2015
DOI: 10.1007/s00024-015-1208-5
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Reason and Condition for Mode Kissing in MASW Method

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Cited by 50 publications
(17 citation statements)
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“…However, a visually continuous energy peak may shift from one mode to another at some frequencies. This phenomenon is called mode osculation (Boaga et al 2013) or mode kissing , and has recently been observed in a real-world example (Gao et al 2016). Because it is almost impossible to identify the conversion between different modes in a continuous energy peak by using one dispersion image alone, it is recommended to use multi-component data (Ikeda et al 2014;Dal Moro et al 2015 or to jointly use Rayleigh and Love-wave data (Gao et al 2016) to reduce the possibility in the misidentification of surface-wave dispersion curves.…”
Section: Maswmentioning
confidence: 99%
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“…However, a visually continuous energy peak may shift from one mode to another at some frequencies. This phenomenon is called mode osculation (Boaga et al 2013) or mode kissing , and has recently been observed in a real-world example (Gao et al 2016). Because it is almost impossible to identify the conversion between different modes in a continuous energy peak by using one dispersion image alone, it is recommended to use multi-component data (Ikeda et al 2014;Dal Moro et al 2015 or to jointly use Rayleigh and Love-wave data (Gao et al 2016) to reduce the possibility in the misidentification of surface-wave dispersion curves.…”
Section: Maswmentioning
confidence: 99%
“…Due to the 1D layered model and the plane wave assumptions involved in the forward calculation of surface-wave dispersion curves, however, methods based on dispersion curves fail to work when strong lateral heterogeneity exists, which is regarded as one of the limitations in MASW. Another problem faced with MASW is the difficulty in the correct estimation and identification of multimodal dispersion curves (Zhang and Chan 2003;Boaga et al 2013;Gao et al 2014), especially when encountering low-velocity layers (Tsuji et al 2012;Pan et al 2013a;Mi et al 2018), strong vertical contrasts (De Nil 2005;Renalier et al 2010;Gao et al 2016), and a non-planar free surface Wang et al 2015).…”
Section: Introductionmentioning
confidence: 99%
“…An inaccurate or erroneous experimental dispersion curve can cause substantial errors in the inverted shear wave velocity profile (Gao et al 2016;Park et al 1999;Zhang and Chan 2003).…”
Section: Challenges Associated With the Dispersion Analysis And Effecmentioning
confidence: 99%
“…However, in reality, surface wave registrations are incomplete to some extent, imposing various challenges when dispersion curves are identified based on a dispersion image. The fundamental mode of Rayleigh wave propagation typically prevails at sites where the stiffness (shear wave velocity) increases gradually with increasing depth (Foti et al 2015;Gao et al 2016;Gucunski and Woods 1991;Tokimatsu et al 1992). However, at sites characterized by a more irregularly varying stiffness profile, e.g., the presence of a stiff surface layer, a stiff layer sandwiched between two softer layers or a sudden increase in stiffness with depth, higher modes can play a significant role in certain frequency ranges.…”
Section: Challenges Associated With the Dispersion Analysis And Effecmentioning
confidence: 99%
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