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  • 1
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    In:  Geophys. Res. Lett., Berlin, Schweizerbart'sche Verlagsbuchhandlung, vol. 28, no. 23, pp. 4379-4382, pp. L07302, (ISSN 0016-8548, ISBN 3-510-50045-8)
    Publication Date: 2001
    Keywords: Earthquake ; Source ; China ; Tectonics ; GRL ; 1242 ; Geodesy ; and ; gravity ; Seismic ; deformations ; (7205) ; 7215 ; Seismology ; Earthquake ; parameters
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  • 2
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    In:  Bull. Seism. Soc. Am., Berlin, Schweizerbart'sche Verlagsbuchhandlung, vol. 92, no. 4, pp. 1192-1207, pp. L07302, (ISSN 0016-8548, ISBN 3-510-50045-8)
    Publication Date: 2002
    Keywords: Seismology ; Earthquake ; USA ; Wavelet processing ; BSSA
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  • 3
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    In:  Bull. Seism. Soc. Am., Berlin, Schweizerbart'sche Verlagsbuchhandlung, vol. 92, no. 4, pp. 1208-1226, pp. L07302, (ISSN 0016-8548, ISBN 3-510-50045-8)
    Publication Date: 2002
    Keywords: Seismology ; Earthquake ; USA ; Source ; Fracture ; BSSA
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  • 4
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    In:  Bull. Seism. Soc. Am., Luxembourg, Conseil de l'Europe, vol. 84, no. 5, pp. 1310-1326, pp. 1006, (ISSN: 1340-4202)
    Publication Date: 1994
    Keywords: Synthetic seismograms ; USA ; Modelling ; Site amplification ; Multiples ; BSSA ; SRICHWALSKI
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  • 5
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    In:  Science, Kunming, China, 3-4, vol. 281, no. 5380, pp. 1170-1172, pp. L07316, (ISSN: 1340-4202)
    Publication Date: 1998
    Keywords: Deep seismic sounding (espec. cont. crust) ; China ; CRUST ; earth mantle
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  • 6
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    In:  J. Geophys. Res., Hannover, D. Reidel Publishing Company, vol. 103, no. B11, pp. 17901-17918, pp. L09303, (ISSN: 1340-4202)
    Publication Date: 1998
    Keywords: Two-dimensional ; Body waves ; combination ; Synthetic seismograms ; Seismology ; JGR
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  • 7
    Publication Date: 2019
    Description: Abstract The 2010 MW 7.2 El Mayor‐Cucapah earthquake ruptured a zone of ~120 km in length in northern Baja California. The geographic distribution of this earthquake sequence was well constrained by waveform relocation. The depth distribution, however, was poorly determined as it is near the edge of, or outside, the Southern California Seismic Network. Here we use two complementary methods to constrain the focal depths of moderate‐sized events (M ≥ 4.0) in this sequence. We first determine the absolute earthquake depth by modeling the regional depth phases at high frequencies (~1 Hz). We mainly focus on Pn and its depth phases pPn and sPn, which arrive early at regional distance and are less contaminated by crustal multiples. To facilitate depth phase identification and to improve signal‐to‐noise ratio, we take advantage of the dense Southern California Seismic Network and use array analysis to align and stack Pn waveforms. For events without clear depth phases, we further determine their relative depths with respect to those with known depths using differential travel times of the Pn, direct P, and direct S phases recorded for event pairs. Focal depths of 93 out of 122 M ≥ 4.0 events are tightly constrained with absolute uncertainty of about 1 km. Aftershocks are clustered in the depth range of 3–10 km, suggesting a relatively shallow seismogenic zone, consistent with high surface heat flow in this region. Most aftershocks are located outside or near the lower terminus of coseismic high‐slip patches of the main shock, which may be governed by residual strains, local stress concentration, or postseismic slip.
    Print ISSN: 2169-9313
    Electronic ISSN: 2169-9356
    Topics: Geosciences , Physics
    Published by Wiley on behalf of American Geophysical Union (AGU).
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  • 8
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 125 (1996), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: Three-component broad-band displacement seismograms with paths sampling the Basin and Range province are studied to constrain the crustal structure. to find an average model that fits the data in both absolute time and waveform, we generate broad-band reflectivity synthetics and conduct sensitivity tests on different parts of a layered crustal model, where only a few layers are involved. Generalized rays are used to help identify the various phases. It proves useful to decompose a regional seismogram into segments so that the impact of model parameters on each segment can be clearly identified. Thus, for mid-crustal earthquakes, it is established that the top crustal layer controls the Rayleigh wave, the Airy phase, in shape over the range from 300 to 600 km, and the crustal layer just above the source depth controls its timing. the Pn waves, the Pn and PL portion, are controlled in broad-band character by the mid-crust while the top layer contributes to their long-period motion. These crustal parameters control the tangential motion similarly. the SV wave, the segment between the Pn wave and the Rayleigh wave, is mostly controlled by the shear velocity of the lower crust. In judging the goodness of fit between the array observations and synthetic waveforms, we allow individual data segments to shift relative to the 1-D synthetics by a few seconds to account for some lateral variation. the amount of time shift is found by the cross-correlation in displacement between the data segment and the synthetics. Applying these tests in a forward modelling approach, we find that a simple two-layer crustal model is effective in explaining this data set. In this model, the main crustal layer has P and S velocities of 6.1 km s-1 and 3.6 km s-1, similar to those found by Langston & Helmberger (1974). A surface layer of thickness 2.5 to 3.5 km is required to fit the Rayleigh waves. the refined model can be used as a reference model for further studies in this region.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 105 (1991), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: This paper addresses the velocity structure of the crust and upper mantle beneath southern China with special emphasis on the Tibet region. Waveform data from 48 earthquakes as recorded on the WWSSN and GDSN are used in this detailed forward modelling study. Constraints on the upper crustal section are derived from modelling local Love waves in the time domain applying the mode-sum modelling technique. Lower crustal constraints are derived by modelling the Pnl-wavetrain with the reflectivity method. An average crustal thickness of 70 km is obtained beneath the Tibetan Plateau with a modest increase of velocity with depth. The lithospheric and upper mantle structure is deduced from modelling S and SS triplication waveform data and relative traveltimes by applying a combination of WKBJ and generalized ray methods. S-SS seismograms chosen with bounce-points directly under Tibet allow remote sensing of this inaccessible region. The resulting model is an averaged 1-D model where corrections for lateral variation have been applied. We conclude that the upper mantle structure in the entire region is basically shield-like below 200 km (SNA). However, the velocity of the lithosphere is abnormally slow, roughly 5 per cent beneath Tibet. The model for Tibet derived does not have a distinct lid, and has a positive velocity gradient in the crust, suggesting crustal shortening. A preliminary velocity model for southeastern China is also suggested.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 105 (1991), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: The Saguenay earthquake, 1988 November 25, is one of the first large shield type events recorded by a broadband-high dynamic range instrument, the Streckeisen system, installed at Harvard station (HRV). The event is sufficiently large to be well recorded teleseismically and thus the source characteristics can be determined by independent means and considered known. This allows a detailed study of the propagational effects along this path, at an epicentral distance of 625 km, where the strengths of the surface waves can be compared with the crustal body phases. Broadband modelling using standard analytical techniques and flat layered models works amazingly well over the period range of 0.5–20 s. A detailed strategy for modelling broadband regional phases is given in terms of a decomposition of the vertical and radial seismograms into three segments: Pnl (containing Pn, pPn, sPn, PmP, P coupled PL-waves); Snl (containing Sn, sSn, SmS, etc.); and the fundamental Rayleigh waves. Information about the upper crust is obtained from the fundamental Rayleigh waves while crustal thickness and velocity gradients in the mantle are obtained from Pnl and Snl. This particular crustal model has a thickness of 35 km with a sharp Moho and a substantial gradient in the top 20 km of the mantle, 0.01 km s−1 per km for both P and S velocities. The mantle velocities, α= 8.2 and β= 4.55 km s−1 are slower than expected for a shield environment. Attenuation is not required for waveform modelling or for absolute amplitude estimation.
    Type of Medium: Electronic Resource
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