2005
DOI: 10.1007/s11200-005-1627-3
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Differences in the Crustal and Uppermost Mantle Structure of the Bohemian Massif from Teleseismic Receiver Functions

Abstract: A target of our study was the Bohemian Massif in Central Europe that was emplaced during the Variscan orogeny. We used teleseismic records from ten broadband stations lying within and around the massif. Different techniques of receiver function interpretation were applied, including 1-D inversion of R-and Q-components, forward modelling of V s velocity, and simultaneous determination of Moho depth and Poisson's ratio in the crust. These results provide new, independent information about the distribution of S-w… Show more

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Cited by 40 publications
(31 citation statements)
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References 40 publications
(37 reference statements)
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“…This apparent mismatch may have its origin in (1) different resolution scales of the two methods and (2) the complex nature of the crust mantle boundary in the area under investigation, possibly leading to the existence of two Mohos ‐ a refraction Moho and a RF Moho. However, our results agree very well with the Moho depths obtained by Wilde‐Piórko et al [2005] using RF analysis at broadband stations within and around the Bohemian Massif. They obtained crustal thicknesses between 28 and 31 km at stations in the Saxothuringian unit.…”
Section: Discussion Of the Moho Depth Mapsupporting
confidence: 89%
“…This apparent mismatch may have its origin in (1) different resolution scales of the two methods and (2) the complex nature of the crust mantle boundary in the area under investigation, possibly leading to the existence of two Mohos ‐ a refraction Moho and a RF Moho. However, our results agree very well with the Moho depths obtained by Wilde‐Piórko et al [2005] using RF analysis at broadband stations within and around the Bohemian Massif. They obtained crustal thicknesses between 28 and 31 km at stations in the Saxothuringian unit.…”
Section: Discussion Of the Moho Depth Mapsupporting
confidence: 89%
“…Our model consists of nine layers with 20 (crustal layers) 60 (deepest mantle layer) km large horizontal blocks, enlarging with depth down to 380 km. The starting model is based on a 1‐D local crustal velocity model derived from Deep Seismic Sounding (DSS) measurements (Beránek & Zátopek 1981; Mayerová et al 1994; Hrubcová et al 2005) and receiver function methods (Geissler et al 2005; Wilde‐Piórko et al 2005), and the 1‐D IASP91 velocity distribution (Kennett & Engdahl 1991) just underneath. The smooth crustal model assumes average crustal velocity, depth of Moho, as well as thickness and average velocity of unconsolidated sediments.…”
Section: Tomographic Imaging Of the Upper Mantle Beneath The Bohemimentioning
confidence: 99%
“…Group, 1988;Behr et al, 1994;DEKORP and Orogenic Processes Working Groups, 1999;Tomek et al, 1997) as well as the refraction and wide-angle reflection experiments as GRANU'95 (Enderle et al, 1998), CELEBRATION 2000 with CEL09 profile (Hrubcová et al, 2005) or SUDETES 2003 with S01 profile (Grad et al, 2008). Passive seismic experiments with permanent and temporary seismic stations were carried out to study the major lithospheric discontinuities using the receiver function method (Geissler et al, 2005;Wilde-Piórko et al, 2005;Heuer et al, 2006). Different seismic methods, namely the receiver function and the refraction and wide-angle reflection measurements, sampled the crust-mantle boundary, which resulted in the interpretation of the depth and nature of this major discontinuity with respect to the method applied.…”
Section: Introductionmentioning
confidence: 99%