2016
DOI: 10.1002/2015jb012737
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Geodetic observations of postseismic creep in the decade after the 1999 Izmit earthquake, Turkey: Implications for a shallow slip deficit

Abstract: The relationship between aseismic slip and tectonic loading is important for understanding both the pattern of strain accumulation along a fault and its ability to generate large earthquakes. We investigate the spatial distribution and temporal evolution of aseismic creep on the western North Anatolian Fault (NAF) using time series analysis of Envisat interferometric synthetic aperture radar (InSAR) data, covering the full extent of the 1999 Izmit and Düzce earthquake ruptures and spanning 2002–2010. Discontin… Show more

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Cited by 51 publications
(68 citation statements)
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References 86 publications
(148 reference statements)
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“…Therefore, it is impossible to calculate the full 3‐D velocity field without a prior assumption. The common assumption made in previous studies is that there is no vertical motion across the region of interest [e.g., Walters et al , ; Hussain et al , ]. In our case we note that both the ascending and descending tracks are equally insensitive to motion in the north‐south direction.…”
Section: Interseismic Velocity Field Across the Central Nafsupporting
confidence: 69%
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“…Therefore, it is impossible to calculate the full 3‐D velocity field without a prior assumption. The common assumption made in previous studies is that there is no vertical motion across the region of interest [e.g., Walters et al , ; Hussain et al , ]. In our case we note that both the ascending and descending tracks are equally insensitive to motion in the north‐south direction.…”
Section: Interseismic Velocity Field Across the Central Nafsupporting
confidence: 69%
“…For every pixel where information from both ascending and descending geometries are available, we use equation to invert for the east‐west and vertical components of motion following the method described by Wright et al [] and Hussain et al [] while taking into account the local incidence angles: DLOS=[]sin(θ)cos(α)1emsin(θ)sin(α)1emcos(θ)[]DEDNDU, where D LOS is the LOS velocity, θ is the local radar incidence angle, α is the azimuth of the satellite heading vector, and [ D E , D N , D U ] T is a vector with the east, north, and vertical components of motion, respectively.…”
Section: Interseismic Velocity Field Across the Central Nafmentioning
confidence: 99%
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