Bulletin of the Seismological Society of America
HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
 QUICK SEARCH:   [advanced]


     


Bulletin of the Seismological Society of America; February 1996; v. 86; no. 1A; p. 144-158
© 1996 Seismological Society of America
This Article
Right arrow Full Text (PDF)
Right arrow References
Right arrow Citation Map
Services
Right arrow Email this article to a friend
Right arrow Similar articles in this journal
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Durek, J. J.
Right arrow Articles by Ekström, G.
Right arrow Search for Related Content
GeoRef
Right arrow GeoRef Citation

A radial model of anelasticity consistent with long-period surface-wave attenuation

Joseph J. Durek* and Göran Ekström

Department of Earth and Planetary Sciences, 20 Oxford St.Harvard University, Cambridge, Massachusetts 02138

Abstract

A new global model of radial variations in intrinsic shear and compressional attenuation, Qµ(r) and Q{kappa}(r), is presented. The model, called QL6, is derived from recent observations of long-period (150 < T < 300 sec) Rayleigh- and Love-wave attenuation and an extensive set of mode decay observations compiled from the literature. Our preferred model consists of six layers of constant Q, where the parameterization of Qµ(r) follows that of the anelastic component of the preliminary reference earth model (PREM). Relative to the commonly used models of PREM and QM1, lower values of Qµ are required in the upper 200 km of the mantle to explain observations of Love-wave attenuation. The observations require a finite level of compressional attenuation, preferentially located in the upper mantle. An analysis using continuous spline-basis functions supports the layered parameterization—with the recovered model possessing strong gradients in Qµ at the 670-km discontinuity; at the bottom of the asthenosphere; and to a lesser extent, at the base of the lithosphere. However, the continuous model does not have a significant discontinuity in Qµ at the 400-km phase boundary.

Footnotes

* Presently at Seismographic Station, 475 McCone Hall, University of California at Berkeley, Berkeley, California 94720.




This article has been cited by other articles:


Home page
Bulletin of the Seismological Society of AmericaHome page
The 14 November 2001 Kokoxili (Kunlunshan), Tibet, Earthquake: Rupture Transfer through a Large Extensional Step-Over
Bulletin of the Seismological Society of America, August 1, 2004; 94(4): 1173 - 1194.



Home page
Bulletin of the Seismological Society of AmericaHome page
M. Antolik and D. S. Dreger
Rupture Process of the 26 January 2001 Mw 7.6 Bhuj, India, Earthquake from Teleseismic Broadband Data
Bulletin of the Seismological Society of America, June 1, 2003; 93(3): 1235 - 1248.
[Abstract] [Full Text] [PDF]


Home page
Bulletin of the Seismological Society of AmericaHome page
Seismic Attenuation and Shallow Velocity Structures at Stromboli Volcano, Italy
Bulletin of the Seismological Society of America, April 1, 2002; 92(3): 1102 - 1116.



Home page
Bulletin of the Seismological Society of AmericaHome page
R. Arvidsson and G. Ekstrom
Global CMT analysis of moderate earthquakes, Mw greater double equals 4.5, using intermediate-period surface waves
Bulletin of the Seismological Society of America, August 1, 1998; 88(4): 1003 - 1013.
[Abstract] [PDF]




HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
Copyright © 1996 by the Seismological Society of America.