Dissertations / Theses on the topic 'Deep subduction'
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Karel, Patrick Robert. "Seismic Analysis of the Tonga Subduction Zone and Implications on the Thermo-Petrologic Evolution of Deep Subduction." Miami University / OhioLINK, 2011. http://rave.ohiolink.edu/etdc/view?acc_num=miami1313773845.
Full textKlonowska, Iwona. "Deep subduction of the Seve Nappe Complex in the Scandinavian Caledonides." Doctoral thesis, Uppsala universitet, Institutionen för geovetenskaper, 2017. http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-332525.
Full textCastle, John C. "Imaging mid-mantle discontinuities : implications for mantle chemistry, dynamics, rheology, and deep earthquakes /." Thesis, Connect to this title online; UW restricted, 1998. http://hdl.handle.net/1773/6809.
Full textYoshida, Kenta. "Deep fluid characteristics in the subduction zone: A window from metamorphic quartz veins." 京都大学 (Kyoto University), 2015. http://hdl.handle.net/2433/199115.
Full textBellew, Glen M. "Consolidation properties, stress history, and modeling of pore pressures for deep sea sediments at the Nankai Trough /." free to MU campus, to others for purchase, 2004. http://wwwlib.umi.com/cr/mo/fullcit?p1421111.
Full textSeccia, Danilo <1980>. "Deep geometry of subduction below the Andean belt of Colombia as revealed by seismic tomography." Doctoral thesis, Alma Mater Studiorum - Università di Bologna, 2012. http://amsdottorato.unibo.it/4290/.
Full textBloch, Wasja [Verfasser]. "In-situ Properties of the Subducting Nazca Slab: Constraints on the Deep Water Cycle and the Dynamics of Subduction from Seismological Observations / Wasja Bloch." Berlin : Freie Universität Berlin, 2017. http://d-nb.info/1140043447/34.
Full textHolmberg, Johanna. "Pressure-Temperature-time Constraints on the Deep Subduction of the Seve Nappe Complex in Jämtland and southern Västerbotten, Scandinavian Caledonides." Thesis, Uppsala universitet, Institutionen för geovetenskaper, 2017. http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-334822.
Full textDe Skandinaviska Kaledoniderna har bildats genom en kollision mellan de två kontinentalplattorna Baltika och Laurentia då Japetushavet stängdes omkring 400 miljoner år sedan. Till följd av de starkt komprimerande krafterna transporterades stora flak (skollor) av havsbottenberggrund och kontinentalskorpa hundratals kilometer upp på Baltikakontinenten. Skollorna är överskjutna på varandra omlott och benämns som undre, mellersta, övre och översta skollberggrunderna och återfinns idag i vår fjällkedja. Innan kollisionen med Laurentia krockade Baltika med en vulkanisk öbåge, vilket resulterade i att delar av Baltika pressades ner så pass djupt att bland annat diamanter bildades till följd av det ultrahöga trycket. Bevis för omvandling under extremt tryck finns i den så kallade Seveskollan som utgör en del av den mellersta skollberggrunden. Seveskollan är ett komplex av tre olika enheter, som utsatts för olika grad av metamorfos till följd av tryck och temperatur. Till följd av väder och vind under miljontals år så är fjällkedjan idag nederoderad och därav väl exponerad. Det gör att de Skandinaviska Kaledoniderna är en av världens bästa platser att studera och förstå bergskedjebildade processer. Av den anledningen borrade djupborrningsprojektet COSC-1 en cirka 2.4 km långt kärnborrhål genom den lägst belägna enheten i Seve komplexet (lägre Seveskollan) strax nedanför Åreskutan i Jämtlandsfjällen. Över COSC-1 profilen ligger den berggrund som tillhör den mellersta Seveskollan, även kallad Åreskutanskollan. Åreskutanskollan är en del av Baltika som utsattes för ultrahöga tryck, och i kyanitförande gnejser har diamanter inneslutna i det motståndskraftiga mineralet granat påträffats. Nyligen, längre norrut i Saxnäs (södra Västerbotten) har ytterligare diamantförande gnejser påträffats i den mellersta Seveskollan, som karaktäriseras i den här studien. Material från COSC-1 borrkärnan har använts för att bestämma under vilka tryck och temperatur bergarterna i den lägre Seveskollan har metmorfoserats, för att förstå den tektoniska och metamorfa utvecklingen och även relationen till den överliggande högmetamorfa Åreskutanskollan. Trycket har bestämts genom den relativt oprövade metoden QuiG -barometri. Små kristaller av kvarts inneslutna i granat har analyserats med Raman spektroskopi och de fysikaliska parametrarna av kvarts och granat kan direkt översättas till tryck. Temperatur har erhållits genom det temperaturkänsliga ämnet titan i kvartsinneslutningarna. Resultatet visar att den lägre Seveskollan har genomgått minst två metamorfa faser genom tektonisk påverkan. Den första fasen varierar från övre grönskiffer-amfibolit till lägre eklogitfacies under tryck och temperatur av ca 8-13 kbar, 525-695 o C. Den andra fasen är associerad med överskjutning och skjuvning, vilket orsakade retrograd metamorfos i grönskifferfacies under lägre tryck och temperatur (ca 7-10 kbar, 450-550 o C). Datering baserat på radioaktivt sönderfall av lutetium till hafnium i granat fastställer att Åreskutanskollan utsattes för ultrahögt tryck för omkring 450 miljoner år sedan, samtidigt som lägre Seveskollan nådde metamorft klimax. Resultaten visar även att lägre och mellersta Seveskollorna skjuvades samtidigt, omkring 424 miljoner år sedan. Det betyder att de erhöll sina nuvarande tektonostratigrafiska positioner på stort djup innan överskjutningen på Baltika. Detaljerad petrografi påvisar att de diamantförande kyanit-och granatförande gnejserna från Saxnäs visar påtagliga likheter med Åreskutanskollans högtrycksgnejser. Det tyder på att berggrunden i Saxnäs kan kopplas samman med Åreskutanskollan och att ultrahögtrycksmetamorfos av den mellersta Seveskollan omfattar ett större område än vad som tidigare antagits.
Mukti, Muhammad Ma'ruf. "Tectonic Evolution of the South Sumatra-Java Forearc System from Deep Seismic Reflection Data." Paris, Institut de physique du globe, 2013. http://www.theses.fr/2013GLOB1101.
Full textHammerschmidt, Sebastian B. [Verfasser], Achim [Akademischer Betreuer] Kopf, and Wolfgang [Akademischer Betreuer] Bach. "Monitoring of Deep Fluids in the Nankai Subduction Complex, SE offshore Japan / Sebastian B. Hammerschmidt. Gutachter: Achim Kopf ; Wolfgang Bach. Betreuer: Achim Kopf." Bremen : Staats- und Universitätsbibliothek Bremen, 2014. http://d-nb.info/1072226421/34.
Full textSoto, Parada Hugo Enrique [Verfasser]. "From Classical Earthquake Location to Deep Learning-based Phase Detection and Picking using Seismic Data from the Northern Chile Subduction Zone / Hugo Enrique Soto Parada." Berlin : Freie Universität Berlin, 2021. http://d-nb.info/1233679252/34.
Full textGonzalez, Miguel. "Nature and origin of sedimentary deposits in the Ecuador subduction trench : paleoseismological implications." Thesis, Rennes 1, 2018. http://www.theses.fr/2018REN1B009/document.
Full textRecent deep marine sedimentation in subduction trenches is characterized by the inter-stratification of hemipelagic and turbidite sediments locally interbedded with debris flow, which can result from continental slope shaking triggered by earthquakes. The active margin of Ecuador comprises tectonic erosion that contributes to the formation of a deep trench filled by a complex suite of sedimentary facies. Gravity flow sedimentation is ubiquitous along the margin and facies range from laterally continuous m-thick mass transport deposits to isolated cm-thick turbidites intercalated with hemipelagite, volcanoclastics and tephra. In this study we show interpretation of swath bathymetry, high-resolution seismic profiles and petrophysical data from cores. The objective is to describe the morphologic complexity on the Ecuadorian border of the Nazca plate where a set of deep marine asperities is subducting at different scales, and their consequences on the distribution of sediments in the different sub-basins. Ecuadorian margin comprises three geomorphological segments: The northern segment, northward of the Carnegie Ridge, is characterized by a wide (5-10 km) and deep trench (3800 – 4000 m), a gentler gullied continental slope and a shelf (10-40 km wide) with active subsidence. The central segment facing the Carnegie Ridge, is strongly influenced by the subduction of the Carnegie ridge which induces a narrow (0–5 km wide) and shallow trench (3100 – 3700 m depth), a steep and gullied slope with no canyons and a 15–40 km wide shelf characterized by areas with active subsidence and uplift. Finally, the southern segment, southward of the Carnegie Ridge, presents a wide (5–10 km) and deep (4000–4700 m) trench, a starved continental slope with well-defined canyon systems and a wide subsiding shelf (20–50 km). The sedimentary dynamics along the margin is evaluated by the analysis of 15 cores. Visual description, high-resolution photographs, X-Ray imagery, XRF data and petrophysical properties led to the identification of 11 sedimentary facies that characterize seven sedimentary processes: turbidites, hemipelagites, tephras, debris flows, homogenites, slumps, and ooze carbonate deposits. Age of the deposits is defined by radiocarbon age dating of hemipelagic sediments. Ages range from 500 to 48,000 years BP. High-resolution seismic profiles allow definition of three echo-facies: transparent, layered and chaotic. Transparent echo-facies is mainly associated to homogenite deposits, layered echo-facies is associated to the turbiditic-hemipelagic interbedded deposits and chaotic echo-facies is associated to reworked gravity flow deposits. The trench fill represents a lacunar but important record of the subduction margin history. Large eastward debris flows in the lower two sequences of the trench fill are provided by the trench outer wall as a results of slope failures along normal faults due to the downward bending of the oceanic plate. The sediment of the upper sequence of the trench fill draping the trench floor, are largely provided by the inner trench wall strongly controlled by the Carnegie Ridge. As a result, depth, frequency, thickness, composition and lateral disposition of the deposits vary greatly from those at north and south. The large, simple mega-beds like slump, debris flows and homogenites are located at the northern and southern segments. They were triggered by large regional faults in the North and enhanced by the activity of sets of splay faults in the South overhanging the seafloor at the slope toe. Small-size, fluid rich events were triggered by subduction of isolated seamounts at the edges of the Carnegie Ridge due to frequent but small destabilizations of an inner trench wall preconditioned by the impacts of successive seamounts. Sets of partly volcanoclastic turbidites in central segment might have been triggered by the complex interaction of slope and continental shelf deformation by seamount subduction
Gunawardana, Prasanna M. "Deep Earthquakes Spatial Distribution| Numerical Modeling of Stress and Stored Elastic Energy Distribution within the Subducting Lithosphere." Thesis, University of Louisiana at Lafayette, 2016. http://pqdtopen.proquest.com/#viewpdf?dispub=10163344.
Full textThe spatial distribution of deep earthquakes remains elusive, as the earthquakes below 30 km depth cannot be explained using the brittle frictional processes due to the fluid behavior of rocks under high pressure and temperature conditions. Several models that have been developed to identify the source distribution fall largely into categories like negative buoyancy and viscous friction to the flow, anti-crack faulting due to metastable olivine, volume reductions from phase transformations etc. Still none of them were able to satisfactorily explain the spatial distribution of deep earthquakes. We propose a new method using the visco-elastic nature of the earth material to model the deformation, stress, and elastic energy of the subducting lithosphere using “Marker in cell method” in combination with a conservative finite difference scheme. The software is written in Python and NumPy. We have tested this code for the known results of a Rayleigh–Taylor instability of solid-fluid interaction, and for a general subduction benchmark (Schmeling et al., 2008). We show a large set of numerical models in which we investigate the role of volatiles in the transition zone by varying the viscosity of the lithosphere and the presence of a high viscosity zone below the upper-lower mantle transition zone. Finally, we compare the rate of inner energy dissipation and the stored elastic energy in the subducting lithosphere with deep earthquake spatial distribution and discuss which constrains geodynamic models offer to deep earthquake location.
Wang, Liang-Chun, and 王亮鈞. "A deep-crust study of the southern Ryukyu subduction system." Thesis, 2011. http://ndltd.ncl.edu.tw/handle/10472855981764781859.
Full textRüpke, Lars Helmuth [Verfasser]. "Effects of plate subduction on the earth's deep water cycles / vorgelegt von Lars Helmuth Rüpke." 2004. http://d-nb.info/972161201/34.
Full textAlbrecht, Nina. "Metamorphic fluids at extreme pressure conditions and their significance for element transfer in subduction zones." Doctoral thesis, 2017. http://hdl.handle.net/11858/00-1735-0000-0023-3E42-C.
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