@article{oai:nagoya.repo.nii.ac.jp:02001363,
 author = {Kumagai, Hiroyuki and Torres, Roberto and Maeda, Yuta},
 issue = {11},
 journal = {Journal of Geophysical Research: Solid Earth},
 month = {Nov},
 note = {Seismic scattering and attenuation at volcanoes, thought to be strongest on the Earth, can be used to map volcanic feeding systems. We systematically analyzed high-frequency (5–10 Hz) seismograms of volcano-tectonic earthquakes at Galeras volcano (Colombia) and active sources at Kirishima, Unzen, Bandai, and Iwate volcanoes (Japan) to investigate their scattering and attenuation characteristics. The envelope widths estimated from these seismograms were compared with those calculated by Monte Carlo envelope simulations for 1D layered models parameterized by the scattering mean free path and the quality factor of medium attenuation for S waves. Our results indicated a surficial, highly heterogeneous, and attenuative layer up to around 1 km thickness at all studied volcanoes. The strongest heterogeneities at volcanoes thus exist in a thin surface layer, likely comprising unconsolidated and/or highly fractured materials. Using the space-weighting function for diffusive wavefields, we mapped the residuals between observed envelope widths and those calculated with our estimated 1D models at Kirishima, Unzen, Bandai, and Iwate. These maps showed spatial distributions of the envelope-width residuals were unique to each volcano and correlated with P wave velocity tomographic images. Areas of positive residuals correspond to low-velocity anomalies and thus to heterogeneous, strongly scattering rocks, whereas areas of negative residuals correspond to high-velocity anomalies and thus less heterogeneous volcanic or basement rocks. Our results demonstrate that envelope widths can improve the characterization of scattering and attenuation structures beneath volcanoes.},
 title = {Scattering and Attenuation Characteristics at Volcanoes Inferred From Envelope Widths of Natural and Active Seismic Sources},
 volume = {125},
 year = {2020}
}