Pub Date : 2026-01-06DOI: 10.1016/j.tecto.2025.231061
J.V. Rama Rao , Ravi Kumar Bandi , T.R.K. Chetty
The East Indian Subcontinent (EISC) is a geologically complex region recording tectonic evolution from the Proterozoic era to the present. This study integrates terrestrial, marine, and satellite gravity data across ∼5 million sq. km covering eastern India, Bangladesh, the Bay of Bengal, and Myanmar, along with earthquake incidences from the past 120 years to unravel the tectonic framework of the region.
A Key focus of this study is building the interrelations among major Proterozoic orogenic belts—Central Indian Tectonic Zone (CITZ), Eastern Ghats Mobile Belt (EGMB), Chhotanagpur Granite Gneissic Complex (CGGC), and Shillong Meghalaya Gneissic Complex (SMGC). From this study, we propose a possible eastern boundary of the CITZ marked as Lucknow–Varanasi–Ranchi lineament, highlight the remarkable affinities between eastern CGGC and EGMB, and redefine the Eastern Continental Margin of India.
Gravity analysis delineates the disposition of collision zones of EISC besides inferring five tectonic domains of EISC, crustal boundaries, plate margins, and transitions from continental to oceanic crust. It also reveals heterogeneity over submarine ridges and the segmentation of the India–Myanmar subduction zone. Aseismic central segment, bounded by cross-faults, is an explicit inference of our study about current Indo-Australian plate subduction dynamics beneath the Sunda–Myanmar Plate.
{"title":"Tectonics of East Indian Subcontinent: As derived from Integrated Gravity Anomalies of India, Bangladesh, Bay of Bengal and Myanmar Regions","authors":"J.V. Rama Rao , Ravi Kumar Bandi , T.R.K. Chetty","doi":"10.1016/j.tecto.2025.231061","DOIUrl":"10.1016/j.tecto.2025.231061","url":null,"abstract":"<div><div>The East Indian Subcontinent (EISC) is a geologically complex region recording tectonic evolution from the Proterozoic era to the present. This study integrates terrestrial, marine, and satellite gravity data across ∼5 million sq. km covering eastern India, Bangladesh, the Bay of Bengal, and Myanmar, along with earthquake incidences from the past 120 years to unravel the tectonic framework of the region.</div><div>A Key focus of this study is building the interrelations among major Proterozoic orogenic belts—Central Indian Tectonic Zone (CITZ), Eastern Ghats Mobile Belt (EGMB), Chhotanagpur Granite Gneissic Complex (CGGC), and Shillong Meghalaya Gneissic Complex (SMGC). From this study, we propose a possible eastern boundary of the CITZ marked as Lucknow–Varanasi–Ranchi lineament, highlight the remarkable affinities between eastern CGGC and EGMB, and redefine the Eastern Continental Margin of India.</div><div>Gravity analysis delineates the disposition of collision zones of EISC besides inferring five tectonic domains of EISC, crustal boundaries, plate margins, and transitions from continental to oceanic crust. It also reveals heterogeneity over submarine ridges and the segmentation of the India–Myanmar subduction zone. Aseismic central segment, bounded by cross-faults, is an explicit inference of our study about current Indo-Australian plate subduction dynamics beneath the Sunda–Myanmar Plate.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"923 ","pages":"Article 231061"},"PeriodicalIF":2.6,"publicationDate":"2026-01-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145915294","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-01-06DOI: 10.1016/j.tecto.2026.231070
Nicolás Alejandro Peluffo , Lucas Martín Fennell , Sarah Ellen Thomas , Federico Exequiel Martos , Victor Valencia , Andrés Folguera , Maximiliano Naipauer
This work presents an update of the evolution of the La Ramada fold-thrust belt (∼32°S-32°30′S), located in a remote area of the Principal Cordillera of Argentina, integrating two measured stratigraphic sections, novel field observations, and three new zircon UPb ages: two detrital and one igneous. Our new stratigraphic framework includes Paleocene to Miocene sedimentary and volcanic rocks, a period previously interpreted as a hiatus in the area. This sheds light on an enigmatic stage in the evolution of the Andes at these latitudes. We describe the Teatinos Formation, a sedimentary unit with a maximum depositional age of 11.2 ± 0.2 Ma at its base. These rocks were deposited in the Teatinos Basin, a newly defined piggyback basin developed within the Principal Cordillera, representing the innermost expression of the Miocene Andean foreland basin system at these latitudes. A new UPb crystallization age of 19.1 ± 0.5 Ma, obtained from a sill intruding ∼900 m of volcanic rocks, confirms the presence of the late Eocene - early Miocene Abanico Formation in an anomalous position, up to 5 km east of the eastern boundary of the Abanico Basin. This boundary is represented in our area by the Major Andean Fault, a first-order structure that juxtaposes rocks of the western Principal Cordillera over the Teatinos Formation. We also present a new maximum depositional age of 145.2 ± 1.5 Ma from sedimentary rocks in the hanging wall of this fault. These are overlain by the Abanico Formation, defining a > 100 Myr hiatus compatible with the existence of a pre-Oligocene contractional event. We propose a polyphasic evolution for the La Ramada fold-thrust belt involving at least three contractional pulses: one pre-Oligocene and two during the Miocene (ca. 22–18 Ma and ca. 12–9 Ma).
{"title":"Polyphasic deformation during the evolution of the southern Central Andes: Insights from the La Ramada fold-thrust belt (32°-32°30′S)","authors":"Nicolás Alejandro Peluffo , Lucas Martín Fennell , Sarah Ellen Thomas , Federico Exequiel Martos , Victor Valencia , Andrés Folguera , Maximiliano Naipauer","doi":"10.1016/j.tecto.2026.231070","DOIUrl":"10.1016/j.tecto.2026.231070","url":null,"abstract":"<div><div>This work presents an update of the evolution of the La Ramada fold-thrust belt (∼32°S-32°30′S), located in a remote area of the Principal Cordillera of Argentina, integrating two measured stratigraphic sections, novel field observations, and three new zircon U<img>Pb ages: two detrital and one igneous. Our new stratigraphic framework includes Paleocene to Miocene sedimentary and volcanic rocks, a period previously interpreted as a hiatus in the area. This sheds light on an enigmatic stage in the evolution of the Andes at these latitudes. We describe the Teatinos Formation, a sedimentary unit with a maximum depositional age of 11.2 ± 0.2 Ma at its base. These rocks were deposited in the Teatinos Basin, a newly defined piggyback basin developed within the Principal Cordillera, representing the innermost expression of the Miocene Andean foreland basin system at these latitudes. A new U<img>Pb crystallization age of 19.1 ± 0.5 Ma, obtained from a sill intruding ∼900 m of volcanic rocks, confirms the presence of the late Eocene - early Miocene Abanico Formation in an anomalous position, up to 5 km east of the eastern boundary of the Abanico Basin. This boundary is represented in our area by the Major Andean Fault, a first-order structure that juxtaposes rocks of the western Principal Cordillera over the Teatinos Formation. We also present a new maximum depositional age of 145.2 ± 1.5 Ma from sedimentary rocks in the hanging wall of this fault. These are overlain by the Abanico Formation, defining a > 100 Myr hiatus compatible with the existence of a pre-Oligocene contractional event. We propose a polyphasic evolution for the La Ramada fold-thrust belt involving at least three contractional pulses: one pre-Oligocene and two during the Miocene (ca. 22–18 Ma and ca. 12–9 Ma).</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"923 ","pages":"Article 231070"},"PeriodicalIF":2.6,"publicationDate":"2026-01-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145956975","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-01-05DOI: 10.1016/j.tecto.2026.231071
Longfei Han , Wenqian Yao , Jing Liu-Zeng , Yann Klinger , Chengguo Yan , Peng Wang , Yanxiu Shao
Accurate measurements of coseismic slip distributions derived from geomorphic markers provide essential insights into earthquake rupture dynamics and make a significant contribution to seismic hazard evaluation. With the increased availability of high-resolution topographic data and advanced statistical techniques such as cumulative offset probability distribution (COPD), reconstructing single-event coseismic displacement from cumulative offsets of successive paleoearthquakes has become more feasible. However, assessing the reliability of these methods remains critical. The 1920 Mw7.9 Haiyuan earthquake, the most recent major event along the strike-slip Haiyuan fault, serves as an ideal case study due to notable discrepancies in previously reported displacement measurements. In this study, we utilize very high-resolution (0.1 m) topographic data derived from aerial imagery processed via the Structure from Motion (SfM) technique, covering approximately 85 km of the ∼240 km rupture length. Our analysis, based on detailed horizontal slip measurements and COPD calculation, yields a maximum displacement of 7.6 ± 0.8 m for the 1920 Haiyuan earthquake, differing from previous estimates but aligning well with global scaling relationships for strike-slip earthquakes. Our results reveal three COPD peaks in the geomorphic records along the Haiyuan fault. The displacement interval between the two most recent peaks is similar to that of the latest peak, with reduced displacement observed in the western section. These findings suggest that previous interpretations of four to five events may significantly overestimate single-event slip. Comparisons with previous studies underscore the methodological challenges in COPD-based reconstructions, including uncertainties from different slip measurement methods, geomorphic marker interpretations, fault geometry, along-strike slip variability, and the contribution of moderate-magnitude earthquakes to cumulative offsets.
{"title":"Reevaluation of geomorphic offsets along the 1920 Haiyuan earthquake rupture, China: A discussion of uncertainties in slip measurements and COPD analyses using high-resolution topography","authors":"Longfei Han , Wenqian Yao , Jing Liu-Zeng , Yann Klinger , Chengguo Yan , Peng Wang , Yanxiu Shao","doi":"10.1016/j.tecto.2026.231071","DOIUrl":"10.1016/j.tecto.2026.231071","url":null,"abstract":"<div><div>Accurate measurements of coseismic slip distributions derived from geomorphic markers provide essential insights into earthquake rupture dynamics and make a significant contribution to seismic hazard evaluation. With the increased availability of high-resolution topographic data and advanced statistical techniques such as cumulative offset probability distribution (COPD), reconstructing single-event coseismic displacement from cumulative offsets of successive paleoearthquakes has become more feasible. However, assessing the reliability of these methods remains critical. The 1920 <em>M</em>w7.9 Haiyuan earthquake, the most recent major event along the strike-slip Haiyuan fault, serves as an ideal case study due to notable discrepancies in previously reported displacement measurements. In this study, we utilize very high-resolution (0.1 m) topographic data derived from aerial imagery processed via the Structure from Motion (SfM) technique, covering approximately 85 km of the ∼240 km rupture length. Our analysis, based on detailed horizontal slip measurements and COPD calculation, yields a maximum displacement of 7.6 ± 0.8 m for the 1920 Haiyuan earthquake, differing from previous estimates but aligning well with global scaling relationships for strike-slip earthquakes. Our results reveal three COPD peaks in the geomorphic records along the Haiyuan fault. The displacement interval between the two most recent peaks is similar to that of the latest peak, with reduced displacement observed in the western section. These findings suggest that previous interpretations of four to five events may significantly overestimate single-event slip. Comparisons with previous studies underscore the methodological challenges in COPD-based reconstructions, including uncertainties from different slip measurement methods, geomorphic marker interpretations, fault geometry, along-strike slip variability, and the contribution of moderate-magnitude earthquakes to cumulative offsets.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"922 ","pages":"Article 231071"},"PeriodicalIF":2.6,"publicationDate":"2026-01-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145902931","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-01-03DOI: 10.1016/j.tecto.2025.231067
Muhammad Qasim , Owais Tayyab , Lin Ding , Javed Iqbal Tanoli , Muhammad Awais , Kamran Tabassum , Fulong Cai , Zhang Dingding , Ishtiaq A.K. Jadoon
The India-Asia collision along the western Indian Plate margin remains debated, with contrasting models for the first arrival of Asian-derived detritus in the region. The Sulaiman Fold–Thrust Belt (SFB) in southwestern Pakistan preserves a crucial record of this transition, with the Paleocene to Eocene stratigraphic succession providing insights into sediment provenance shifts. To constrain the collision timing, we analyzed detrital zircon for U-Pb-Hf geochronology, supplemented by petrography and zircon Th/U geochemistry, from Cenozoic sequences exposed in the Mughalkot section, SFB. Detrital zircon age distributions from the Paleocene Dunghan Formation are dominated by ∼500–1100 Ma, ∼1400–2000 Ma, and ∼ 2400–2600 Ma grains, indicating a primary sediment source from the Indian Plate. A similar detrital zircon age pattern in the early to middle Eocene Ghazij Formation suggests continued derivation from the Indian craton. However, a pronounced provenance shift is observed in the lowermost Baska Formation (middle Eocene), marked by the arrival of Late Cretaceous–Paleocene (<100 Ma) detrital zircons, which possess Th/U ratios (>0.3) indicative of an igneous origin. Juvenile Hf signatures of the younger detrital zircons further support their derivation from the Kohistan-Ladakh Arc, which is located between the Indian and the Asian plates in North Pakistan. The arrival of this detritus signals the onset of the India-Asia collision, constrained by the maximum depositional age to post–51 Ma. When compared to northern and central segments of the Himalayan orogen, this suggests a diachronous collision with its later onset in the westernmost region. These findings contribute to the broader framework of India-Asia convergence, supporting models that invoke regional variability in collision timing and foreland basin evolution.
{"title":"Timing of India-Asia diachronous collision: A view from the westernmost Indian margin, Pakistan","authors":"Muhammad Qasim , Owais Tayyab , Lin Ding , Javed Iqbal Tanoli , Muhammad Awais , Kamran Tabassum , Fulong Cai , Zhang Dingding , Ishtiaq A.K. Jadoon","doi":"10.1016/j.tecto.2025.231067","DOIUrl":"10.1016/j.tecto.2025.231067","url":null,"abstract":"<div><div>The India-Asia collision along the western Indian Plate margin remains debated, with contrasting models for the first arrival of Asian-derived detritus in the region. The Sulaiman Fold–Thrust Belt (SFB) in southwestern Pakistan preserves a crucial record of this transition, with the Paleocene to Eocene stratigraphic succession providing insights into sediment provenance shifts. To constrain the collision timing, we analyzed detrital zircon for U-Pb-Hf geochronology, supplemented by petrography and zircon Th/U geochemistry, from Cenozoic sequences exposed in the Mughalkot section, SFB. Detrital zircon age distributions from the Paleocene Dunghan Formation are dominated by ∼500–1100 Ma, ∼1400–2000 Ma, and ∼ 2400–2600 Ma grains, indicating a primary sediment source from the Indian Plate. A similar detrital zircon age pattern in the early to middle Eocene Ghazij Formation suggests continued derivation from the Indian craton. However, a pronounced provenance shift is observed in the lowermost Baska Formation (middle Eocene), marked by the arrival of Late Cretaceous–Paleocene (<100 Ma) detrital zircons, which possess Th/U ratios (>0.3) indicative of an igneous origin. Juvenile Hf signatures of the younger detrital zircons further support their derivation from the Kohistan-Ladakh Arc, which is located between the Indian and the Asian plates in North Pakistan. The arrival of this detritus signals the onset of the India-Asia collision, constrained by the maximum depositional age to post–51 Ma. When compared to northern and central segments of the Himalayan orogen, this suggests a diachronous collision with its later onset in the westernmost region. These findings contribute to the broader framework of India-Asia convergence, supporting models that invoke regional variability in collision timing and foreland basin evolution.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"922 ","pages":"Article 231067"},"PeriodicalIF":2.6,"publicationDate":"2026-01-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145894830","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-01-03DOI: 10.1016/j.tecto.2026.231068
Weini Zhang , Wengao Zhang , Fengbin Han , Jian Chang , Hailong Huo , Jiayong Pan , Bakhtiar Nurtaev , Shukhrat Shukurov , Zhengle Cheng
The western Tian Shan in Uzbekistan, forming the orogen's western terminus, provides critical insights into Meso-Cenozoic tectonic evolution through its uplift-exhumation history. This study integrates apatite/zircon fission-track (AFT/ZFT) and zircon (UTh)/He analyses on 15 granitic samples from the Kyzylkum Nurata segment. Key findings include: (1) AFT ages span 67.50 ± 10.03–215.31 ± 14.53 Ma, with short mean track lengths (11.47 ± 1.38–12.65 ± 0.75 μm), indicating partial thermal resetting.(2)The western Tian Shan experienced Meso-Cenozoic multi-phase rapid uplift-exhumation, revealing a progressive northwest-to-southeast younging of apatite fission track ages and a marked contrast in exhumation regimes between the northwestern Nurata Range and adjacent ranges within the Kyzylkum-Nurata segment, highlighting spatiotemporal migration of tectonic activity and localized deformation partitioning. (3) Three thermo-tectonic phases were identified: Triassic rapid exhumation responding to Turan-Qiangtang/Paleo-Asia collision; Jurassic-Early Cretaceous uplift controlled by Lhasa-Qiangtang collision effects; Late Cretaceous-Cenozoic burial-rejuvenation cycles linked to Kohistan-Dras arc accretion in the Late Cretaceous and India-Eurasia/Kunlun-Pamir collisions in the Cenozoic. Differential exhumation patterns reflect inherited crustal heterogeneity, suture zone reactivation, and far-field stresses from Tethyan plate interactions. This study fills critical gaps in understanding Meso-Cenozoic uplift-exhumation processes in the westernmost Tian Shan, providing enhanced constraining models for the tectonic evolution of the entire orogen. Based on the investigation into the dynamic origins of uplift and exhumation, it can be concluded that the trend of uplift and exhumation in the Kyzylkum-Nurata segment of the Western Tian Shan propagated from southeast to northwest.
{"title":"Mesozoic differential uplift-exhumation processes in the western Tian Shan, Uzbekistan: Constraints from apatite/zircon fission track and (UTh)/He thermochronology","authors":"Weini Zhang , Wengao Zhang , Fengbin Han , Jian Chang , Hailong Huo , Jiayong Pan , Bakhtiar Nurtaev , Shukhrat Shukurov , Zhengle Cheng","doi":"10.1016/j.tecto.2026.231068","DOIUrl":"10.1016/j.tecto.2026.231068","url":null,"abstract":"<div><div>The western Tian Shan in Uzbekistan, forming the orogen's western terminus, provides critical insights into Meso-Cenozoic tectonic evolution through its uplift-exhumation history. This study integrates apatite/zircon fission-track (AFT/ZFT) and zircon (U<img>Th)/He analyses on 15 granitic samples from the Kyzylkum Nurata segment. Key findings include: (1) AFT ages span 67.50 ± 10.03–215.31 ± 14.53 Ma, with short mean track lengths (11.47 ± 1.38–12.65 ± 0.75 μm), indicating partial thermal resetting.(2)The western Tian Shan experienced Meso-Cenozoic multi-phase rapid uplift-exhumation, revealing a progressive northwest-to-southeast younging of apatite fission track ages and a marked contrast in exhumation regimes between the northwestern Nurata Range and adjacent ranges within the Kyzylkum-Nurata segment, highlighting spatiotemporal migration of tectonic activity and localized deformation partitioning. (3) Three thermo-tectonic phases were identified: Triassic rapid exhumation responding to Turan-Qiangtang/Paleo-Asia collision; Jurassic-Early Cretaceous uplift controlled by Lhasa-Qiangtang collision effects; Late Cretaceous-Cenozoic burial-rejuvenation cycles linked to Kohistan-Dras arc accretion in the Late Cretaceous and India-Eurasia/Kunlun-Pamir collisions in the Cenozoic. Differential exhumation patterns reflect inherited crustal heterogeneity, suture zone reactivation, and far-field stresses from Tethyan plate interactions. This study fills critical gaps in understanding Meso-Cenozoic uplift-exhumation processes in the westernmost Tian Shan, providing enhanced constraining models for the tectonic evolution of the entire orogen. Based on the investigation into the dynamic origins of uplift and exhumation, it can be concluded that the trend of uplift and exhumation in the Kyzylkum-Nurata segment of the Western Tian Shan propagated from southeast to northwest.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"922 ","pages":"Article 231068"},"PeriodicalIF":2.6,"publicationDate":"2026-01-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145894828","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-01-02DOI: 10.1016/j.tecto.2025.231065
Busheng Xie , Lixin Wu , Licheng Sun , Youyou Xu , Akimasa Yoshikawa , Wenfei Mao
This study investigates multi-type pre-seismic geomagnetic anomalies observed before the August 15, 2007, Mw 8.0 Pisco earthquake, and proposes Pressure-Stimulated Rock Current (PSRC) as an underlying mechanism. Using time-domain and frequency-domain analyses, the research identifies ultra-low frequency (ULF) emissions and magnetic vector deflections related to the earthquake. Based on the diurnal variation anomalies across multiple stations, a novel algorithm, the Forward Intersection of Magnetic Disturbance Vector (FIMDV), was developed to estimate the location of the seismogenic zone by analyzing the magnetic vector deflection. The FIMDV algorithm integrates the magnitude and directional information of magnetic disturbance vectors to pinpoint rock currents, providing new insights into geomagnetic anomalies and earthquake preparation. The study identifies two key phases of potential PSRC generation: the crack coalescence phase, associated with ULF emissions detected a month before the earthquake, and the crack interconnection phase, which corresponds to diurnal anomalies observed on the earthquake day. The former involves microcrack formation and positive hole activation, leading to varying electromagnetic fields that propagate as low-frequency waves detectable at the ground surface. The latter involves cracks interconnection facilitating the propagation of direct rock currents to the ground surface and inducing stable magnetic disturbance vectors. Geological validation confirmed that the local lithology, rich in silicate minerals, enables positive holes activation and propagation, further supporting PSRC as a driving mechanism of the observed multi-mode geomagnetic anomalies, including diurnal variation, vector deflection, Z/H polarization ratio, and horizontal polarization ellipse.
{"title":"Multi-mode pre-seismic geomagnetic anomalies reveal potential mechanisms of the August 15, 2007, Mw8.0 Pisco earthquake: Pressure-stimulated rock current","authors":"Busheng Xie , Lixin Wu , Licheng Sun , Youyou Xu , Akimasa Yoshikawa , Wenfei Mao","doi":"10.1016/j.tecto.2025.231065","DOIUrl":"10.1016/j.tecto.2025.231065","url":null,"abstract":"<div><div>This study investigates multi-type pre-seismic geomagnetic anomalies observed before the August 15, 2007, M<sub>w</sub> 8.0 Pisco earthquake, and proposes Pressure-Stimulated Rock Current (PSRC) as an underlying mechanism. Using time-domain and frequency-domain analyses, the research identifies ultra-low frequency (ULF) emissions and magnetic vector deflections related to the earthquake. Based on the diurnal variation anomalies across multiple stations, a novel algorithm, the Forward Intersection of Magnetic Disturbance Vector (FIMDV), was developed to estimate the location of the seismogenic zone by analyzing the magnetic vector deflection. The FIMDV algorithm integrates the magnitude and directional information of magnetic disturbance vectors to pinpoint rock currents, providing new insights into geomagnetic anomalies and earthquake preparation. The study identifies two key phases of potential PSRC generation: the crack coalescence phase, associated with ULF emissions detected a month before the earthquake, and the crack interconnection phase, which corresponds to diurnal anomalies observed on the earthquake day. The former involves microcrack formation and positive hole activation, leading to varying electromagnetic fields that propagate as low-frequency waves detectable at the ground surface. The latter involves cracks interconnection facilitating the propagation of direct rock currents to the ground surface and inducing stable magnetic disturbance vectors. Geological validation confirmed that the local lithology, rich in silicate minerals, enables positive holes activation and propagation, further supporting PSRC as a driving mechanism of the observed multi-mode geomagnetic anomalies, including diurnal variation, vector deflection, Z/H polarization ratio, and horizontal polarization ellipse.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"922 ","pages":"Article 231065"},"PeriodicalIF":2.6,"publicationDate":"2026-01-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145894841","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-01-02DOI: 10.1016/j.tecto.2025.231062
Junpeng Wang , Agathe Eijsink , Matthew Roseboom , Chris Marone , Jacques Riviere , Parisa Shokouhi , Derek Elsworth
Induced seismicity is the main uncertainty to safely produce geothermal energy, raising questions as to how applicable known physical laws are at increased temperatures. We explore the impact of elevated temperatures on maximum seismic moments anticipated in induced seismicity. We conduct laboratory reactivation experiments on a single inclined fracture (SIF) at equilibrated temperatures of 23 °C, 78 °C and 137 °C. Fractures are loaded at a constant shear stress of ∼80 % of the peak shear strength with slip activated by fluid injection. Reactivated seismic moments scale linearly with volume injected but decrease by one-order-of-magnitude with incremented temperatures over the range 23–137 °C. We provide a new perspective of temperature influence on fracture shearing – emphasizing the role of fracture properties (stiffnesses) of elastic tangential and normal stiffnesses on the energetics of slip. We use these stiffnesses to define a relationship linking injected volume to the resulting seismic moment. In transiting from 23 °C to 137 °C, tangential stiffness is halved and normal stiffness quadrupled, thus the resulting seismic moment is potentially reduced by a factor of eight – congruent with observations of reactivated seismic moments over the same temperature range. The change in stiffness can be explained by an increasing contact area, which we also observe by P wave measurements. Our results suggest that increased temperature inhibits fault seismicity and the expected maximum seismic moment of induced seismicity.
{"title":"Controls of temperature on seismic moment released from reactivated faults","authors":"Junpeng Wang , Agathe Eijsink , Matthew Roseboom , Chris Marone , Jacques Riviere , Parisa Shokouhi , Derek Elsworth","doi":"10.1016/j.tecto.2025.231062","DOIUrl":"10.1016/j.tecto.2025.231062","url":null,"abstract":"<div><div>Induced seismicity is the main uncertainty to safely produce geothermal energy, raising questions as to how applicable known physical laws are at increased temperatures. We explore the impact of elevated temperatures on maximum seismic moments anticipated in induced seismicity. We conduct laboratory reactivation experiments on a single inclined fracture (SIF) at equilibrated temperatures of 23 °C, 78 °C and 137 °C. Fractures are loaded at a constant shear stress of ∼80 % of the peak shear strength with slip activated by fluid injection. Reactivated seismic moments scale linearly with volume injected but decrease by one-order-of-magnitude with incremented temperatures over the range 23–137 °C. We provide a new perspective of temperature influence on fracture shearing – emphasizing the role of fracture properties (stiffnesses) of elastic tangential and normal stiffnesses on the energetics of slip. We use these stiffnesses to define a relationship linking injected volume to the resulting seismic moment. In transiting from 23 °C to 137 °C, tangential stiffness is halved and normal stiffness quadrupled, thus the resulting seismic moment is potentially reduced by a factor of eight – congruent with observations of reactivated seismic moments over the same temperature range. The change in stiffness can be explained by an increasing contact area, which we also observe by P wave measurements. Our results suggest that increased temperature inhibits fault seismicity and the expected maximum seismic moment of induced seismicity.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"923 ","pages":"Article 231062"},"PeriodicalIF":2.6,"publicationDate":"2026-01-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145894840","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-01-01DOI: 10.1016/j.tecto.2025.231063
Jiangtao Qiu , Jianbao Sun , Lingyun Ji , Liangyu Zhu
The Tianshan orogen, located at the northern margin of the India–Eurasia collision zone, is one of the world's most seismically active intracontinental mountain belts. However, a comprehensive understanding of its crustal deformation, strain accumulation, and fault locking patterns remains limited due to the lack of large-scale, high-resolution geodetic observations. In this study, we integrate Sentinel-1 interferometric synthetic aperture radar (InSAR) time-series analysis with regional Global Navigation Satellite System (GNSS) data to reconstruct a three-dimensional (3D) deformation field covering the entire Tianshan range. We apply atmospheric corrections using ERA5 reanalysis and constrain the InSAR solutions with GNSS data to significantly improve their consistency, enabling reliable quantification of crustal motions. Our results reveal pronounced spatial variability in north–south shortening, with rates reaching ∼20 mm/yr in the western segment (75°-79°E) and decreasing to 6–9 mm/yr in the eastern segment (85°-87°E). Uplift rates are higher in the South Tianshan (1.8–2.2 mm/yr) than in the North Tianshan (0.8–1.2 mm/yr), while strike-slip motions are concentrated along the southern foreland. Non-tectonic deformation is also identified, including large-scale subsidence due to groundwater extraction (∼34 mm/yr) and localized oilfield-induced subsidence (∼20 mm/yr). From the 3D deformation field, we derive the strain rate distribution and invert fault locking parameters using a block model with Bayesian optimization. High strain accumulation and strong locking are observed along the Pamir frontal thrust, the Maidan fault (which ruptured in the 2024 Mw 7.1 Wushi earthquake), the south Issyk-Kul fault, the Kepingtag fault (which ruptured in the 2020 Mw 6.0 Jiashi earthquake), and the Qiulitag belt. Our findings highlight the coupled tectonic and anthropogenic processes shaping Tianshan deformation and identify the western Qiulitag as a potential source for future large earthquakes.
{"title":"Multi-source geodetic constraints on 3D crustal deformation, strain accumulation, and fault locking in the Tianshan Orogen","authors":"Jiangtao Qiu , Jianbao Sun , Lingyun Ji , Liangyu Zhu","doi":"10.1016/j.tecto.2025.231063","DOIUrl":"10.1016/j.tecto.2025.231063","url":null,"abstract":"<div><div>The Tianshan orogen, located at the northern margin of the India–Eurasia collision zone, is one of the world's most seismically active intracontinental mountain belts. However, a comprehensive understanding of its crustal deformation, strain accumulation, and fault locking patterns remains limited due to the lack of large-scale, high-resolution geodetic observations. In this study, we integrate Sentinel-1 interferometric synthetic aperture radar (InSAR) time-series analysis with regional Global Navigation Satellite System (GNSS) data to reconstruct a three-dimensional (3D) deformation field covering the entire Tianshan range. We apply atmospheric corrections using ERA5 reanalysis and constrain the InSAR solutions with GNSS data to significantly improve their consistency, enabling reliable quantification of crustal motions. Our results reveal pronounced spatial variability in north–south shortening, with rates reaching ∼20 mm/yr in the western segment (75°-79°E) and decreasing to 6–9 mm/yr in the eastern segment (85°-87°E). Uplift rates are higher in the South Tianshan (1.8–2.2 mm/yr) than in the North Tianshan (0.8–1.2 mm/yr), while strike-slip motions are concentrated along the southern foreland. Non-tectonic deformation is also identified, including large-scale subsidence due to groundwater extraction (∼34 mm/yr) and localized oilfield-induced subsidence (∼20 mm/yr). From the 3D deformation field, we derive the strain rate distribution and invert fault locking parameters using a block model with Bayesian optimization. High strain accumulation and strong locking are observed along the Pamir frontal thrust, the Maidan fault (which ruptured in the 2024 Mw 7.1 Wushi earthquake), the south Issyk-Kul fault, the Kepingtag fault (which ruptured in the 2020 Mw 6.0 Jiashi earthquake), and the Qiulitag belt. Our findings highlight the coupled tectonic and anthropogenic processes shaping Tianshan deformation and identify the western Qiulitag as a potential source for future large earthquakes.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"922 ","pages":"Article 231063"},"PeriodicalIF":2.6,"publicationDate":"2026-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145894842","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-01-01DOI: 10.1016/j.tecto.2025.231066
Wei Cheng , Xiaogang Hu , Yan Lu , Xinghui Liang , Lintao Liu , Panpan Zhang , Yufeng Zhou
The northwestern part of the Pacific plate is subducting into the Kuril trench at high speed, which is expected to result in strong shear on the underlying mantle asthenosphere. However, the splitting measurements in the Kuril subslab mantle reveal complex patterns of seismic anisotropy along the Kuril subduction zone. Love-to-Rayleigh scattered waves (quasi-Love waves) are straightforward indicators of sharp lateral gradients in the anisotropic properties of the Earth's upper mantle (at depths of 100–200 km). Here, we present observations of quasi-Love waves at stations located in Japan from surface waves that sampled the Kuril subslab mantle. Clear quasi-Love waves were diagnosed from 11 earthquakes. The inferred quasi-Love scatterers are located mainly in central and northern Kuril, suggesting the presence of extensive lateral anisotropic gradients in the Kuril subslab mantle, whereas southern Kuril lacks similar anisotropic gradients in the subslab mantle. The lateral anisotropic gradients in northern Kuril may simply reflect the transition from anisotropic subducted slab to mantle flow in the asthenosphere or reflect local toroidal flow around the slab edges, while the lateral anisotropic gradients in northern Kuril may indicate the regions where subslab mantle flow is significantly deflected. Considering the specific slab geometry in and around the Kuril subduction zone, we infer that the detachment of the subducting northwest Pacific slab beneath the Aleutian–Kamchatka junction and the fast slab rollback in central Kuril may be the driving forces for the generation of lateral anisotropic gradients beneath the central Kuril. Our observations of quasi-Love waves provide new constraints on the mantle anisotropy in Kuril.
{"title":"Lateral anisotropic gradients in the subslab mantle beneath the Kuril subduction zone detected by observations of quasi-Love wave scattering","authors":"Wei Cheng , Xiaogang Hu , Yan Lu , Xinghui Liang , Lintao Liu , Panpan Zhang , Yufeng Zhou","doi":"10.1016/j.tecto.2025.231066","DOIUrl":"10.1016/j.tecto.2025.231066","url":null,"abstract":"<div><div>The northwestern part of the Pacific plate is subducting into the Kuril trench at high speed, which is expected to result in strong shear on the underlying mantle asthenosphere. However, the splitting measurements in the Kuril subslab mantle reveal complex patterns of seismic anisotropy along the Kuril subduction zone. Love-to-Rayleigh scattered waves (quasi-Love waves) are straightforward indicators of sharp lateral gradients in the anisotropic properties of the Earth's upper mantle (at depths of 100–200 km). Here, we present observations of quasi-Love waves at stations located in Japan from surface waves that sampled the Kuril subslab mantle. Clear quasi-Love waves were diagnosed from 11 earthquakes. The inferred quasi-Love scatterers are located mainly in central and northern Kuril, suggesting the presence of extensive lateral anisotropic gradients in the Kuril subslab mantle, whereas southern Kuril lacks similar anisotropic gradients in the subslab mantle. The lateral anisotropic gradients in northern Kuril may simply reflect the transition from anisotropic subducted slab to mantle flow in the asthenosphere or reflect local toroidal flow around the slab edges, while the lateral anisotropic gradients in northern Kuril may indicate the regions where subslab mantle flow is significantly deflected. Considering the specific slab geometry in and around the Kuril subduction zone, we infer that the detachment of the subducting northwest Pacific slab beneath the Aleutian–Kamchatka junction and the fast slab rollback in central Kuril may be the driving forces for the generation of lateral anisotropic gradients beneath the central Kuril. Our observations of quasi-Love waves provide new constraints on the mantle anisotropy in Kuril.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"923 ","pages":"Article 231066"},"PeriodicalIF":2.6,"publicationDate":"2026-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145894944","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-12-31DOI: 10.1016/j.tecto.2025.231064
Yan Xu, Shunping Pei, Xinhua Jia, Chaodi Xie, Mingrui Huang
Two intermediate-depth earthquakes with moment magnitude 5.8 and 5.3 respectively occurred in the Pamir-Hindu Kush in August 2023. We select three subarrays that exhibit a two-dimensional delta-shaped array response function from a temporary regional short-period array. For each event/subarray pair, the data is slant-stacked and normalized with respect to the initial p phase. Two secondary arrivals, P410p and s140p, bring out the information of the upper mantle beneath Pamir-Hindu Kush area. The reflection depth of the P-wave from the 410-km discontinuity suggests that the subducted cold slab of the Hindu Kush penetrates the discontinuity, uplifting it to a shallower depth as the reflection point approaches the cold core. The deepening trend of the reflection depth along the strike of the Pamir slab is consistent with the model that suggests the splitting of the subducted Pamir slab with its western part abutting against the Hindu Kush slab below 350 km. Our data provide a direct sampling of the boundary zone between the abutted Pamir-Hindu Kush slab and the normal mantle material. We observe a P wave, s140p, that was converted from an upgoing S wave at a depth of 140 km. This s140p phase exhibits a rapid drop in energy within a spatially confined, northwest-southeast oriented area, suggesting a near-vertical velocity boundary.
{"title":"Detailed structure of upper mantle discontinuities beneath the Pamir-Hindu Kush from the short period regional seismic array","authors":"Yan Xu, Shunping Pei, Xinhua Jia, Chaodi Xie, Mingrui Huang","doi":"10.1016/j.tecto.2025.231064","DOIUrl":"10.1016/j.tecto.2025.231064","url":null,"abstract":"<div><div>Two intermediate-depth earthquakes with moment magnitude 5.8 and 5.3 respectively occurred in the Pamir-Hindu Kush in August 2023. We select three subarrays that exhibit a two-dimensional delta-shaped array response function from a temporary regional short-period array. For each event/subarray pair, the data is slant-stacked and normalized with respect to the initial <em>p</em> phase. Two secondary arrivals, <em>P</em>410<em>p</em> and <em>s</em>140<em>p</em>, bring out the information of the upper mantle beneath Pamir-Hindu Kush area. The reflection depth of the P-wave from the 410-km discontinuity suggests that the subducted cold slab of the Hindu Kush penetrates the discontinuity, uplifting it to a shallower depth as the reflection point approaches the cold core. The deepening trend of the reflection depth along the strike of the Pamir slab is consistent with the model that suggests the splitting of the subducted Pamir slab with its western part abutting against the Hindu Kush slab below 350 km. Our data provide a direct sampling of the boundary zone between the abutted Pamir-Hindu Kush slab and the normal mantle material. We observe a P wave, <em>s</em>140<em>p</em>, that was converted from an upgoing S wave at a depth of 140 km. This <em>s</em>140<em>p</em> phase exhibits a rapid drop in energy within a spatially confined, northwest-southeast oriented area, suggesting a near-vertical velocity boundary.</div></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"922 ","pages":"Article 231064"},"PeriodicalIF":2.6,"publicationDate":"2025-12-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145894945","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}