2013
DOI: 10.1093/gji/ggt010
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A new catalogue of normal-mode splitting function measurements up to 10 mHz

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Cited by 66 publications
(175 citation statements)
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References 40 publications
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“…The synthetic data for the normal modes thus consisted of 309 (184 + 125) free oscillation centre frequencies. The synthetic data were corrupted by adding Gaussian noise with zero mean and a standard deviation given by the uncertainty estimate for each measurement, as reported by Deuss et al (2013), Koelemeijer et al (2013), Koelemeijer (2014) and on the REM website (http :/ / igppweb .ucsd .edu /~gabi /rem .dir /surface /tmodes .list). We note that the measurement errors were estimated using a cross-validation approach, which may not fully account for any systematic uncertainties.…”
Section: Synthetic Datamentioning
confidence: 99%
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“…The synthetic data for the normal modes thus consisted of 309 (184 + 125) free oscillation centre frequencies. The synthetic data were corrupted by adding Gaussian noise with zero mean and a standard deviation given by the uncertainty estimate for each measurement, as reported by Deuss et al (2013), Koelemeijer et al (2013), Koelemeijer (2014) and on the REM website (http :/ / igppweb .ucsd .edu /~gabi /rem .dir /surface /tmodes .list). We note that the measurement errors were estimated using a cross-validation approach, which may not fully account for any systematic uncertainties.…”
Section: Synthetic Datamentioning
confidence: 99%
“…Furthermore, PREM was used as a reference model in an iterative damped least-squares inversion of normal-mode spectra for splitting function coefficients, e.g. Deuss et al (2013). As such, the coefficients could in principle be biased towards PREM.…”
Section: Synthetic Datamentioning
confidence: 99%
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“…Measurements of surface-wave dispersion (i.e., the frequency-dependent surface-wave speed) are key in our understanding of lithospheric structure, especially in oceanic regions where few seismic stations are located (e.g., Debayle et al, 2005;Ekströ m et al, 1997;Laske, 1995;Lévêque and Cara, 1985;Lin and Ritzwoller, 2011;Montagner and Tanimoto, 1991;Nakanishi and Anderson, 1982;Nataf et al, 1986;Ritsema et al, 2004;Trampert and Woodhouse, 1995;van Heijst and Woodhouse, 1999;Visser et al, 2008a;Zhang and Tanimoto, 1993). Normal-mode spectral measurements provide constraints on the longest wavelength part of lateral heterogeneity through the Earth (e.g., Deuss et al, 2011Deuss et al, , 2013Häfner and WidmerSchnidrig, 2013;He and Tromp, 1996;Masters et al, 1982Masters et al, , 1996Resovsky and Ritzwoller, 1999). These data lend themselves for joint inversions for shear and compressional velocity Masters et al, 1996) and even density Tromp, 1999, 2001;Kuo and Romanowicz, 2002).…”
Section: Data Types In Seismic Tomographymentioning
confidence: 99%
“…Lateral heterogeneity (both elastic heterogeneity and anisotropy) also has a significant effect. Tomographers use observations of splitting to constrain the large-scale variations (e.g., Deuss et al, 2011Deuss et al, , 2013Giardini et al, 1987;He and Tromp, 1996;Ishii and Tromp, 1999;Masters et al, 1996;Resovsky and Ritzwoller, 1999;Ritzwoller et al, 1998), although in general only the 'even-degree' structure of the Earth can be constrained in a direct manner. Splitting measurements are not easy to make.…”
Section: Normal Modesmentioning
confidence: 99%