Association of Rayleigh Waves Using Backazimuth Measurements: Application to Test Ban Verification

The defining characteristic of a fundamental mode Rayleigh wave in a spherical, isotropic Earth is its elliptical polarization in the plane of propagation. Measurement of this polarization is thus critical both in identification and in determining the backazimuth of a Rayleigh wave from receiver to source and hence the association with a particular seismic disturbance. Currently, the prototype International Data Center (pIDC) and the International Data Center (IDC) measure backazimuth but do not utilize this in association because it is believed that measurement of backazimuth is unreliable. In this article, we demonstrate that an accurate measurement of backazimuth can be obtained for the large majority of Rayleigh waves reported in the bulletins of the pIDC/IDC. A reliable backazimuth measurement confirms the association of a waveform with a seismic disturbance, whereas the inclusion of large backazimuth errors in the bulletin can cast doubt on the association. Because the object of event screening is to positively identify earthquakes, it is vital that surface-wave magnitudes are only measured from positively identified and associated Rayleigh waves.

[1]  Frank L. Vernon,et al.  Frequency dependent polarization analysis of high‐frequency seismograms , 1987 .

[2]  Walter H. F. Smith,et al.  New, improved version of generic mapping tools released , 1998 .

[3]  F. Pollitz,et al.  Analysis of Rayleigh wave refraction from three‐component seismic spectra , 1993 .

[4]  M. Ritzwoller,et al.  The nature and cause of polarization anomalies of surface waves crossing northern and central Eurasia , 1994 .

[5]  K. L. McLaughlin,et al.  Improved Methods for Regionalized Surface Wave Analysis. , 1997 .

[6]  G. Masters,et al.  Frequency-dependent polarization measurements of long-period surface waves and their implications for global phase-velocity maps , 1994 .

[7]  R. A. Fowler,et al.  Polarization analysis of natural and artificially induced geomagnetic micropulsations , 1967 .

[8]  A. Dziewoński,et al.  A technique for the analysis of transient seismic signals , 1969 .

[9]  J. C. Samson,et al.  Descriptions of the Polarization States of Vector Processes: Applications to ULF Magnetic Fields , 1973 .

[10]  Jon Berger,et al.  Peculiarities of surface-wave propagation across central Eurasia , 1992, Bulletin of the Seismological Society of America.

[11]  Jeffry L. Stevens,et al.  Optimization of Surface Wave Identification and Measurement , 2001 .

[12]  J. C. Samson,et al.  Pure states, polarized waves, and principal components in the spectra of multiple, geophysical time-series , 1983 .

[13]  Roel Snieder,et al.  Time- and frequency-dependent polarization analysis: anomalous surface wave observations in Iberia , 1990 .

[14]  G. Masters,et al.  SURFACE-WAVE POLARIZATION DATA AND GLOBAL ANISOTROPIC STRUCTURE , 1998 .

[15]  Ernest R. Kanasewich,et al.  Enhancement of Teleseismic Body Phases with a Polarization Filter , 1970 .

[16]  J. C. Samson,et al.  Matrix and Stokes vector representations of detectors for polarized waveforms: theory, with some applications to teleseismic waves , 1977 .

[17]  J. Means Use of the three‐dimensional covariance matrix in analyzing the polarization properties of plane waves , 1972 .

[18]  Jeannot Trampert,et al.  Global phase velocity maps of Love and Rayleigh waves between 40 and 150 seconds , 1995 .

[19]  John H. Woodhouse,et al.  Mapping the upper mantle: Three‐dimensional modeling of earth structure by inversion of seismic waveforms , 1984 .

[20]  A. Jurkevics Polarization analysis of three-component array data , 1988 .

[21]  J. Woodhouse,et al.  GLOBAL HIGH-RESOLUTION PHASE VELOCITY DISTRIBUTIONS OF OVERTONE AND FUNDAMENTAL-MODE SURFACE WAVES DETERMINED BY MODE BRANCH STRIPPING , 1999 .

[22]  Jeroen Tromp,et al.  Measurements and global models of surface wave propagation , 1997 .

[23]  Eric P. Chael,et al.  An automated Rayleigh-wave detection algorithm , 1997, Bulletin of the Seismological Society of America.

[24]  K. Yoshizawa,et al.  Resolving power of surface wave polarization data for higher-order heterogeneities , 1999 .

[25]  G. Masters,et al.  Constraints on global phase velocity maps from long-period polarization data , 1996 .

[26]  R. S. Simons A surface wave particle motion discrimination process , 1968 .

[27]  G. Laske Global observation of off-great-circle propagation of long-period surface waves , 1995 .