tagh Fault, China, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-19215, https://doi.org/10.5194/egusphere-egu25-19215, 2025.

11:20–11:30
|
EGU25-4021
|
ECS
|
On-site presentation
Shmuel Marco, Shimon Wdowinski, Yin Lu, Anne Le Blanc, and Machel Higgins

The Dead Sea Basin, a pull-apart basin situated along the Sinai-Arabia transform plate boundary, presents a unique natural laboratory to examine the long-term variability of earthquake activity through its extensive paleoseismic record, spanning the past 220,000 years. This record is constructed from borehole and outcrop data documenting seismites—earthquake-induced sedimentary deformations formed within the ancient lakes of the basin. Preliminary studies have identified a strong correlation between earthquake occurrence and fluctuations in lake levels, pointing to a potential climatic influence on seismic activity.

Through an NSF-funded project, we aim to quantify the relationship between lake-level variations and the paleo-earthquake record by investigating the mechanisms underlying seismite formation. These processes include sediment accumulation, seismic shaking, unit disruption, gravitational sliding, and subsequent deposition. Seismic shaking results from the interplay of tectonic processes such as strain accumulation, surface load changes, pore pressure variations, and stress release. This shaking interacts with sedimentary processes to form seismites. The study incorporates five research components: (1) advanced time series analyses of the 220 ka seismite record; (2) spatial detection analysis to assess the uncertainty of single-core paleo-earthquake event detection; (3) geospatial paleo-bathymetry analysis of sediment availability for turbidite generation at different lake levels; (4) fluid mechanical modeling of sediment rheology and deformation style at varying lake levels; and (5) pore fluid pressure, fault strength and mechanical modeling related to earthquake occurrence on both primary strike-slip and secondary normal faults at This research aims to elucidate the role of climatic factors in modulating seismic activity within the Dead Sea Basin. By integrating methodologies from geology, geodesy, geophysics, paleoseismology, paleoclimatology, and sedimentology, the study provides critical insights into the physical processes governing long-term earthquake variability along continental transform faults.

How to cite: Marco, S., Wdowinski, S., Lu, Y., Le Blanc, A., and Higgins, M.: Paleoseismic Records of the Dead Sea Reveals Climatic Modulation of Seismicity Along the Continental Transform Fault, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-4021, https://doi.org/10.5194/egusphere-egu25-4021, 2025.

11:30–11:40
|
EGU25-16028
|
ECS
|
On-site presentation
Natalie Forrest, Laura Gregory, Tim Craig, Tim Wright, Richard Shanks, Bora Uzel, and Elif Çam

Seismic hazard models often assume near-constant earthquake recurrence intervals on faults since the Last Glacial Maximum, approximately 15,000 years ago. However, it is tricky to show that real fault systems exhibit this behaviour, particularly for distributed networks of normal faults in extensional regimes. Instead, data is limited to historical seismology records, which is likely over a much shorter time than earthquake recurrence intervals, or a single time-averaged Holocene slip rate from paleoseismology methods. Neither method measures slip rate variability over multiple earthquake cycles.

Cosmogenic nuclide analysis on limestone bedrock fault scarps, combined with Bayesian modelling, is an established method to interpret exhumation histories of normal faults since the Last Glacial Maximum. Production of chlorine-36 (36Cl) is primarily by interaction of calcium-40 in the limestone scarp with cosmic rays. Concentration profiles of 36Cl on a fault scarp therefore correlate with fault slip in earthquakes. Previous 36Cl studies demonstrate slip rate variability of normal faults in Italy and Türkiye.

We apply this technique to interpret the slip history of the Eşen Fault, a major normal fault in southwest Türkiye with no known historical seismicity. Bayesian models suggest the last major earthquake was 1000 years ago, but prior to that, there was a period of fast slip of 2-3 mm/yr, which exposed at least 5 m of scarp in 2-3 kyr. Before that, the slip rate was much lower, at about 1 mm/yr. These results demonstrate slip rate variability, which informs our understanding of fault dynamics over millennia, and may help to improve seismic hazard models.

How to cite: Forrest, N., Gregory, L., Craig, T., Wright, T., Shanks, R., Uzel, B., and Çam, E.: Measuring slip rate variability on the Eşen Fault, SW Türkiye, with cosmogenic chlorine-36 nuclide analysis, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-16028, https://doi.org/10.5194/egusphere-egu25-16028, 2025.

11:40–11:50
|
EGU25-7699
|
ECS
|
On-site presentation
What can the limited and uncertain geological record tell us about the earthquake cycle?
(withdrawn)
Jonathan Griffin, Ting Wang, and Mark Stirling
11:50–12:00
|
EGU25-11371
|
ECS
|
On-site presentation
Jorge Jara, Mathieu Soret, Nadaya Cubas, Andrei Maksymowicz, Fabrice Cotton, and Romain Jolivet

Aseismic slip, particularly in the form of Slow Slip Events (SSEs), plays an undisputed role in the release of stress along faults, occurring slowly and without generating classical seismic waves. SSEs are recognized as critical phenomena influencing various stages of the seismic cycle, including postseismic phases, earthquake triggering or arresting, and interseismic transients. However, the mechanisms governing their underlying physics remain debated. Three primary hypotheses have been proposed: (1) heterogeneities in fault constitutive properties that may drive episodic SSEs; (2) stress interactions arising from geometric complexities (e.g., damage zones) that could explain the full observed slip spectrum; and (3) the influence of fluids circulating along fault zones, which increase pore pressure and reduce normal stress, thereby promoting slip. To investigate these mechanisms, we integrate SSE databases, slab thermal models, and thermodynamic metamorphic modeling.

Our study examines nine subduction zones around the Pacific region, using thermal slab models that account for uncertainties in temperature estimations. By using an extensive SSE database (1800 events, Slow Earthquake Database, from the Japanese project “Science of Slow-to-Fast Earthquakes), we compare modeled temperature and pressure conditions with observed SSE distributions. Statistical analysis reveals two distinct temperature ranges where SSEs cluster: approximately 100°C and 350–550°C. Thermodynamic modeling of mafic rocks under subduction conditions indicates that the 100°C cluster aligns with the smectite-to-illite transition, a reaction known to release significant amounts of water. The 350–550°C cluster corresponds to metamorphic transitions from greenschists to amphibolites, which also release considerable water. SSEs are notably absent at pressure-temperature conditions where mafic rocks are fully dehydrated.

The water released during such metamorphic reactions increases pore pressure, reduces normal stress, and facilitates slip. While the mechanisms sustaining slow slip—such as nucleation length or dilatant stress—remain debated, our results suggest that water release due to metamorphic reactions is a key trigger for SSEs along subduction interfaces. In addition to the release of fluids, we hypothesize that the change in resistance induced by the change in mineralogical configuration might also play a role in the nucleation of SSEs. These findings highlight the importance of integrating geophysical observations with petrological processes to better understand the dynamics of SSE in subduction zones

How to cite: Jara, J., Soret, M., Cubas, N., Maksymowicz, A., Cotton, F., and Jolivet, R.: Metamorphic dehydration reactions trigger slow slip events in subduction zones, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-11371, https://doi.org/10.5194/egusphere-egu25-11371, 2025.

12:00–12:10
|
EGU25-4256
|
ECS
|
On-site presentation
Tobias Köhne, Rishav Mallick, Théa Ragon, and Mark Simons

The evolution of the shear traction at plate interfaces is a key input to seismic hazard assessments, as it relates rheological properties of the interface material to the slip history of the fault. However, at the relevant spatial scales, shear tractions can only be modelled indirectly, with kinematic coupling commonly used as a proxy for inferring any slip deficit that drives seismic hazard. When the 2011 Mw 9.1 Tohoku-oki earthquake ruptured the Northern Japanese megathrust, it did so in an area where simplified models estimated low-to-medium kinematic coupling (Uchida and Bürgmann, 2021). 
The reliance on kinematic coupling for seismic hazard assessment could be reduced if instead the long-term slip budget (or equivalently, the shear stress history) could be estimated for a given fault zone. Such a method, in turn, would require the definition of specific constitutive laws in order to simulate multiple earthquake super-cycles, as well as an inversion independent of initial conditions. We have built such a scheme building on previous work (Kanda and Simons, 2010; Hetland and Simons, 2010; Kanda et al., 2013; Mallick et al., 2022; Köhne et al., in press). Our approach assumes that the plate interface is divided into fully-locked asperities surrounded by regions of the fault interface characterized by rate-dependent friction. We impose a historically realistic rupture timeline for each of the assumed asperities, but let the remaining fault interface evolve freely otherwise according to its mechanical properties, until it obtains cycle-invariance. After reaching the time period where GNSS observations of the region exist, we calculate the residuals to surface displacement timeseries, and use a Bayesian inference approach to estimate the best-fit frictional parameters. This inference is sensitive to our inherent ignorance of the elastic structure of the area around the plate interface. Therefore, we extend our framework to assess the impact of such heterogeneity.
We present results from our updated Northern Japanese subduction zone model, where we consider both pre- and post-2011 Tohoku-oki earthquake GNSS surface displacement observations. We first show, using a homogeneous halfspace model, how estimates of slip deficit and kinematic coupling differ.  We also find that the product of the rate-dependent frictional parameter (a-b) with effective normal stress generally decreases with depth. We then show how these conclusions change after considering the more realistic 3D elastic structure of Hashima et al. (2016), who have shown the importance for the coseismic fault slip and associated surface deformation (Hsu et al., 2011; Ragon and Simons, 2023). The structure includes depth-varying elastic moduli for the continental plate, down going slab, and mantle. Using PyLith, we calculate the relevant stress and displacement kernels for our earthquake simulation framework. Our model results provide important perspectives for future seismic hazard assessments and postseismic studies of rheological properties.

How to cite: Köhne, T., Mallick, R., Ragon, T., and Simons, M.: The Impact of 3D Elastic Structure on Estimates of Megathrust Frictional Properties Derived from Earthquake Cycle Inversions of Pre- and Post-2011 Tohoku-oki Earthquake GNSS Observations, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-4256, https://doi.org/10.5194/egusphere-egu25-4256, 2025.

12:10–12:20
|
EGU25-11563
|
ECS
|
On-site presentation
Sylvain Michel, Diego Molina-Ormazabal, Jean-Paul Ampuero, Andrés Tassara, and Romain Jolivet

To become very large earthquakes, seismic ruptures that saturate the seismogenic width (M>8.3 in subduction zones) need to propagate long distances along-strike. Multiple factors can hinder this propagation, among them the available energy on the fault. A recent extension of Linear Elastic Fracture Mechanics theory to elongated ruptures provides a framework to estimate when a portion of a fault has enough potential energy, and is hence sufficiently loaded, to generate a large earthquake. Based on this framework, we present a method that takes into account the along-strike distribution of available energy to evaluate, using a probabilistic approach, the timing and magnitude of potential future large earthquakes, and thus the seismogenic potential of the fault. This approach assumes that the ruptures have already saturated the seismogenic width of the fault. We apply and assess this method on the Chilean subduction zone. We first perform a sensitivity test and explore the impact of the uncertainties of model parameters on the timing Tc at which a section of a fault is ready to host large ruptures. This initial test shows that Tc is controlled by the uncertainty of the parameter B, a coefficient involved in the scaling between fracture energy and final slip, which controls the energy consumed by the rupture. We further constrain B by comparing the observed interevent time between ~M9.5 earthquakes on the Valdivia segment and the one predicted from our model, assuming that such earthquakes occur as soon as the fault is ready to host it. Fixing B to this constrained value, we then estimate the evolution of the probability of earthquakes exceeding M8.5 over the whole Chilean subduction. Along-strike heterogeneity of the available energy arises from the heterogeneity of the loading rate, based on an geodetically-inferred coupling map, and from the along-strike changes of the seismogenic width. Our results highlight that the earthquake potential on a specific segment can be significantly altered by the occurrence of earthquakes on neighboring segments. This is illustrated by the drops in the probability of >M8.5 events on the Copiapo segment after the 2010 Maule and 2015 Illapel earthquakes. By combining our estimates with the rate of events that saturate the seismogenic zone, we are able to estimate the probability of occurrence of >M8.5 events. Such physics-based modeling is a novel approach to time-dependent seismic hazard analysis.

How to cite: Michel, S., Molina-Ormazabal, D., Ampuero, J.-P., Tassara, A., and Jolivet, R.: Spatio-temporal evolution of earthquake potential constrained by a physical and statistical approach: Application to the Chilean subduction zone, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-11563, https://doi.org/10.5194/egusphere-egu25-11563, 2025.

12:20–12:30
|
EGU25-5899
|
On-site presentation
Olaf Zielke, Theodoros Aspiotis, Sarah Fadhladeen, and Paul Martin Mai

Seismic hazard assessment (SHA) requires, among other components, a comprehensive representation of seismic sources that could affect sites or regions of interest, including their location and seismogenic character. Observational earthquake catalogs are generally too short or incomplete to provide a comprehensive source representation. Computer-generated earthquake catalogs, created by physics-based earthquake cycle simulations, can augment the observational catalogs, therefore contributing to improved SHA. With MCQsim, we developed an earthquake cycle simulator with this purpose in mind. MCQsim is openly available via GitHub. Since its initial publication in 2023, we were able to improve the code substantially, improving its performance and scalability, therefore enabling simulation for large-scale fault systems. Additionally, we built an interface between MCQsim and seismic hazard engine OpenQuake to streamline the incorporation of simulated catalogs into PSHA.

Here, we want to showcase these recent improvements. We perform earthquake cycle simulations for the Gulf of Aqaba and East Anatolian fault systems, creating earthquakes catalogs that span tens of thousands of years, with magnitude ranging from M3.5 to M7.8+. We validate these catalogs with observational constraints of the respective fault systems. Using these simulated catalogs, we investigate the occurrence of earthquake sequences, highlighting variations in large-earthquake occurrence probability as a function of time. We further showcase the integration of simulated catalogs into the OpenQuake environment, creating seismic hazard maps.

How to cite: Zielke, O., Aspiotis, T., Fadhladeen, S., and Mai, P. M.: Earthquake cycle simulations for seismic hazard assessment, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-5899, https://doi.org/10.5194/egusphere-egu25-5899, 2025.

Posters on site: Fri, 2 May, 08:30–10:15 | Hall X2

Display time: Fri, 2 May, 08:30–12:30
X2.7
|
EGU25-19994
|
ECS
Gayatri Indah Marliyani, Yann Klinger, Wenqian Yao, Agung Setianto, Hurien Helmi, Telly Kurniawan, Rahmat Triyono, Andi Azhar Rusdin, Supriyanto Rohadi, and Dwikorita Karnawati

The Aceh Fault, part of Indonesia's Great Sumatran Fault System, exhibits recent faulting through prominent scarps along its 250-kilometer length. Running northwest-southeast, it spans northwestern Sumatra from Tripa to Banda Aceh, a city of over 268,000 residents. Understanding the complete faulting history is essential for assessing seismic risk, as instrumental records are too recent to capture long-term patterns. We study the fault by combining remote sensing using 8-m resolution DEM (DEMNAS) for the entire area and 15-cm resolution (LiDAR drone survey) for selected areas, field methods, and paleoseismology. We excavated two paleoseismic trenches across the fault and documented evidence of at least three well-dated ground-rupturing earthquakes from the upper 2 meters of strata spanning the last ~1000 years. The event chronology is constrained by 15 radiocarbon dates on detrital charchoal. This new paleoseismic data confirms that the Aceh Fault is active. Our study delineates the active trace of the fault zone and provides the first detailed information about significant prehistoric earthquakes along this fault. These findings improve seismic hazard maps and enhance understanding of the region's seismic risks.

How to cite: Marliyani, G. I., Klinger, Y., Yao, W., Setianto, A., Helmi, H., Kurniawan, T., Triyono, R., Rusdin, A. A., Rohadi, S., and Karnawati, D.: Preliminary Results of the Paleoseismology of Aceh Fault in northern Sumatra, Indonesia, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-19994, https://doi.org/10.5194/egusphere-egu25-19994, 2025.

X2.8
|
EGU25-876
|
ECS
Constanza Rodriguez Piceda, Zoë Mildon, Billy Andrews, Yifan Yin, Jean-Paul Ampuero, Martijn van den Ende, and Claudia Sgambato

Stress interactions between neighbouring faults plays a key role in controlling earthquake recurrence and size, and therefore in the seismic hazard posed by individual faults within a fault network. In this study, we investigate how differences in the predominant arrangement of faults, specifically, whether it is along-strike or across-strike, affect earthquake recurrence rates and magnitude of earthquakes. To address this topic, we use the boundary-element code QDYN to simulate earthquake cycles of two fault systems within the actively extending region of the Italian Apennines: one to the south where faults are predominantly arranged along-strike, and another in the central Apennines where faults are predominantly arranged across-strike.  The different styles of fault network between the Central and Southern Apennines, and high seismic hazard of the region, make this the ideal area to investigate the role of fault geometry on earthquake behaviour across multiple seismic cycles in this region.

The models account for variable fault slip rates between faults and network geometry to determine their impact on seismic cycles and earthquake statistics. These simulations produce spontaneous ruptures, with slip modes encompassing full and partial ruptures as well as slow-slip events. We found a good fit between the modelled magnitudes and the ones derived from historical ruptures and empirical relationships. Fault networks with multiple across-strike faults produce more complex seismic sequences, including greater variability in recurrence times and higher proportion of partial ruptures, compared to fault networks with faults arranged predominantly along-strike. Lastly, we assessed the seismic hazard in the studied regions based on the modelled earthquake rates and magnitudes. Our findings show that the spatial distribution of peak ground acceleration corresponding to a 50-year exceedance probability has a greater heterogeneity compared to classical seismic hazard assessment approaches. Hazard levels are elevated in areas where multiple faults overlap, highlighting the influence of fault interactions on regional hazard patterns. These findings show the influence of fault system geometry on how stresses redistribute across multiple earthquake cycles and associated seismic hazard.

How to cite: Rodriguez Piceda, C., Mildon, Z., Andrews, B., Yin, Y., Ampuero, J.-P., van den Ende, M., and Sgambato, C.: Seismic sequences in the Italian Apennines influenced by fault network geometry , EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-876, https://doi.org/10.5194/egusphere-egu25-876, 2025.

X2.9
|
EGU25-2435
|
ECS
Wenjun Kang, Zhanfei Li, and Xiwei Xu

The characteristics and factors that control the Off-Fault Deformation(OFD)remain poorly understood. The existing studies shows the 2021 Mw 7.4 Maduo earthquake produce the largest OFD than other earthquake cases. We try to use the China Gaofen-serie-satellite images to re-constrain the OFD deformation. By correlating pairs of images before and after this earthquake, we obtain the coseismic deformation parttern of  the 2021 Mw 7.4 Maduo earthquake. By measuring the coseismic deformation, we constrain the near-field and far-field surface displacement distribution. The result shows that this earthquake accommodated 69% of total surface deformation as OFD deformation over a mean deformation-zone width of 237 m.  Our result show the OFD proportation of the Maduo earthquake is large, but our result is lower than the result by using the SPOT and Sentienl-2 images. By analying the fault geometry  and geological deposit, we think the magnitude and width of off-fault deformation along the rupture is primarily controlled by the fault maturity and structural complexity of the fault. 

How to cite: Kang, W., Li, Z., and Xu, X.: Large Off-Fault Deformation of 2021 Mw 7.4 Maduo Earthquake along an Immature Strike-Slip Fault, Tibetan Plateau, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-2435, https://doi.org/10.5194/egusphere-egu25-2435, 2025.

X2.10
|
EGU25-4056
|
ECS
Simona Guastamacchia, Fabio Corbi, Giacomo Mastella, Silvia Brizzi, and Francesca Funiciello

Subduction megathrusts are among the largest fault systems on Earth and are responsible for generating megaearthquakes-the most powerful earthquakes and one of the most destructive natural phenomena. However, obtaining natural data on the Subduction Earthquake Cycle (SEC) in these areas is challenging due to the long recurrence intervals of such events. To overcome this limitation, we used analogue models to reproduce in the laboratory hundreds of seismic cycles under different conditions in just a few minutes. The models feature a single velocity weakening asperity (i.e., rice) surrounded by a velocity-neutral material (i.e., sand). Using a parametric approach, we systematically varied two key parameters of our single asperity model: (1) the rheology of the upper plate, which affects its stiffness and (2) the normal load (σn) applied on the asperity. We performed four distinct models, each with a different upper plate stiffness. For each upper plate stiffness we implemented four σn (i.e., 16 models in total). High-resolution monitoring of our models, combined with Particle Image Velocimetry, allowed for a detailed analysis of the analog earthquakes. The variation in upper plate rheology enabled the models to simulate the transition from stick-slip behavior to stable sliding, governed by the ratio k/kc, the stability parameter within the rate-and-state framework. Moreover, the models demonstrate that this variation is a controlling factor of magnitude and recurrence time of the analogue events. Comparing the results with natural data, we found that all the models exhibit moment magnitudes (Mw) comparable to those of natural megaearthquakes. The possibility of crossing the k/kc=1 threshold allows us to explore the stick-slip behavior in a regime that includes period doubling linked to the coexistence of faster and slower slip rates. The findings in our experimental models demonstrate the influence of the upper plate rheology in the spectrum of megathrust slip behaviors, providing constraints that could potentially be applied to natural subduction zones. 

How to cite: Guastamacchia, S., Corbi, F., Mastella, G., Brizzi, S., and Funiciello, F.: Subduction Earthquake Cycle through the lens of analogue modelling: the role of the upper plate rheology, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-4056, https://doi.org/10.5194/egusphere-egu25-4056, 2025.

X2.11
|
EGU25-4323
|
ECS
|
James Wood, Alexander Whittaker, Rebecca Bell, Haralambos Kranis, Athanassios Ganas, and Gwenn Peron-Pinvidic

Normal faults in a rate-and-state friction model release seismic energy in distinct, instantaneous seismic events (i.e. earthquakes) between steady state periods. However, recent geodetic work in the Gulf of Corinth, Greece suggests that some seismogenic normal faults can also undergo transient aseismic slip events above steady state deformation rates in interseismic periods. Integrating the full range of fault slip behaviours into fault evolution frameworks is required to better constrain how normal faults accommodate and release strain with implications for rift development and seismic hazard. Therefore, further detailed observation of both coseismic and aseismic slip behaviours across normal faults at all time scales are needed.

In this analysis, we exploit open-source, vertical ground motion data from the European Ground Motion Service (EGMS), derived from five-years of Interferometric Synthetic Aperture Radar (InSAR) measurements, to evaluate uplift and subsidence in areas of active tectonics. While vertical ground motion data likely reflects a range of geological, hydrological and anthropogenic processes, isolating tectonic signals allows quantification of fault motion on annual to decadal time scales using the Europe-wide dataset. Therefore, this data bridges an important time-scale gap between event-specific InSAR studies and geological assessments and provides regional context to ground motion. Here, we use time series spanning 2019 to 2023 to assess vertical ground motion across normal faults in Central Greece that have, and have not, hosted large earthquakes in this period.

Spatio-temporal ground motion analysis is conducted for the March 2021, Mw > 6 earthquakes in the Larissa Basin (Thessaly). The cascading rupture style of the earthquakes and aftershocks is resolved in EGMS time series, and geometries of uplift and subsidence are plotted to define rupture parameters and fault plane projections. High coseismic uplift to subsidence ratios of 1:6 – 1:9 reflect the tight structural controls on this earthquake sequence. In contrast to Larissa, EGMS time series across the Coastal Fault System of the North Gulf of Evia imply aseismic normal fault slip. Differential vertical ground motion is recorded across both the Kamena Vourla and Arkitsa fault segments with little to no associated seismicity. Time-averaged throw rates of 2 - 3 mm/yr are measured at an uplift to subsidence ratio of 1:2. These throw rates exceed the long-term, geodetic extension rates across the North Gulf of Evia suggesting that the faults are moving in a transient period of elevated aseismic slip between 2019 and 2023. The nearby Atalanti Fault, which hosted two Mw > 6.4 earthquakes in 1894, shows no differential ground motion across its plane reflecting that the fault is in a locked state. The observed variable shallow crustal behaviour of normal faults implies long-term, geologically derived throw rates on normal faults likely combine transient periods of elevated aseismic slip, coseismic slip, and steady state strain accommodation.

How to cite: Wood, J., Whittaker, A., Bell, R., Kranis, H., Ganas, A., and Peron-Pinvidic, G.: Coseismic and aseismic normal fault slip in Central Greece from InSAR time series, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-4323, https://doi.org/10.5194/egusphere-egu25-4323, 2025.

X2.12
|
EGU25-5877
|
ECS
|
Cecilia Martinelli, James Hollingsworth, Romain Jolivet, and Marion Thomas

The study of natural hazards like earthquakes requires accurate measurement of ground displacement. When paired with high-resolution satellite imagery, Optical Image Correlation (OIC) has proven to be highly effective in mapping near-field ground displacements for large earthquakes, offering detailed and precise data. This is crucial for understanding fault mechanics and the generation of strong ground motions during shallow earthquakes.

OIC has several advantages over field or traditional geodetic methods. First, it is robust against image noise, allowing meaningful data extraction from various types of imagery, even when separated over long time periods. Second, unlike InSAR, OIC does not suffer from decorrelation close to fault ruptures, thus providing rich data in the near-field region and offering insight into shallow fault characteristics. Third, OIC has subpixel resolution, enabling the detection of small (cm-scale) displacements. Fourth, OIC provides dense displacement measurements that would be difficult to replicate with field methods. Finally, OIC can help to identify subtle ground features and long-wavelength displacement signals, including those associated with off-fault deformation. OIC has been widely used to characterize near-field displacements during several recent surface-rupturing earthquakes. Displacements measured by OIC typically surpass field measurements due to the latter's inability to capture smaller, distributed deformations away from the primary fault rupture. OIC data can thus help us to more accurately infer the width of the fault zone, encompassing both on-fault and off-fault deformation. 

Studies on the 2019 Ridgecrest earthquake used various optical datasets and correlation methods to explore near-field displacement and the extent of off-fault deformation. However, the choice of correlation approach used can impact the magnitude and nature of the observed deformation, which, in turn, may impact subsequent analysis of the strain field. 

This study aims to analyze multiple correlation algorithms (MicMac, COSI-Corr, Ames Stereo Pipeline and AmpCor) and optical datasets (Pleiades, WorldView, Spot and ADS80), spanning a range of resolutions, incidence angles, and temporal variations. We explore how correlation techniques influence displacement values and whether they can artificially smooth discrete fault offsets, creating apparent (artificial) off-fault deformation. Using synthetic tests and the 2019 Ridgecrest earthquakes as a case study, we explore the variability in off-fault deformation and fault zone width, depending on the processing approach adopted. Ultimately, we highlight the limitations of OIC in quantifying off-fault deformation, thus providing constraints on the extent to which such data can be used to address aspects of fault mechanics.

How to cite: Martinelli, C., Hollingsworth, J., Jolivet, R., and Thomas, M.: How well can displacement be resolved close to earthquake surface ruptures using optical image correlation?  , EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-5877, https://doi.org/10.5194/egusphere-egu25-5877, 2025.

X2.13
|
EGU25-6505
Jiapei Wang, Qingqing Tan, and Chongyang Shen

On September 5, 2022, a magnitude Ms6.8 earthquake occurred in Luding County, Sichuan Province. This earthquake occurred at the key part of the southeast-clockwise extrusion of material on the eastern margin of the Tibetan Plateau, the Y-shaped confluence of the Xianshuihe, Longmenshan and Anninghe fault zones. In this study, the three-dimensional dynamic crustal density changes in the earthquake area are obtained by the typical gravity change data from 2019 to 2022 before the earthquake and gravity inversion by growing bodies. The results indicate that gravity changes presented an obvious four-quadrant and gradient belt distribution in the Luding area before the earthquake. The three-dimensional density horizontal slices show that small density changes occurred at the epicenter in the mid-to-upper crust between 2019.9 - 2020.9 and 2019.9 - 2021.9. At the same time, the surrounding areas exhibited a positive and negative quadrant distribution. These observations indicate that the source region was likely in a stable locked state, with locking in shear forces oriented in the NW and NE directions. From 2021.9 to 2022.8, the epicentral region showed negative density changes, indicating that the source region was in the expansion stage, approaching a near-seismic state. The three-dimensional density vertical slices reveal a southeastward migration of positive and negative densities near the epicenter and on the western of the Xianshuihe Fault Zone, indicating that the material is flowing out to the southeast. The observed local negative density changes at the epicenter along the Longmenshan Fault Zone are likely associated with the NE-oriented extensional stress shown by the seismic source mechanism. The above results can provide a basis for interpreting pre-earthquake gravity and density changes, thereby contributing to the advancement of earthquake precursor theory.

How to cite: Wang, J., Tan, Q., and Shen, C.: Dynamic changes of gravity field before the Luding Ms6.8 earthquake and its crustal material migration characteristics, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-6505, https://doi.org/10.5194/egusphere-egu25-6505, 2025.

X2.14
|
EGU25-9148
Laurent Bollinger, Laure Manceau, Yann Klinger, Jean Letort, Ulziibat Munkhuu, Battulga Bakthuu, Tuguldur Ganbold, and Iag-dase Technical_team

Mongolian tectonics is shaped by the far-reaching effects of the Indo-Eurasian collision, which drives deformation and stress over 2000 km behind the Himalayan front. During the 20th century, Mongolia experienced four earthquakes with magnitudes greater than 8, making it an exceptional location for studying intraplate seismicity, predominantly with strike-slip components. Among these events, the Tsetserleg-Bulnay fault system recorded the largest intraplate earthquake doublet, with two magnitude 8 earthquakes occurring 14 days apart in 1905, rupturing more than 500 km of fault. The surface rupture, remarkably well-preserved due to the region's low erosion rate, has enabled extensive paleoseismic investigations. Despite this, the junction between the two faults remains unclear at the surface, and the fault structures at depth are still poorly constrained, leaving the interactions between fault segments not well understood.

In the present day, the significant microseismic activity affecting the Bulnay and Tsetserleg faults is anomalous given the low regional deformation rate and overall Mongolian seismicity. This persistent microseismicity could be interpreted as aftershocks that illuminate the faults’ structures more than a century after their mainshocks. By tracking this microseismicity with precision, we aim to map the faults’ 3D geometry at depth and address several questions including: how do these faults interact, why did the Bulnay earthquake occur only 14 days after the Tsetserleg earthquake, and why is its epicenter located 150km west of the junction zone?

In 2024, the French Atomic Energy Commission (CEA) and the Mongolian Institute of Astronomy and Geophysics (IAG) collaborated to strategically deploy a temporary seismic network, TDBnet, at the Bulnay-Tsetserleg junction. This network, comprising 10 geophones in addition to 5 broadband stations, operated altogether for five months, complementing the national network, and recorded local seismicity with unprecedented resolution. The collected data are being processed to automatically detect seismic phases using state-of-the-art methods, including the EQTransformer artificial neural network implemented in Seisbench. The detected events are then precisely located using an absolute location method, followed by an absolute relocation corrected with a Source Specific Station Time approach as proposed in the NonLinLoc-SSST framework. We present the experiment along with preliminary results, including a precisely determined earthquake epicenter map.

Acknowledgement  : We sincerely acknowledge the IAG-DASE technical team for their collaboration in the deployment of the temporary seismic network (TDBnet): Narmandakh Adyasuren4, Dorjdavaa Myagmar4, Youndonjunai Sodvoobavuu4, Nyamdorj Badarch4, Munkhbat Dagva4, Enkhtuvshin Begzsuren4, Purevsuren Dosmaa4, Leo Chazellet1,4, Serge Olivier1,4, Vincent Lisette1,4, Denis Lubin1,4.

How to cite: Bollinger, L., Manceau, L., Klinger, Y., Letort, J., Munkhuu, U., Bakthuu, B., Ganbold, T., and Technical_team, I.: Investigating the Tectonic Complexity of the Bulnay-Tsetserleg Fault Junction in Mongolia Using a Temporary Seismic Network, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-9148, https://doi.org/10.5194/egusphere-egu25-9148, 2025.

X2.15
|
EGU25-11845
|
ECS
|
Adélaïde Allemand, Yann Klinger, and Luc Scholtès

A strike-slip fault is subjected to earthquakes spanning seconds to minutes, separated by periods of hundreds to thousands of years. As the fault matures and undergoes multiple seismic events, its geometry and strength evolve, hence impacting in return the course of seismic cycles. Given the variability of timescales, two approaches are generally chosen in order to model the deformation of the lithosphere. On one hand, long-term modeling looks at the tectonic evolution of deformation, and is usually quasi-static and disregards the effects of dynamic events. On the other, short-term modeling respects well earthquake mechanics, but does not account for the impact of evolution of fault geometry on seismic cycles.

Here, we construct a numerical model of a continental strike-slip fault system, in a way that can effectively bridge together the different spatio-temporal scales of lithospheric deformation, and include the mutual influence of fault maturation and earthquakes upon one another. The developed approach uses the Discrete Element Modeling (DEM) method, which is based on the discretization of the medium in a finite number of rigid, spherical particles interacting via predefined contact laws. Using this method, we build a 3-D model of a portion of the crust. Initially, the material is homogeneous and intact. Then, shearing boundary conditions are applied, leading to the spontaneous emergence of a through-going, strike-slip fault showing complexities and evolving naturally as the shearing is maintained. On this evolving strike-slip fault, unstable sliding occurs, that we identify as earthquakes.

In order to validate our model, we first compare the long-term tectonic deformation with that of previous analog and numerical experiments described in the literature, and with natural observations. Second, we assess the physical validity of the recurrence behaviour of our created fault by comparing the frequence-magnitude distribution of our events with the Gutemberg-Richter law. Finally, we also provide tools able to characterize particular events by imaging the rupture geometry, the coseismic surface deformation as well as the coseismic displacement field on the fault.

How to cite: Allemand, A., Klinger, Y., and Scholtès, L.: A 3-D numerical model to bridge long- and short-term approaches of deformation on a strike-slip fault, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-11845, https://doi.org/10.5194/egusphere-egu25-11845, 2025.

X2.16
|
EGU25-13444
|
ECS
|
|
Margarita Solares-Colon, Diego Melgar, and Mary Grace Bato

We are interested in systematically analyzing large ruptures to establish scaling laws of kinematic properties, such as rise times, slip rates, and rupture speeds. The challenge is that kinematic models for large (M6+) events are often produced with heterogenous methodologies and datasets. This makes synthesis of general behaviors challenging and results ambiguous. Additionally, as methods continue to develop, past events with good observations do not necessarily have slip models produced with modern methods. Thus, retrospective analysis of slip distributions is fundamental to allow us to further investigate general characteristics of source parameters during a rupture. 

Here we will discuss our plans to retrospectively process significant ruptures with new inversion techniques that are capable of jointly inverting teleseimsic body and surface waves, static and high-rate GNSS, InSAR, strong motion and tsunami data. We will highlight the approach by focusing on the M9.1 Tohoku-oki earthquake to showcase the advantages of the new approach. This earthquake in 2011 stands as one of the largest ruptures ever recorded and most closely observed earthquake in history due to the dense array of seismic and geodetic instrumentation in Japan. This provided an unprecedented opportunity to study this megathrust event and collect data near source. 

This analysis extends beyond the great M9.1 Tohoku-oki earthquake, actively contributing to the ongoing reevaluation of finite-fault models for large earthquakes dating back to the 1990s, while also incorporating regional data when available. Ultimately, we aim to refine source scaling properties of large earthquakes worldwide. Therefore, we will present our proposed workflow that involves not only systematizing the inversion process but also the creation of standardized and analysis-ready input source products. This is particularly important for InSAR and GNSS, which are quickly expanding their temporal and spatial sampling of crustal deformation worldwide. 

How to cite: Solares-Colon, M., Melgar, D., and Bato, M. G.: Towards systematic kinematic source models of historically large earthquakes, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-13444, https://doi.org/10.5194/egusphere-egu25-13444, 2025.

X2.17
|
EGU25-13813
Unveiling the Surface Rupture of the 1946 Chatkal Earthquake (Mw 7.5, Tien Shan): Insights from Pleiades, UAV Imagery, and Trenching
(withdrawn)
Magali Rizza, Pousse Léa, and Fleury Jules
X2.18
|
EGU25-14410
|
ECS
Mason Perry, Lujia Feng, Emma Hill, and Gina Sarkawi

Following the 2004 Mw 9.2 Sumatra-Andaman event, a series of earthquakes occurred along the Sunda megathrust of the Sumatran subduction zone, extending from the southern terminus of the 2004 rupture to Bengkulu. A notable exception is the Mentawai seismic gap, spanning from just south of the Batu Islands to Sipora for ~200 km in length. Historical records of regional seismicity from paleogeodetic measurements (i.e. coral microatolls) indicate that the last major event that ruptured the current seismic gap occurred in 1797. An adjacent patch ruptured in 1833, broadly coincident with the 2007 Bengkulu rupture. More recent M≥7 events surrounding the Mentawai seismic gap have occurred in 2007, 2008, 2010, and 2023. However, slip distributions of these events show limited slip propagation into the gap and a significant slip deficit remains. Thus, a potential earthquake in the region poses a threat to local communities from both ground shaking, as well as a potential tsunami. Previous geodetic estimates of coupling in the region indicate low coupling at shallow depths on the megathrust. However, these estimates lack near-trench observations and ignore the influence of stress shadows originating from frictionally locked asperities downdip, and thus may underestimate the tsunami hazard, especially in light of the 2010 Mentawai tsunami earthquake that ruptured to the trench at depths of <6 km. Additionally, new estimates of long-term slip rates on the Sumatran Fault indicate the forearc sliver is deforming as rigid block and substantial oblique convergence is taken up within the oceanic plate. By correcting published geodetic velocities to remove the motion of the forearc sliver, we place updated constraints on subduction obliquity. Combining these observations with paleogeodetic uplift and subsidence rates, we invert for a coupling distribution on the Sunda megathrust, accounting for the effect of stress shadows, and constraining the coupling direction based on earthquake slip vectors. We find, in contrast to previous estimates, that the megathrust appears coupled to the trench. This coupled region extends from just north of Siberut south to the Pagai Islands and includes the region of the 2007 Bengkulu rupture. While the risk for large earthquakes in this region is relatively well known, our results indicate that the Mentawai seismic gap contains a strongly coupled patch that extends to the trench, suggesting that the tsunami hazard is significantly higher than inferred from previous coupling estimates. Additionally, this updated coupling model allows us to place new constraints on the influence of tectonics on regional sea level projections.

How to cite: Perry, M., Feng, L., Hill, E., and Sarkawi, G.: Updating megathrust coupling models for the Mentawai Seismic Gap and surrounding regions, Sumatra, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-14410, https://doi.org/10.5194/egusphere-egu25-14410, 2025.

X2.19
|
EGU25-14536
|
ECS
|
Mitchel Soederberg, Shreya Arora, Drew Cochran, and Gurvinder Singh

Earthquakes represent a significant hazard to human life, having claimed nearly a quarter of a million lives worldwide and strongly affecting an additional 125 million people between 1998 and 2017 (WHO). The Himalayan Front is an especially active continental collision zone spanning over 2500 kilometers across five countries, with its Himalayan Frontal Thrust (HFT) producing surface ruptures at the southern leading edge of the front (Kumar et al, 2001). Although recent earthquakes have produced surface ruptures along eastern and western sections of the HFT, paleoseismic and historical investigations have not revealed any surface rupture-forming earthquakes in the central Himalayas since at least the 17th century (Arora and Malik, 2017). This gap raises the potential for a mega-earthquake (> Mw 8) in coming years (Wesnousky, 2020). Here, we share preliminary results from a paleoseismic investigation of an exposed river section on the central HFT adjacent to Shahjahanpur village, 20 km southwest of Dehradun, Uttarakhand, India (30° 12 '04.6"N, 77° 49' 39.6"E). Optically stimulated luminescence (OSL) bulk sediment dates in combination with river section interpretations will aid in evaluating the presence of surface ruptures related to a major 1505 earthquake event in this area, for which numerous historical accounts exist (Jackson, 2002). Implications of these results include an improved estimation of this event’s western lateral extent in conjunction with previous studies. This will allow for the calculation of a more accurate paleo magnitude for the 1505 earthquake, ultimately informing the region’s seismic hazard potential.

How to cite: Soederberg, M., Arora, S., Cochran, D., and Singh, G.: Determining the Western Extent of the 1505 Central Himalayan Earthquake through a Paleoseismic Investigation of Surface Ruptures, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-14536, https://doi.org/10.5194/egusphere-egu25-14536, 2025.

X2.20
|
EGU25-16771
|
ECS
I-Ting Wang, Kuo-En Ching, and Erwan Pathier

Under the assumption that the plate convergence rate is distributed across faults along the plate boundary, in the Chungliao Tunnel area of southwest Taiwan, the total surface velocity change between the Chegualin fault (CGLF) to the west and the Chishan fault (CSNF) to the east exceeds 90 mm/yr, which is larger than the palte convergence rate of approximately 82 mm/yr in Taiwan. However, the physical processes driving these high-rate deformation is still debated. As the deformation is mainly aseismic, and to increase the spatial resolution of the large-scale surface deformation field, we used GNSS and ALOS-2 InSAR to understand tectonic processes. To examine the spatial continuity of the ultra-rapid deformation beyond the Chungliao Tunnel, InSAR processing was conducted using ALOS-2 ascending and descending datasets to improve the spatial extension and resolution of surface deformation. We introduced a priori phase discontinuity at mapped fault trace by setting the temporal coherence to correct the unwrapping errors. Then several Line-Of-Sight (LOS) velocity discontinuities are consistent with fault traces, indicating shallow creep along those faults. Furthermore, we demonstrated the continuity of few-hundred meters of high deformation between the CGLF and the CSNF with LOS velocity of 30-40 mm/yr, a LOS velocity gradient of 20-30 mm/yr across two faults. A 3D velocity reconstruction inverted by combining GNSS and ALOS-2 InSAR result reveals a local counter-clockwise rotation from NW to SW align north to south and the significant uplift (~80 mm/yr) in the narrow band between the Chishan fault and Chegualin fault near the Chungliao Tunnel. The local deformation implies the opposite lateral components of CSNF and CGLF in different segments of two faults as well, providing precise constraints to enhance the tectonic interpretation of this area. This rapid deformation identified in the narrow zone may be resulting from the interaction between the thrust faults and the surrounding mobile shale, in agreement with the hypothesis of a mud diapir of large mud diatreme that developed in the thick two thrusts.

How to cite: Wang, I.-T., Ching, K.-E., and Pathier, E.: Revisiting Rapid Surface Deformation in Southwestern Taiwan Using GNSS and ALOS-2 InSAR Data: Case study in Chungliao Tunnel, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-16771, https://doi.org/10.5194/egusphere-egu25-16771, 2025.

X2.21
|
EGU25-17648
|
ECS
Ayşegül Doğan and Ulaş Avşar

Lacustrine paleoseismology, which focuses on sedimentary traces of past earthquakes in lakes, has gained increasing attention over the past two decades, even though on-fault trenching remains the most common technique in paleoseismology. This field primarily investigates Mass Wasting Deposits (MWD) and Soft Sediment Deformation Structures (SSDS) in lake sediments. Additionally, catchment response (CR), characterized by a temporary increase in erosion rates within catchments due to strong ground motions, is another significant trace of past earthquakes in lake sediments. In this study, past earthquake traces were analyzed in 19 gravity cores (98.880-138.70 cm in length) retrieved from the varved sediments of Köyceğiz Lake. High-resolution elemental profiles and optical images were obtained using ITRAX micro-XRF core scanner. ITRAX optical and XRF data along one core was used to generate varve chronology, and Ca/Ti profiles of the other cores were used to chronostratigraphically correlate 19 cores. Although the region experienced several notable earthquakes over the past 600 years, no MWDs were identified in Köyceğiz sediments; instead, SSDS and CR were observed. Distinct anomalies in Cr/Ti profiles related to the 1959 earthquake were evident in all cores. Conversely, CR associated with a mid-19th-century earthquake was detected only in the northern basin, which has significantly larger catchment than the southern basin. SSDS, including faults, intraclast breccias and laminae disturbances were identified in Köyceğiz sediments. While some of these SSDS correlate temporally with historical earthquakes, most do not correlate either with seismic events or with each other. This implies that, contrary to what has been thought so far, SSDS formation may not be limited to the water-sediment interface but could also occur in deeper parts of the sequence. Moreover, the study indicates that the formation of SSDS may be controlled not only by peak ground acceleration (PGA) but also by peak ground displacement (PGD) due to earthquakes.

How to cite: Doğan, A. and Avşar, U.: Sedimentary records of past earthquakes in varved lake sediments, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-17648, https://doi.org/10.5194/egusphere-egu25-17648, 2025.

X2.22
|
EGU25-17661
|
ECS
Kai-Feng Chen, Maryline Le Béon, Arthur Delorme, Yann Klinger, Ewelina Rupnik, Lulin Zhang, Erwan Pathier, Kuo-En Ching, and Marc Pierrot-Deseilligny

In southwestern Taiwan, about 45-50 mm/yr of westward shortening occurs across the 40-45 km wide fold-and-thrust belt, accompanied with tectonic extrusion towards the southwest. Within this broad framework, measurements from a local ground-based geodetic network revealed rapid ground deformation surrounding two sub-parallel geological thrust faults, located only 500 m apart. 50 mm/yr of shortening occurs on the western fault and 32 mm/yr of extension across the eastern one. In-between the faults, uplift relative to the east block increases eastward from 20 to 80 mm/yr. Sharp deformation gradients indicate aseismic slip on both structures. This remarkable deformation raises the question of the deep structure and mechanism at play: Is it driven by tectonic forces, possibly released as transient slip events? Or does it involve shale tectonics related to fluid overpressure within the mudstone formation that dominates the geology?

To investigate this phenomenon, we monitored ground deformation using image correlation for horizontal displacements and DSM time series for vertical displacements, aiming at high-resolution observations covering a wider area than the ground-based network. Eight sets of aerial images acquired from 2008 to 2015 were processed using the MicMac photogrammetric software. The resulting horizontal velocities are in good agreement with ground-based observations. The compressional gradient across the western fault (the Chegualin Fault) vanishes northward, but remains clearly visible towards the south, with an increasing right-lateral component. While we detect extension across the eastern fault (the Chishan Fault), precise location and quantification of the deformation gradient remains challenging due to poor correlation caused by dense vegetation. Elevation differences based on the DSMs derived from aerial images have a similar spatial pattern as ground-based observations, but the amplitudes are overestimated. On-going refinement in the processing and time series based on LiDAR datasets are expected to improve the results.

This work was complemented by the field survey of the numerous bedrock shear zones in the area to build a structural map of active structures. We confirm the Chegualin Fault as an active thrust fault, with an oblique component along its southern part. Extension across the Chishan Thrust is accommodated by SE-dipping en-echelon normal faults, found up to 1.4 km north of the ground-based network. The change in rake of the slickenlines indicates an increasing right-lateral component northward. While the pattern of horizontal velocities may fit with the regional tectonics, the hypothesis of a shale piercement so far best explains the ratio between uplift and shortening. Achieving a better imaging of the vertical deformation would help further discussing this assumption and eventually propose a structural model consistent with local and regional observations, which will also allow further assessing the associated natural hazards.

How to cite: Chen, K.-F., Le Béon, M., Delorme, A., Klinger, Y., Rupnik, E., Zhang, L., Pathier, E., Ching, K.-E., and Pierrot-Deseilligny, M.: Measuring rapid aseismic ground deformation within the foothills of southwestern Taiwan using aerial image correlation and DSM time series, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-17661, https://doi.org/10.5194/egusphere-egu25-17661, 2025.

X2.23
|
EGU25-19066
Yann Klinger, Nicolas Pinzon Matapi, Pierre Sabatier, Edward Duarte, Jin-Hyuck Choi, Taehyung Kim, and Baatara Ga

On July 1905, two M~8 earthquakes occurred 14 days apart along the Bulnay Fault system, in northwestern Mongolia. These seismic events are among the largest recorded earthquakes in intracontinental regions. However, our current understanding of the earthquake behavior of the Bulnay Fault is quite limited due to the scarcity of paleoseismic data. Additionally, the geographic and climatic conditions of the region play a major key in permafrost development, posing challenges in the excavation of paleoseismological trenches and causing cryoturbation. Lacustrine environments, conversely, are isolated depositional systems that minimize the influence of external factors and provide high temporal resolution with continuous sedimentation. Here, we present our findings on earthquake-triggered turbidites of eight sedimentary cores collected from three lakes around the Bulnay Fault. These cores were analyzed using X-ray tomography, X-ray fluorescence, and hyperspectral imaging. We found that prior to the 1905 event, three large earthquakes ruptured the Bulnay Fault, with recurrence intervals of 1.5 to 3 kyr. By integrating our observations with previous paleoseismic trench investigations, we proposed that strain is primarily accommodated through large earthquakes along the Bulnay fault, and major events involving both the Bulnay and Tsetserleg faults, potentially analogous to the 1905 doublet.

How to cite: Klinger, Y., Pinzon Matapi, N., Sabatier, P., Duarte, E., Choi, J.-H., Kim, T., and Ga, B.: Potential record of large earthquakes from lacustrine sedimentary archives along the Bulnay fault system (Mongolia), EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-19066, https://doi.org/10.5194/egusphere-egu25-19066, 2025.

X2.24
|
EGU25-11133
|
ECS
|
Yiqing Liu, Yan Hu, and Xin Cui

In Southwest Japan, interseismic deformation exhibits distinct patterns, particularly across Kyushu Island, where its magnitude decreases significantly from north to south. Various mechanisms, including plate motions, fault slip on onshore fault systems, dilatational sources, and variable interplate coupling along the Nankai and Ryukyu subduction zones, have been proposed to explain these features. While previous studies have effectively modeled horizontal deformation and attributed the rotational pattern in southern Kyushu primarily to plate motion, they often neglect or inconsistently predict vertical deformation, underscoring the need for further investigation.

In this study, we employ a three-dimensional (3D) viscoelastic finite element model (FEM) to analyze interseismic deformation in Southwest Japan, spanning the transition from the Nankai to the Ryukyu subduction zone. To focus on megathrust coupling, we exclude block motion and consider other factors as secondary influences. Our goal is to reconcile horizontal and vertical geodetic observations and provide a first-order estimate of megathrust coupling in this margin through a viscoelastic model, offering a direct comparison with previously published elastic models.

How to cite: Liu, Y., Hu, Y., and Cui, X.: Megathrust Coupling in Southwest Japan Inferred from Viscoelastic Modeling, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-11133, https://doi.org/10.5194/egusphere-egu25-11133, 2025.

X2.25
|
EGU25-9782
Fabio Corbi, Adriano Gualandi, Giacomo Mastella, and Francesca Funiciello

We investigate the complexity of two types of scaled seismotectonic models mimicking subduction megathrust seismic cycles. Our research encompasses a variety of model sizes, materials, deformation rates, and frictional configurations. Using nonlinear time-series analysis tools and displacement as an input variable, we characterize the dynamics of laboratory earthquakes in different phases of the labquake cycle. The number of active degrees of freedom that we are able to retrieve is low (<5) during most of the cycle, akin to slow slip episodes observed in natural settings and friction experiments performed with quartz powder. Results seem insensitive to the along-strike frictional segmentation of the megathrust. Nonetheless, the instantaneous dimension d can reach large values (>10), revealing the complexity of the system. High values of d correlate with slip phases, while significant drops in the extremal index anticipate slip episodes. Our results suggest that prediction horizons are in the order of a fraction of slip duration similarly to prediction horizons inferred for slow slip events in nature. This research not only enhances our understanding of earthquake dynamics, but also validates scaled seismotectonic models as effective tools for studying frictional physics across diverse spatio-temporal scales.



How to cite: Corbi, F., Gualandi, A., Mastella, G., and Funiciello, F.: Complexity of scaled seismotectonic models, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-9782, https://doi.org/10.5194/egusphere-egu25-9782, 2025.