N. Terence Edgar
United States Geological Survey
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Marine and Petroleum Geology | 1992
William P. Dillon; Jim Austin; Kathryn M. Scanlon; N. Terence Edgar; Lindsay M. Parson
Abstract Broad-range side-scan sonar (GLORIA) images and single- and multi-channel seismic reflection profiles demonstrate that the margin of north-western Hispaniola has experienced compression as a consequence of oblique North American-Caribbean plate convergence. Two principal morphological or structural types of accretionary wedges are observed along this margin. The first type is characterized by a gently sloping (≈4°) sea floor and generally margin-parallel linear sets of sea-floor ridges that gradually deepen towards the flat Hispaniola Basin floor to the north. The ridges are caused by an internal structure consisting of broad anticlines bounded by thrust faults that dip southwards beneath Hispaniola. Anticlines form at the base of the slope and are eventually sheared and underthrust beneath the slope. In contrast, the second type of accretionary wedge exhibits a steeper (≈6–16°) sea-floor slope characterized by local slumping and a more abrupt morphological transition to the adjacent basin. The internal structure appears chaotic on seismic reflection profiles and probably consists of tight folds and closely spaced faults. We suggest that changes in sea-floor declivity and internal structure may result from variations in the dip or frictional resistance of the decollement, or possibly from changes in the cohesive strength of the wedge sediments. The observed pattern of thickening of Hispaniola Basin turbidites towards the insular margin suggests differential southwards tilting of the Hispaniola Basin strata, probably in response to North America-Caribbean plate interactions since the Early Tertiary. Based upon indirect age control from adjacent parts of the northern caribbean plate boundary, we infer a Late Eocene to Early Miocene episode of transcurrent motion (i.e. little or no tilting), an Early Miocene to Late Pliocene period of oblique convergence (i.e. increased tilt) during which the accretionary wedge began to be constructed, and a Late Pliocene to Recent episode of increased convergence (i.e. twice the Miocene to Pliocene tilt), which has led to rapid uplift and erosion of sediment sources on the margin and on Hispaniola, generating a submarine fan at the base of the insular slope.
Eos, Transactions American Geophysical Union | 2007
Thomas M. Cronin; N. Terence Edgar; Gregg R. Brooks; David W. Hastings; Rebekka A Larson; Albert C. Hine; Stanley D. Locker; B. C. Suthard; Benjamin P. Flower; David J. Hollander; John F. Wehmiller; Debra A. Willard; Shannon A. Smith
Understanding relative sea level (RSL) rise during periods of rapid climatic change is critical for evaluating modern sea level rise given the vulnerability of Antarctic ice shelves to collapse [Hodgson et al, 2006], the retreat of the worlds glaciers [Oerlemans, 2005], and mass balance trends of the Greenland ice sheet [Rignot and Kanagaratnam, 2006]. The first-order pattern of global sea level rise following the Last Glacial Maximum (LGM, ∼21,000 years ago) is well established from coral [Fairbanks, 1989], continental shelf [Hanebuth et al, 2000], and other records [Pirazzoli, 2000] and has been integrated into a global ICE-5G model of glacio-isostatic adjustment (GIA) [Peltier, 2004]. However, uncertainty introduced by paleo water depth of sea level indicators, radiocarbon chronology (i.e., reservoir corrections for marine shell dates), postglacial isostatic adjustment, and other processes affecting vertical position of former shorelines produces scatter in RSL curves, limiting our knowledge of sea level rise during periods of rapid glacial decay. One example of this limitation is the Gulf of Mexico/Florida region where, despite decades of study, RSL curves produce two conflicting patterns: those showing progressive submergence with a decelerating rate during the past 5000 years [Scholl et al, 1969] and those showing high sea level during the middle of the Holocene [Blum et al, 2001; Balsillie and Donoghue, 2004], where the Holocene represents a geologic epoch that extends from about 10,000 years ago to present times. This discrepancy is emblematic of the uncertainty surrounding Holocene sea level and ice volume history in general.
Archive | 1996
William P. Dillon; N. Terence Edgar; Kathryn M. Scanlon; Dwight F. Coleman
Archive | 1996
William P. Dillon; N. Terence Edgar; Kathryn M. Scanlon; Dwight F. Coleman
Geological Society of America Special Papers | 1991
N. Terence Edgar
Archive | 2002
N. Terence Edgar; Debra A. Willard; G.R. Brooks; Thomas D. Cronin; David W. Hastings; Benjamin P. Flower; Peter W. Swarzenski; David J. Hollander; Richard A. Larson; Albert C. Hine; B. C. Suthard; Stanley D. Locker; Wm. Jason Greenwood
Geology | 1992
N. Terence Edgar; William P. Dillon; Eric Rosencrantz; Paul Mann
Archive | 2005
David W. Hastings; T. A. Hollweg; Benjamin P. Flower; Thomas M. Cronin; N. Terence Edgar; Todd M. Quinn
Archive | 2004
David W. Hastings; T. A. Hollweg; Benjamin P. Flower; Thomas M. Cronin; N. Terence Edgar; Todd M. Quinn
Archive | 2002
B. C. Suthard; Albert C. Hine; Stanley D. Locker; David Scott Duncan; Robert A. Morton; Mary Eschelbach Hansen; N. Terence Edgar