Pre-S observations at station SLK, NW of Long Valley caldera, California, and their relation to possible magma bodies

1989 ◽  
Vol 79 (6) ◽  
pp. 1894-1904
Author(s):  
William A. Peppin ◽  
Thomas W. Delaplain ◽  
J. Scott Lewis

Abstract The authors describe and catalog 280 observations of a seismic phase taken at the single station SLK, NW of Long Valley caldera. These observations are observed to precede S by a more or less constant 1.6 sec in the distance range 30 to 90 km, and are closely fit by the least-squares line TSLK = (0.2853 ± 0.0009)Δ − (0.9029 ± 0.052). These observations can only be explained in terms of laterally heterogeneous velocity structure near the caldera. The model proposed here—that these so-called “SLK phases” result from an S-to-P conversion across a dipping planar structure NW of the caldera in the vicinity of Inyo Craters—fits not only these observations, but is consistent with the data presented in two recent papers (Luetgert and Mooney, 1985; Zucca et al., 1987). On the other hand, the data presented here are inconsistent with the models proposed by those authors involving deep reflections from magma bodies associated with the caldera. Furthermore, these observations are not related to the magma bodies within the caldera proposed by Sanders (1984), as suggested in previous abstracts. The original vertical-component observations at SLK are supplemented by three-component observations obtained on a small (several hundred meters aperture) array near SLK, which identify the SLK phase unambiguously as having longitudinal particle motion, consistent with the proposal that it is a S-to-P conversion occurring NW of the caldera boundary.

1993 ◽  
Vol 98 (B11) ◽  
pp. 19869-19879 ◽  
Author(s):  
Arturo E. Romero ◽  
Thomas V. McEvilly ◽  
Ernest L. Majer ◽  
Alberto Michelini

2019 ◽  
Vol 220 (3) ◽  
pp. 1677-1686 ◽  
Author(s):  
Janire Prudencio ◽  
Michael Manga

SUMMARY Unrest at Long Valley caldera (California) during the past few decades has been attributed to the ascent of hydrothermal fluids or magma recharge. The difference is critical for assessing volcanic hazard. To better constrain subsurface structures in the upper crust and to help distinguish between these two competing hypotheses for the origin of unrest, we model the 3-D seismic attenuation structure because attenuation is particularly sensitive to the presence of melt. We analyse more than 47 000 vertical component waveforms recorded from January 2000 through November 2016 obtained from the Northern California Earthquake Data Center. We then inverted the S-to-coda energy ratios using the coda normalization method and obtained an average Q of 250. Low attenuation anomalies are imaged in the fluid-rich western and eastern areas of the caldera, one of which corresponds to the location of an earthquake swarm that occurred in 2014. From a comparison with other geophysical images (magnetotellurics, seismic tomography) we attribute the high attenuation anomalies to hydrothermal systems. Average to high attenuation values are also observed at Mammoth Mountain (southwest of the caldera), and may also have a hydrothermal origin. A large high attenuation anomaly within the caldera extends from the surface to the depths we can resolve at 9 km. Shallow rocks here are cold and this is where earthquakes occur. Together, these observations imply that the high attenuation region is not imaging a large magma body at shallow depths nor do we image any isolated high attenuation bodies in the upper ≈8 km that would be clear-cut evidence for partially molten bodies such as sills or other magma bodies.


2005 ◽  
Author(s):  
John W. Ewert ◽  
Christopher J. Harpel ◽  
Suzanna K. Brooks

2017 ◽  
Author(s):  
Graham D.M. Andrews ◽  
◽  
Abigail E. Martens ◽  
William Krugh ◽  
Sarah R. Brown

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