59 research outputs found

    Spatio-temporal trends in normal-fault segmentation recorded by low-temperature thermochronology: Livingstone fault scarp, Malawi Rift, East African Rift System

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    The evolution of through-going normal-fault arrays from initial nucleation to growth and subsequent interaction and mechanical linkage is well documented in many extensional provinces. Over time, these processes lead to predictable spatial and temporal variations in the amount and rate of displacement accumulated along strike of individual fault segments, which should be manifested in the patterns of footwall exhumation. Here, we investigate the along-strike and vertical distribution of low-temperature apatite (U–Th)/He (AHe) cooling ages along the bounding fault system, the Livingstone fault, of the Karonga Basin of the northern Malawi Rift. The fault evolution and linkage from rift initiation to the present day has been previously constrained through investigations of the hanging wall basin fill. The new cooling ages from the footwall of the Livingstone fault can be related to the adjacent depocentre evolution and across a relay zone between two palaeo-fault segments. Our data are complimented by published apatite fission-track (AFT) data and reveal significant variation in rock cooling history along-strike: the centre of the footwall yields younger cooling ages than the former tips of earlier fault segments that are now linked. This suggests that low-temperature thermochronology can detect fault interactions along strike. That these former segment boundaries are preserved within exhumed footwall rocks is a function of the relatively recent linkage of the system. Our study highlights that changes in AHe (and potentially AFT) ages associated with the along-strike displacement profile can occur over relatively short horizontal distances (of a few kilometres). This is fundamentally important in the assessment of the vertical cooling history of footwalls in extensional systems: temporal differences in the rate of tectonically driven exhumation at a given location along fault strike may be of greater importance in controlling changes in rates of vertical exhumation than commonly invoked climatic fluctuations

    Large-scale mass wasting in the western Indian Ocean constrains onset of East African rifting

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    Faulting and earthquakes occur extensively along the flanks of the East African Rift System, including an offshore branch in the western Indian Ocean, resulting in remobilization of sediment in the form of landslides. To date, constraints on the occurrence of submarine landslides at margin scale are lacking, leaving unanswered a link between rifting and slope instability. Here, we show the first overview of landslide deposits in the post-Eocene stratigraphy of the Tanzania margin and we present the discovery of one of the biggest landslides on Earth: the Mafia mega-slide. The emplacement of multiple landslides, including the Mafia mega-slide, during the early-mid Miocene is coeval with cratonic rifting in Tanzania, indicating that plateau uplift and rifting in East Africa triggered large and potentially tsunamigenic landslides likely through earthquake activity and enhanced sediment supply. This study is a first step to evaluate the risk associated with submarine landslides in the region

    Skorohod representation theorem via disintegrations

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    Let (mun:ngeq0)(mu_n:ngeq 0) be Borel probabilities on a metric space SS such that munightarrowmu0mu_n ightarrowmu_0 weakly. Say that Skorohod representation holds if, on some probability space, there are SS-valued random variables XnX_n satisfying XnsimmunX_nsimmu_n for all nn and XnightarrowX0X_n ightarrow X_0 in probability. By Skorohod's theorem, Skorohod representation holds (with XnightarrowX0X_n ightarrow X_0 almost uniformly) if mu0mu_0 is separable. Two results are proved in this paper. First, Skorohod representation may fail if mu0mu_0 is not separable (provided, of course, non separable probabilities exist). Second, independently of mu0mu_0 separable or not, Skorohod representation holds if W(mun,mu0)ightarrow0W(mu_n,mu_0) ightarrow 0 where WW is Wasserstein distance (suitably adapted). The converse is essentially true as well. Such a WW is a version of Wasserstein distance which can be defined for any metric space SS satisfying a mild condition. To prove the quoted results (and to define WW), disintegrable probability measures are fundamental
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