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  • 1
    Publication Date: 2024-04-20
    Description: To examine the temperature impact on the DPG signals related to internal motions, four Cox-Webb differential pressure gauges (DPGs) fixed on the ocean bottom and a high-resolution temperature sensor (T-sensor) 13 m above the seafloor as a square-kilometer array deployed offshore eastern Taiwan facing the open Pacific Ocean. The DPGs and T-sensor were built by the Institute of Earth Sciences of Academia Sinica and Royal Netherlands Institute for Sea Research (NIOZ), respectively. In addition, a Nortek AquaDopp acoustic current meter with pressure sensor was attached on the same vertical string with the T-sensor at 2936 m. The multiple instruments in the array were located at depths between 3000 and 3200 m with inter-station horizontal distances ranging from about 300 m to 1 km. The time series data with 2 mHz sampling rate in ASCII format were used to study propagation of the deep-sea internal waves between September 2017 and April 2018. Fifteen events of the internal motions were selected by T-sensor-DPG correlation coefficient 〉 0.7 at every DPG in a 3-day time window that is shifted in time by 1 day. The propagating direction and apparent horizontal phase speed of the internal waves can be estimated by the DPG data using array analysis methods.
    Keywords: MULT; Multiple investigations; Taiwan; Taiwan_SEcoast
    Type: Dataset
    Format: application/zip, 644.1 kBytes
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  • 2
    Publication Date: 2022-05-25
    Description: Author Posting. © The Authors, 2009. This article is posted here by permission of John Wiley & Sons for personal use, not for redistribution. The definitive version was published in Geophysical Journal International 179 (2009): 1859-1869, doi:10.1111/j.1365-246X.2009.04391.x.
    Description: A broad-band ocean-bottom seismometer (OBS) deployed ~180 km east of Taiwan provides a first glimpse into the upper mantle beneath the westernmost section of the Philippine Sea or the Huatung basin (HB). We measured interstation phase velocities of Rayleigh waves between the OBS and stations on the eastern coast of Taiwan. The phase velocities show smooth variations from 3.8 to 3.9 km s−1 for periods of 25–40 s. In this short period range, phase velocities are comparable to those characterizing the 15–30 Ma Parece-Vela basin of the Philippine Sea. Modelling of the finite-frequency effect proves the validity of the measurement for the average HB. The shear-wave velocity models inverted from the 25 to 40 s dispersion show a velocity at lithospheric depths about 0.1 km s−1 lower than that of the west Philippine Sea, which agrees with the age effect derived from the Pacific pure-path model. Inversions incorporating the less reliable data above 40 s yield a shear velocity 〈4.0 km s−1 below 150 km, an unrealistic value even for a hotspot plume environment. The seismological evidence, together with the correlation in seafloor depth, suggests that the HB and the Parece-Vela basin may have a similar age. This is at odds with the previous geochronological study suggesting an early-Cretaceous age for the HB. Thermal rejuvenation of the lithosphere was examined as a potential solution to reconciling the two age models.
    Description: The research is supported by the National Science Council, Taiwan, Republic of China, under grant NSC 96–2745-M-001–005.
    Keywords: Surface waves and free oscillations ; Wave propagation ; Continental margins: convergent ; Dynamics of lithosphere and mantle
    Repository Name: Woods Hole Open Access Server
    Type: Article
    Format: application/pdf
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  • 3
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 121 (1995), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: The anomalous sea-floor topography and geoid height over the Australian-Antarctic Discordance (AAD) are examined and attributed to dynamic mantle flow in this study. Because the subsidences of sea-floor depth and geoid with age exhibit forms of isostatic response of cooling from the surface, they are removed from the data to retain the dynamic components. In removing the cooling effect we allow for different subsidence rates for different spreading corridors. The reduction yields primarily north-south-trending lows crossing the AAD in both the residual topography and the residual geoid. Assuming that the mantle behaves viscously, the residual data were inverted to thermal perturbations in the assigned depth extents. The obtained thermal perturbations exhibit mainly east-west, or axis-parallel variation and indicate that along the 3000 km long ridge, the mantle beneath the AAD is about 150 and 50°C colder than average for perturbation layers confined within 100 and 300 km from the surface, respectively. As a result, the 3-D flow driven by the thermal anomaly is also predominantly east-west oriented with a major downwelling near the AAD and its aged mantle. To independently constrain these results, we derive a simple formula to estimate the mantle temperature beneath the ridge from the subsidence rates of topography and geoid for different corridors. This simple estimation yields a variation of about 200°C with the low near AAD and high at the segment to the east. The trend of variation is consistent with that from the dynamic modelling, and the magnitude is relatively high but favours the model in which the dynamic source is concentrated within the upper asthenosphere. The thermal anomaly could be, however, eliminated by lateral advection in the along-axis direction which is not considered in the inversion. The advection effect is estimated to cause a decay of the dynamic topography at a rate of the order of 0.005 km Myr−1, making the downwelling die out very slowly with age. The actual 3-D anomalous flow in the south-east Indian Ridge area is probably still characterized more by a downwelling stretched across-axis as depicted by our dynamic modelling than in the form of a focused plume sinking at the AAD.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 108 (1992), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: To test a prediction of the anisotropic properties of the upper mantle beneath the central North Atlantic, we measure splitting of the waveforms of SKS phases recorded at WWSSN stations in the Azores (PDA), and on Bermuda (BEC). Because the analysis of individual, analogue records does not provide sufficient resolution, we have developed a new technique for representing the confidence limits that permits a straightforward estimation of the average splitting beneath a station from a group of events. If events from a variety of different azimuths are recorded, the average splitting parameters can be tightly constrained. We found five records for PDA and eight for BEC that have good signal-to-noise ratio and a prominent SKS phase. Only one of the phases at PDA shows evidence of splitting; the average anisotropy must be small if it exists at all. At BEC, the average anisotropy is significant with a fast direction between NW-SE and N-S and a time delay between the two split components of about 1 s. Both of these observations are significantly smaller than predicted by a model of the upper mantle anisotropy based on SS-S differential traveltimes. The absence of systematic anisotropy at PDA may be attributable to a complex flow pattern in the upper mantle at this site near the Eurasian-African plate boundary in the vicinity of an active hotspot. At BEC, the observed direction is consistent with the prediction and both the direction and the magnitude of the average anisotropy are indicative of a sublithospheric source.To check the reliability of these results from analogue records, we have performed a similar analysis for station KIP on Oahu where digital records are available for comparison. The results from digital and analogue records are similar. At KIP, the splitting is more variable than expected for uniform anisotropy, with the fast directions for individual records ranging from about N26°E to about N83°E and with variable time delays. Similar variability is observed at all three stations. The average anisotropy at KIP is well-constrained, however, with a time delay of about 0.6 s and fast direction N75°E. The fast direction coincides with the fossil sea-floor spreading direction beneath the Hawaiian islands, suggesting that the dominant source of anisotropy beneath KIP is lithospheric.
    Type of Medium: Electronic Resource
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  • 5
    ISSN: 1573-0581
    Keywords: Gravity anomalies ; Ridge-transform system ; Mantle upwelling ; Crustal thickness
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract To decipher the distribution of mass anomalies near the earth's surface and their relation to the major tectonic elements of a spreading plate boundary, we have analyzed shipboard gravity data in the vicinity of the southern Mid-Atlantic Ridge at 31–34.5° S. The area of study covers six ridge segments, two major transforms, the Cox and Meteor, and three small offsets or discordant zones. One of these small offsets is an elongate, deep basin at 33.5° S that strikes at about 45° to the adjoining ridge axes. By subtracting from the free-air anomaly the three-dimensional (3-D) effects of the seafloor topography and Moho relief, assuming constant densities of the crust and mantle and constant crustal thickness, we generate the mantle Bouguer anomaly. The mantle Bouguer anomaly is caused by variations in crustal thickness and the temperature and density structure of the mantle. By subtracting from the mantle Bouguer anomaly the effects of the density variations due to the 3-D thermal structure predicted by a simple model of passive flow in the mantle, we calculate the residual gravity anomalies. We interpret residual gravity anomalies in terms of anomalous crustal thickness variations and/or mantle thermal structures that are not considered in the forward model. As inferred from the residual map, the deep, major fracture zone valleys and the median, rift valleys are not isostatically compensated by thin crust. Thin crust may be associated with the broad, inactive segment of the Meteor fracture zone but is not clearly detected in the narrow, active transform zone. On the other hand, the presence of high residual anomalies along the relict trace of the oblique offset at 33.5° S suggests that thin crust may have been generated at an oblique spreading center which has experienced a restricted magma supply. The two smaller offsets at 31.3° S and 32.5° S also show residual anomalies suggesting thin crust but the anomalies are less pronounced than that at the 33.5° S oblique offset. There is a distinct, circular-shaped mantle Bouguer low centered on the shallowest portion of the ridge segment at about 33° S, which may represent upwelling in the form of a mantle plume beneath this ridge, or the progressive, along-axis crustal thinning caused by a centered, localized magma supply zone. Both mantle Bouguer and residual anomalies show a distinct, local low to the west of the ridge south of the 33.5° S oblique offset and relatively high values at and to the east of this ridge segment. We interpret this pattern as an indication that the upwelling center in the mantle for this ridge is off-axis to the west of the ridge.
    Type of Medium: Electronic Resource
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