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  • 1
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1996
    In:  Geophysical Research Letters Vol. 23, No. 16 ( 1996-08), p. 2037-2040
    In: Geophysical Research Letters, American Geophysical Union (AGU), Vol. 23, No. 16 ( 1996-08), p. 2037-2040
    Abstract: On December 28, 1994 a segment along the northern Japan trench failed in a M w =7.7 underthrusting earthquake, the Sanriku‐oki earthquake. Less than 30 years earlier, the great Tokachi‐oki underthrusting earthquake of May 16, 1968 (M w =8.2) occurred in the same region. We examine the rupture process of the recent event, using teleseismic body and surface wave data, and compare our results to the rupture characteristics of the Tokachi‐oki earthquake, as estimated by various authors in previous studies. We use an empirical Green’ function technique to obtain relative source time functions spanning a large range of the directivity parameter. The strong azimuthal dependence of the durations of these source time functions indicates a significant unilateral component of rupture in a down‐dip direction (west‐northwest). The main rupture initiated about 35 km southwest of the epicenter approximately 20 seconds after the onset of a low energy precursor. The main Tokachi‐oki rupture was also preceded by low moment release. However, it is unclear whether the low moment release preceding both earthquakes represents part of the rupture process or a distinct foreshock. The main rupture areas (asperities) of the Sanriku‐oki and the Tokachi‐oki earthquakes do not significantly overlap.
    Type of Medium: Online Resource
    ISSN: 0094-8276 , 1944-8007
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1996
    detail.hit.zdb_id: 2021599-X
    detail.hit.zdb_id: 7403-2
    SSG: 16,13
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  • 2
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1998
    In:  Geophysical Research Letters Vol. 25, No. 13 ( 1998-07), p. 2293-2296
    In: Geophysical Research Letters, American Geophysical Union (AGU), Vol. 25, No. 13 ( 1998-07), p. 2293-2296
    Abstract: The similarity of acoustic and seismic spectra recorded during Strombolian activity of Arenal Volcano provides conclusive evidence that pressure waves are generated and propagated within the magma‐gas mixture inside volcanic conduits. These pressure waves are sensitive to the flow velocity and to small changes in the gas content of the magma‐gas mixture, and thus can provide useful indicators of the time‐varying properties of the unsteady flow regime and the chemical composition of the melt. The dominant features of the observed explosion and tremor signals are attributed to the source excitation functions and the acoustic resonance of a magma‐gas mixture inside the volcanic conduit. We postulate that explosions are triggered in the shallow parts of the magma conduit, where a drastic pressure drop with depth creates a region where violent degassing can occur. Tremor may be sustained by unsteady flow fluctuations at depth. Equilibrium degassing of the melt creates a stable, stratified magma column where the void fraction increases with decreasing depth. Disruption of this equilibrium stratification is thought to be responsible for observed variations in the seismic efficiency of explosions and enhanced acoustic transmission from the interior of the conduit to the atmosphere.
    Type of Medium: Online Resource
    ISSN: 0094-8276 , 1944-8007
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1998
    detail.hit.zdb_id: 2021599-X
    detail.hit.zdb_id: 7403-2
    SSG: 16,13
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  • 3
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1997
    In:  Geophysical Research Letters Vol. 24, No. 1 ( 1997-01), p. 9-12
    In: Geophysical Research Letters, American Geophysical Union (AGU), Vol. 24, No. 1 ( 1997-01), p. 9-12
    Abstract: We report low average crustal P‐wave velocities (5.9–6.1 km/s, Poisson's ratio 0.23‐0.27, thickness 68–76 km) in southern Tibet from modelling regional Pnl waveforms recorded by the 1991–1992 Tibetan Plateau Experiment. We also find that the mantle lithosphere beneath the Indus‐Tsangpo Suture and the Lhasa Terrane is shield‐like (Pn velocity 8.20–8.25 km/s, lid thickness 80–140 km, positive velocity gradient 0.0015–0.0025 s −1 ). Analysis of relative Pn travel time residuals requires a decrease in the mantle velocities beneath the northern Lhasa Terrane, the Banggong‐Nujiang Suture and the southern Qiangtang Terrane. Tectonic and petrologic considerations suggest that low bulk crustal velocities could result from a thick (50–60 km) felsic upper crust with vertically limited and laterally pervasive partial melt. These results are consistent with underthrusting of Indian Shield lithosphere beneath the Tibetan Plateau to at least the central Lhasa Terrane.
    Type of Medium: Online Resource
    ISSN: 0094-8276 , 1944-8007
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1997
    detail.hit.zdb_id: 2021599-X
    detail.hit.zdb_id: 7403-2
    SSG: 16,13
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  • 4
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1996
    In:  Journal of Geophysical Research: Solid Earth Vol. 101, No. B7 ( 1996-07-10), p. 16043-16058
    In: Journal of Geophysical Research: Solid Earth, American Geophysical Union (AGU), Vol. 101, No. B7 ( 1996-07-10), p. 16043-16058
    Abstract: The April 25, 1992, Cape Mendocino earthquake ( M S 7.1) has renewed speculation about the nature of subduction along the Cascadia subduction zone and the associated seismic hazard. This event may represent the first large ( M 〉 6) thrust event along the entire Cascadia subduction zone in historic times (last 200 years). We analyze long‐period surface waves and broadband body waves in order to estimate the mainshock source parameters. We also examine broadband body waves from the nearby 1991 Honeydew earthquake ( M 6) in order to assess the contributions of both rupture complexity and unmodeled source and receiver structure in the Cape Mendocino waveforms. From both body and surface wave inversions, as well as forward modeling of body waves, we estimate a best double couple mechanism for the Cape Mendocino earthquake (strike = 330 ± 10°, dip = 12 ± 2°, rake = 75 ± 15°, seismic moment = 1.93 × 10 19 N m, and M w = 6.8). This mechanism contains a significant component of slip in the estimated direction of Gorda‐North America plate convergence. Although this earthquake had suitable geometry for relieving strain accumulated by Gorda‐North America plate convergence, we cannot resolve whether it occurred on the interplate megathrust or on a fault within the overriding accretionary prism. We find evidence for southwest (offshore) rupture toward an azimuth of 240°. In addition, we find evidence for early aftershocks in both the teleseismically recorded body waves and in locally recorded strong motions. We model one aftershock delayed ∼13 s from the mainshock with a mechanism that is different from the mainshock mechanism but is consistent with the north‐south trending, horizontal compression found offshore within the Gorda plate. We postulate that this aftershock and two additional large, strike‐slip aftershocks that ruptured the Gorda plate within 24 hours of the mainshock were caused by the transfer of stress accumulated across the Cascadia subduction zone and accretionary prism far offshore, to the Gorda plate, where it reduced the normal stress across NW‐SE oriented faults, triggering failure. The complexity of fault interactions near the Mendocino triple junction needs to be understood before potential seismic hazards of the southern Cascadia subduction zone can be quantified.
    Type of Medium: Online Resource
    ISSN: 0148-0227
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1996
    detail.hit.zdb_id: 161666-3
    SSG: 16,13
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  • 5
    Online Resource
    Online Resource
    Seismological Society of America (SSA) ; 1996
    In:  Bulletin of the Seismological Society of America Vol. 86, No. 3 ( 1996-06-01), p. 655-669
    In: Bulletin of the Seismological Society of America, Seismological Society of America (SSA), Vol. 86, No. 3 ( 1996-06-01), p. 655-669
    Abstract: A rectangular (4 by 5) array of short-period three-component seismometers with 15-m spacing was deployed to record several U.S. Geological Survey calibration explosions detonated around the Santa Cruz Mountains. The array was located at a site where an earlier station had recorded frequency-dependent polarized site resonances for aftershocks of the 1989 Loma Prieta earthquake. The site is on a hillside believed to be a landslide structure, with the near surface consisting of poorly sorted sediments and weathered rocks with dipping subsurface layers. The primary objective was to explore the site effects in this complex three-dimensional soft-rock environment, characteristic of much of the Loma Prieta source region. The direct P waves from four nearby (15 to 20 km) explosions at easterly azimuths from the array show counterclockwise arrival azimuth anomalies of 30° to 50°. These deflections are attributed to the presence of more than one dipping velocity contrast beneath the array, with dips of from 10° to 50° and dip directions generally toward the south. One such boundary may correspond to the landslide slip surface, and the presence of dipping velocity contrasts underlying the site is probably responsible for some of the observed directional site resonance. A slowness vector analysis demonstrates that arrivals early in the P coda have similar azimuthal anomalies, while later scattered arrivals come from many azimuths. Particle motions indicate that the more coherent arrivals in the coda are comprised of scattered P waves and Rayleigh waves, probably associated with scattering from the rough topography in the region. The coda displays greater spatial coherency along the hill strike than down the slope, consistent with a wedge-shaped landslide. The overall wave-field spatial coherence, CCC(f, Δx), decreases with increasing frequency, f, and spatial offset, Δx, and on average can be well represented by CCC(f, Δx) = e−cfΔx, with c = 0.6 km−1 Hz−1 for the vertical P wave in the first 1-sec window. This behavior is comparable to that found for previously studied hard-rock locations.
    Type of Medium: Online Resource
    ISSN: 1943-3573 , 0037-1106
    Language: English
    Publisher: Seismological Society of America (SSA)
    Publication Date: 1996
    detail.hit.zdb_id: 419141-9
    detail.hit.zdb_id: 2065447-9
    SSG: 16,13
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  • 6
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1998
    In:  Journal of Geophysical Research: Solid Earth Vol. 103, No. B4 ( 1998-04-10), p. 7137-7152
    In: Journal of Geophysical Research: Solid Earth, American Geophysical Union (AGU), Vol. 103, No. B4 ( 1998-04-10), p. 7137-7152
    Abstract: We report models of P and S wave velocity and attenuation for the the crust and uppermost mantle of the Qiangtang Terrane, northern Tibetan Plateau, inferred by fitting reflectivity synthetic seismograms to observed complete regional waveforms. The data are three‐component broadband seismograms recorded by the 1991–1992 IRIS‐PASSCAL (Incorporated Research Institutions for Seismology‐Program for Array Seismic Studies of the Continental Lithosphere) Tibetan Plateau Experiment and Global Seismic Network stations in the region. The Qiangtang Terrane has thick crust (65±5 km) with P and S wave velocities of 6.1–6.3 and 3.34–3.43 km/s, respectively, yielding an anomalously high crustal Poisson's ratio of 0.29±0.02. Seismic velocities of the upper mantle of the Qiangtang Terrane are normal for P waves and slow for S waves (8.10 and 4.35–4.41 km/s, respectively) with a high mantle Poisson's ratio of 0.29±0.01. Attenuation in the crust and upper mantle is high ( Q P = 100–200 and Q S = 44–89). Modeling of the broadband P waveforms suggests that a decrease in mantle velocity occurs at about 160 km depth in the mantle; however, this is not unambiguously supported by the data and modeling. The crust and uppermost mantle of the Qiangtang Terrane probably contains partial melt based on the high Poisson's ratio, low shear wave velocities, and low Q . The absence of high‐frequency S n and the presence of volcanism of mantle lithospheric origin support the presence of partial melt. Crustal and uppermost mantle structure in the Qiangtang Terrane is different from that for the Lhasa Terrane (immediately to the south) based on results of our previous studies. The average crustal P and S wave velocities are 4% faster and 2% slower, respectively, in the Qiangtang Terrane relative to the Lhasa Terrane. This yields a significant difference in the crustal Poisson's ratio with values of 0.29 for the Qiangtang Terrane and 0.25 for the Lhasa Terrane. Differences in the uppermost mantle P and S wave velocities and Poisson's ratios of these two adjacent terranes cannot be explained by temperature differences alone. Using the mantle temperature estimates of McNamara et al. . [1997] we suggest that partial melt of an ultramafic composition beneath the Qiangtang Terrane fits the velocity and Poisson's ratio estimates.
    Type of Medium: Online Resource
    ISSN: 0148-0227
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1998
    detail.hit.zdb_id: 161666-3
    SSG: 16,13
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  • 7
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1997
    In:  Geophysical Research Letters Vol. 24, No. 10 ( 1997-05-15), p. 1263-1266
    In: Geophysical Research Letters, American Geophysical Union (AGU), Vol. 24, No. 10 ( 1997-05-15), p. 1263-1266
    Abstract: Focal mechanisms of 70 earthquakes occurring in the region of the Mendocino triple junction between 1977 and 1995 are inverted to obtain the regional stress orientations and relative magnitudes in this technically complex area. A diverse set of earthquake geometries is consistent with a single stress field characterized by north‐northwest, horizontal, maximum principal compressive stress. Although this stress direction is almost perpendicular to convergence between the North American and Gorda plates, it is consistent with the stress direction inferred within the Gorda plate northwest of the triple junction. A maximum compressive stress direction nearly parallel to strike of the Cascadia subduction zone implies very low resolved shear stress across this plate boundary. Evidence for failure along the southernmost section of the Cascadia subduction zone comes from the occurrence of the recent 1992 (Ms=7.1) Cape Mendocino underthrusting earthquake as well as from measurements of Holocene surface uplift consistent with the 1992 coseismic uplift pattern. Rupture of the Cascadia subduction zone under this stress regime requires that the southernmost region of the Gorda‐North American Plate boundary is weak.
    Type of Medium: Online Resource
    ISSN: 0094-8276 , 1944-8007
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1997
    detail.hit.zdb_id: 2021599-X
    detail.hit.zdb_id: 7403-2
    SSG: 16,13
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  • 8
    Online Resource
    Online Resource
    American Geophysical Union (AGU) ; 1999
    In:  Journal of Geophysical Research: Solid Earth Vol. 104, No. B10 ( 1999-10-10), p. 23111-23125
    In: Journal of Geophysical Research: Solid Earth, American Geophysical Union (AGU), Vol. 104, No. B10 ( 1999-10-10), p. 23111-23125
    Abstract: The last few years have been remarkable with respect to the number of large underthrusting earthquakes in subduction zones that reruptured plate boundary segments that failed in previous great events. Availability of modern seismic data for two consecutive large earthquakes rupturing the same portion of the plate interface provides the opportunity to compare the spatial distribution of moment release for both events. Such comparisons have been made for the plate boundary segments that failed in (1) the 1957 ( M w = 8.6), 1986 ( M w = 8.0), and 1996 ( M w = 7.9) Aleutian Islands earthquakes; (2) the 1963 ( M w = 8.5) and 1995 ( M w = 7.9) Kuril Islands earthquakes; (3) the 1971 ( M w = 8.0) and 1995 ( M w = 7.7) Solomon Islands earthquakes; and (4) the 1968 ( M w = 8.2) and 1994 ( M w = 7.7) northern Honshu earthquakes. The spatial distribution of moment release for all four of the initial great earthquakes and two of the repeat events has been determined in previous studies. Here, slip distributions for the three most recent events are determined from inversion of source time functions, derived by empirical Greens function analysis of long‐period surface waves and broadband body waves. Comparisons of the spatial distribution of moment release for sequential earthquake ruptures reveal considerable differences in the pattern of recurrent fault slip. The 1994 northern Honshu and 1995 Solomon Islands earthquakes primarily fill in areas of slip deficit left by their preceding events rather than rerupture identical asperities. The 1995 Kuril Islands and the 1996 Aleutian Islands earthquakes both rerupture portions of an asperity distribution defined by preceding events but with variable amounts of slip. This study provides the first direct evidence that recurrence of large circum‐Pacific plate boundary events is more complex than repeat rupture of dominant asperities. Recurrent fault slip for the four plate boundary segments studied does not support characteristic slip models either where failure on an entire fault segment occurs repeatedly in events with nearly identical rupture lengths, locations, and slip magnitudes or where failure of individual asperities occurs with identical slip functions through consecutive earthquake cycles. These sequential slip patterns are not consistent with physical models of earthquake rupture where slip complexity is exclusively controlled by invariant geometric and/or material heterogeneity but suggest that dynamic considerations are also important.
    Type of Medium: Online Resource
    ISSN: 0148-0227
    Language: English
    Publisher: American Geophysical Union (AGU)
    Publication Date: 1999
    detail.hit.zdb_id: 161666-3
    SSG: 16,13
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  • 9
    Online Resource
    Online Resource
    Seismological Society of America (SSA) ; 1995
    In:  Bulletin of the Seismological Society of America Vol. 85, No. 6 ( 1995-12-01), p. 1560-1575
    In: Bulletin of the Seismological Society of America, Seismological Society of America (SSA), Vol. 85, No. 6 ( 1995-12-01), p. 1560-1575
    Abstract: Source parameters of aftershocks of the 22 April 1991 (MW = 7.7) Costa Rica and the 25 April 1992 (MW = 7.1) Cape Mendocino, California, earthquakes are determined using a grid search inversion of P, SH, and SV amplitude ratios recorded by sparse local networks of three-component broadband and short-period stations. The inversion procedure consists of computing synthetic seismograms for three fundamental fault orientations for all source-receiver pairs over a range of source depths; calculating the complex envelopes of the observed and synthetic seismograms to determine peak amplitudes of P, SH, and SV waves; combining the fundamental fault amplitudes for all possible values of strike, dip, and rake, at 10° increments; and determining the best fault orientation and depth as the one that yields the smallest misfit between observed and synthetic P/SH, P/SV, and SV/SH amplitude ratios. The ambiguity in the sense of motion on the nodal planes, arising due to the use of amplitude ratios, is resolved by examining P-wave polarities. The sensitivity of source parameters to uncertainties in earthquake location and crustal structure is explored. For events with good station coverage, focal mechanism determinations are stable for a wide range of assumed values of crustal structure, earthquake location, and depth. Source parameters for many of the largest events (M & gt; 3.4) are also determined by inversion of broadband displacement waveforms using a similar grid-search technique. Comparable results were obtained using both broadband waveforms and amplitude ratios. Focal mechanism solutions for 20 aftershocks of the Costa Rica earthquake reveal a complicated faulting geometry, indicating active thrust, normal, and strike-slip faults in the back-arc of Costa Rica. The 1992 Cape Mendocino earthquake occurred at the intersection of the North American, Gorda, and Pacific plates. While the mainshock was associated with underthrusting of the Gorda plate beneath the North American plate, fault plane solutions for 70% of the 38 largest aftershocks indicate that these events result from either motion between the Gorda and Pacific plates or from internal deformation within the Gorda plate.
    Type of Medium: Online Resource
    ISSN: 1943-3573 , 0037-1106
    Language: English
    Publisher: Seismological Society of America (SSA)
    Publication Date: 1995
    detail.hit.zdb_id: 419141-9
    detail.hit.zdb_id: 2065447-9
    SSG: 16,13
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  • 10
    Online Resource
    Online Resource
    Seismological Society of America (SSA) ; 1996
    In:  Bulletin of the Seismological Society of America Vol. 86, No. 1A ( 1996-02-01), p. 19-31
    In: Bulletin of the Seismological Society of America, Seismological Society of America (SSA), Vol. 86, No. 1A ( 1996-02-01), p. 19-31
    Abstract: We have imaged the complex crustal and upper mantle structure beneath central Costa Rica using P-wave arrival times from locally recorded earthquakes. Thurber's (1983) iterative inversion method is used to simultaneously estimate velocities along a three-dimensional grid and hypocentral parameters of local earthquakes. Our data consist of over 12,000 arrival times from more than 1300 earthquakes recorded by stations of a permanent seismographic network in Costa Rica. Our resulting velocity model correlates well with mapped geologic units at very shallow depth and with tectonic features at greater depth. We find low velocities (4.0 to 4.8 km/sec) in the shallow crust (above 10 km) near the active volcanoes and associated with a NW-SE trending late Cretaceous to late Tertiary sedimentary basin southeast of Herradura peninsula. High velocities (5.4 to 5.7 km/sec) in the shallow crust correlate with outcrops of late Jurassic to early Tertiary ultramafic ophiolitic units and with basic Tertiary volcanic units. At depths between 20 and 30 km, high velocities (6.8 to 7.2 km/sec) are associated with the subducting Cocos plate under Costa Rica and two prominent low-velocity bodies (6.3 to 6.5 km/sec) are present about 30 km trenchward of the volcanic arc and along the projection of the aseismic Cocos Ridge as it subducts beneath Costa Rica. The thickened oceanic crust of the Cocos Ridge is most likely responsible for its low velocities. The deep low-velocity anomaly located trenchward of the axis of the volcanoes may indicate the presence of a low-density intrusive resulting from an earlier phase of magmatism, possibly the late Miocene episode that produced the Talamanca intrusive complex.
    Type of Medium: Online Resource
    ISSN: 1943-3573 , 0037-1106
    Language: English
    Publisher: Seismological Society of America (SSA)
    Publication Date: 1996
    detail.hit.zdb_id: 419141-9
    detail.hit.zdb_id: 2065447-9
    SSG: 16,13
    Location Call Number Limitation Availability
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