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Shear wave splitting

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similar waveforms. The Shear wave splitting varies with both incidence angle and propagation azimuth. Unless this data is viewed in polar projection, the 3-D nature is not reflected and may be misleading. Shear wave splitting may be caused by more than just one layer that is anisotropic and located anywhere between the source and the receiver station. The shear wave splitting measurements have extensive lateral resolution but very poor vertical resolution. The polarizations of shear waves vary throughout the rock mass. Therefore, the observed polarizations may be those of the near surface structure and are not necessarily representative of the structure of interest.
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liquid, the particles are much less tightly bound and it generally takes a longer time for the energy to be transmitted. This is because the particles have further to travel to transfer the energy from one to another. If a shear wave is polarized parallel to the cracks in this anisotropic medium, then it may look like the dark blue wave in Figure 4. This wave is acting on the particles like energy being transferred through a solid. It will have a high velocity because of the proximity of the grains to each other. If there is a shear wave that is polarized perpendicular to the liquid-filled cracks or elongated
1451: 531:. He reviewed the current theory, updated equations to better understand shear-wave splitting, and presented a few new concepts. Crampin established that the solution to most anisotropic problems can be developed. If a corresponding solution for an isotropic case can be formulated, then the anisotropic case can be arrived at with more calculations. The correct identification of body and surface wave polarizations is the key to determining the degree of anisotropy. The modeling of many two-phase materials can be simplified by the use of anisotropic 1965:{\displaystyle {\begin{cases}N_{j}\left(U^{\left(n\right)}\right)=\Gamma _{jk}U_{k}^{\left(n\right)}-U_{j}^{\left(n\right)}\\M_{j}\left(U^{\left(n\right)}\right)=p_{i}~a_{ijkl}{\frac {\partial U_{k}^{\left(n\right)}}{\partial x_{l}}}+\rho ^{-1}{\frac {\partial }{\partial x_{i}}}\left(\rho ~a_{ijkl}~p_{l}U_{k}^{\left(n\right)}\right)\\L_{j}\left(U^{\left(n\right)}\right)=\rho ^{-1}{\frac {\partial }{\partial x_{i}}}\left(\rho ~a_{ijkl}{\frac {\partial U_{k}^{\left(n\right)}}{\partial x_{l}}}\right)\end{cases}}} 571:. The energy would be transferred more slowly through the medium and the velocity would be slower than the first shear wave. The time delay between the shear wave arrivals depends on several factors including the degree of anisotropy and the distance the waves travel to the recording station. Media with wider, larger cracks will have a longer time delay than a media with small or even closed cracks. Shear wave splitting will continue to occur until the shear-wave velocity anisotropy reaches about 5.5%. 40: 3901:
isotropic medium (green). This single incident shear wave splits into two shear waves (orange and purple) upon entering the anisotropic media (red). The faster shear wave is oriented parallel to the cracks or crystals in the medium. The arrivals of the shear waves are shown on the right, as they appear at the recording station. The north–south polarized shear wave arrives first (purple) and the east–west polarized shear wave (orange) arrives about a second later.
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10, they sent another email specifying that an earthquake was likely to occur within the next 5 months. Three days later, on November 13, IMO reported a magnitude 5 earthquake near the BJA station. Crampin et al. suggests that this is the first scientifically, as opposed to precursory or statistically, predicted earthquake. They proved that variations of shear-wave splitting can be used to forecast earthquakes.
4252:, they write very complicated signatures. Polarizations and time delays are heavily scattered and vary greatly both in time and space. Because of the variation in signature, it is easy to misinterpret the arrivals and polarization of incoming shear waves. Below is an explanation of a few of the common misunderstandings associated with shear waves, further information can be found in Crampin and Peacock (2008). 524:. Because shear wave splitting signatures are dependent on both the orientation of the microcracks (perpendicular to the dominant stress direction) and the abundance of cracks, the signature will change over time to reflect the stress changes in the area. Once the signatures for an area are recognized, they may then be applied to predict nearby earthquakes with the same signatures. 4348:
over time to reflect the amount of stress present in an area. After several earthquakes have been recorded and studied, the signatures of shear wave splitting just before an earthquake occurs become well known and this can be used to predict future events. This same phenomenon can be seen before a volcanic eruption and it is inferred that they may be predicted in the same manner.
3924:. Shear wave splitting is produced by seismic waves traveling through a medium with oriented cracks or crystals. The changes in shear wave splitting measurements over the time leading up to an impending earthquake can be studied to give insight to the timing and location of the earthquake. These phenomena may be observed many hundreds of kilometers from the epicenter. 2486: 4239:
Shear wave splitting is very sensitive to fine changes in the pore pressure in the Earth's crust. In order to successfully detect the degree of anisotropy in a region there must be more several arrivals that are well distributed in time. Too few events cannot detect the change even if they are from
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Shear wave splitting measurements have been used successfully to predict several earthquakes. With better equipment and more densely spaced recording stations, we have been able to study the signature variations of shear wave splitting over earthquakes in different regions. These signatures change
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with the dominant direction of anisotropy in the area. The interactions between the tiny particles that make up solids and liquids can be used as an analogue for the way a wave travels through a medium. Solids have very tightly bound particles that transmit energy very quickly and efficiently. In a
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Shear-wave splitting measurements can provide the most accurate and in depth information about a particular region. However, there are limits that need to be accounted for when recording or analyzing shear wave splitting measurements. These include the sensitive nature of shear waves, that shear
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These features suggested that the crust was approaching fracture criticality and that an earthquake was likely to occur in the near future. Based on this information, an alert was sent to the Iceland Meteorological Office (IMO) on October 27 and 29, warning of an approaching earthquake. On November
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or character of the medium. When a polarized shear wave enters a new, anisotropic medium, it splits into two shear waves (Fig.2). One of these shear waves will be faster than the other and oriented parallel to the cracks or crystals in the medium. The second wave will be slower than the first and
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Stacking seismic data from a reflection survey is useful because it was collected with a predictable, controlled source. When the source is uncontrolled and unpredictable, stacking the data only degrades the signal. Because recorded shear wave time delays and polarizations vary in their incidence
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The pattern of increasing shear wave splitting time-delays is typical of the increase now seen before many earthquakes in Iceland and elsewhere. The time delays just before earthquakes characteristically decrease immediately following the eruption because the majority of the stress is released at
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prediction using shear wave splitting measurements. This theory is based on the fact that microcracks between the grains or crystals in rocks will open wider than normal at high stress levels. After the stress subsides, the microcracks will return to their original positions. This phenomenon of
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This statement only holds true if the fluid in the cracks is somehow removed. This may be accomplished via chemical absorption, drainage, or flow to the surface. However, these occur in relatively rare instances and there is evidence that supports the presence of fluids at depth. This includes
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Our understanding of shear wave splitting and how to best use the measurements is constantly improving. As our knowledge improves in this area, there will invariably be better ways of recording and interpreting these measurements and more opportunities to use the data. Currently, it is being
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up to 260 km beneath the volcanic area. The depths of these earthquakes make this area ideal for studying the structure of the upper mantle. They noted the arrivals of two distinct shear waves with different polarizations (N-S, fast and E-W, slow) approximately 0.7 seconds apart. It was
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Figure 6 is a schematic animation showing the process of shear wave splitting and the seismic signature generated by the arrivals of two polarized shear waves at the surface recording station. There is one incident shear wave (blue) traveling vertically along the center grey axis through an
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medium (Fig. 1). The incident shear wave splits into two polarized shear waves (Fig. 2). Shear wave splitting is typically used as a tool for testing the anisotropy of an area of interest. These measurements reflect the degree of anisotropy and lead to a better understanding of the area's
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to both the first shear wave and the cracks or crystals in the media. The time delays observed between the slow and fast shear waves give information about the density of cracks in the medium. The orientation of the fast shear wave records the direction of the cracks in the medium.
466:. Hess found that the slow compressional waves propagated perpendicular to the plane of slip and the higher velocity component was parallel to it. He inferred that the structure of oceanic basins could be recorded quickly and understood better if these techniques were used. 3943:. Shear-wave splitting measurements are recorded and analyzed to obtain the degree of anisotropy throughout the reservoir. The area with the largest degree of anisotropy will generally be the best place to drill because it will contain the largest number of open fractures. 2166: 3773: 1421: 3960:, Crampin and his coworkers recognized that time delays between split shear-waves were increasing at two seismic recording stations, BJA and SAU, in southwest Iceland. The following factors lead the group to recognize this as a possible precursor to an earthquake: 4179:
More observations are needed to confirm whether the increase and decrease time delay pattern is universal for all volcanic eruptions or if each area is different. It is possible that different types of eruptions show different shear wave splitting behaviors.
500:. Data from other nearby stations were used to constrain the source of the seismic anisotropy. He found the anisotropy to be consistent with the area directly below the volcanic area and was hypothesized to occur due to oriented crystals in a deep rooted 742: 2302: 1256: 3285: 3544: 462:, that if the crystals had even a slight statistical orientation this would be extremely evident in the seismic velocities recorded using seismic refraction. This concept was tested using seismic refraction profiles from the 953: 423:
material that is weakly anisotropic, the incident shear wave will split into two quasi-shear waves with approximately orthogonal polarizations that reach the receiver at approximately the same time. In the deeper
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Aster, R.; Shearer, P. (1991). "Quantitive measurements of shear wave polarizations at the Anza seismic network, southern California - Implications for shear-wave splitting and earthquake prediction".
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Ucisik, N.; Hanka, W.; Dahl-Jensen, T.; Mosegaard, K.; Priestley, K. (2008). "Variations of shear-wave splitting in Greenland: Mantle anisotropy and possible impact of the Iceland plume".
1168: 3036: 921: 458:. This area was chosen for this study because oceanic basins are made of large, relatively uniform homogeneous rocks. Hess observed, from previous seismic velocity experiments with 3340: 3920:
According to Crampin shear wave splitting measurements can be used to monitor stress levels in the earth. It is well known that rocks near an earthquake-prone zone will exhibit
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wave splitting varies with incidence and azimuth, and that shear waves may split multiple times throughout an anisotropic medium, possibly every time the orientation changes.
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to spreading centers or parallel to cracks, the polarizations of shear waves will always vary in three dimensions with incidence and azimuth within the shear wave window.
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S. Crampin; S. Peacock (2008). "A review of the current understanding of seismic shear-wave splitting in the Earth's crust and common fallacies in interpretation".
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Volti and Crampin observed temporal increases in Band-1 time-delays for 5 months at approximately 240 kilometer depth in directions N,SW and W,SW before the 1996
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When plotted using polarization diagrams, the arrival of split shear waves can be identified by the abrupt changes in direction of the particle motion (Fig.3).
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that one time. The increase in normalized time-delays in volcanic eruptions does not decrease at the time of the eruption but gradually declines at about
4845: 3939:. The best production in a field is associated with an area where there are multiple small fractures that are open, allowing for constant flow of the 4903: 4227:
No direct interpretation of the decrease is proposed but it is suggested that the decrease is associated with stress release by the induced events.
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S. Crampin; R.Evans; B. Ucer; M.Doyle; et al. (1980). "Observations of dilatancy-induced polarization anomalies and earthquake prediction".
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to gain invaluable information about the reservoir for years. Equipment is constantly being updated to reveal new images and more information.
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Piccinini, D; Pastori, M.; Margheriti, L. (2013). "ANISOMAT+: An automatic tool to retrieve seismic anisotropy from local earthquakes".
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inclusions oriented approximately N-S, then the maximum velocity direction would also be N-S, accounting for the presence of seismic
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The process of shear wave splitting can be represented as the application of the splitting operator to the shear wave function.
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have polarizations that are only orthogonal in a few specific directions. Polarizations of body waves are orthogonal in all
3768:{\displaystyle u_{s}\left(\omega \right)=A~w\left(\omega \right)\exp \left\Gamma \left(\phi ,\delta t\right)\cdot {\hat {p}}} 96: 1416:{\displaystyle N\left(U^{\left(n\right)}\right)-M\left(U^{\left({n-1}\right)}\right)+L\left(U^{\left({n-2}\right)}\right)=0} 277: 4200:. They observed shear-wave splitting from injection-induced events at a pilot well offset 190 meters form the KTB well. A 496:
concluded that the splitting was not caused by the earthquake source but by the travel path of the waves on the way to the
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Crampin, S.; Peacock, S. (2005). "A review of shear-wave splitting in the compliant crack-critical anisotropic Earth".
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Aki, K.; Richards, P.G. (2002). "Quantitative Seismology" (Second ed.). University Science Books, Sausalito, CA.
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Bokelmann and Harjes reported the effects on the shear waves of fluid injection at about 9 kilometer depth in the
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S. Crampin; Y. Gao (2006). "A review of techniques for measuring shear-wave splitting above small earthquakes".
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It had approximately the same duration and slope as a previously recorded magnitude 5.1 earthquake in Iceland.
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Pastori, M.; Piccinini, D.; Margheriti, L.; Improta, L.; Valoroso, L.; Chiaraluce, L.; Chiarabba, C. (2009).
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M. Ando; Y.Ishikawa; H. Wada (1980). "S-wave anisotropy in the upper mantle under a volcanic area in Japan".
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Figure 4. Schematic diagram of two orthogonal polarized shear waves traveling through an anisotropic medium.
463: 420: 71: 3314: 4766: 4352: 3892:. These two parameters can be individually estimated from multiple component seismic recordings (Fig. 5). 737:{\displaystyle {\frac {\partial }{\partial x_{i}}}\left=\rho {\frac {\partial ^{2}U_{j}}{\partial t^{2}}}} 404: 287: 254: 4868: 4217:
That the initial ~1% shear wave splitting decreases by 2.5% in the next 12 hours following the injection.
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density and orientation or crystal alignment. We can think of the anisotropy of a particular area as a
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Crampin (1981) first acknowledged the phenomenon of azimuthally-aligned shear wave splitting in the
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The difference in the travel velocities of the two shear waves can be explained by comparing their
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over several. This decrease is approximately linear and there appeared to be no other significant
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Vecsey, L. J.; Babuska, V. (2008). "Shear-wave splitting measurements-Problems and solutions".
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directions, however this type of propagation is generally very difficult to observe or record.
432:, the high frequency shear waves split completely into two separate shear waves with different 5056: 4320: 4107: 3794: 3347: 3308: 830: 4049: 4010: 5522: 5463: 5432: 5413:"Seismic anisotropy and mantle deformation: What have we learned from shear wave splitting?" 5399: 5370: 5360: 5323: 5290: 5257: 5224: 5184: 5138: 5097: 5078:"Seismic anisotropy and mantle deformation: What have we learned from shear wave splitting?" 5048: 5009: 4948: 4893: 4789: 4731: 4689: 4627: 4582: 4565: 4532: 4515: 4487: 4470: 4450: 3973: 3387: 3380: 2947: 470: 429: 121: 5503:
Shear-Wave-Splitting-in-Anisotropic-Media Collection (Goethe University Frankfurt, Germany)
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Temporal variations in shear-wave splitting as a direct result of injection-induced events.
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Due to the nature of split shear waves, when they are recorded in typical three-component
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This technique was not successful again until 2008 due to the lack of appropriate source-
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present in the medium, then it would act upon these particles like those that make up a
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S. Crampin (1981). "A review of wave motion in anisotropic and cracked elastic-media".
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The petroleum industry has been using shear wave splitting measurements recorded above
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data from the Kola deep well and the presence of high conductivity in the lower crust.
4268: 4264: 4204: 4111: 3280:{\displaystyle u\left(\omega \right)=A~w\left(\omega \right)\exp \left\cdot {\hat {p}}} 2760: 865: 543: 5537: 5365: 5338: 5328: 5303: 4960: 4898: 4631: 4365: 4283: 3931:
uses shear-wave splitting measurements to map the fractures throughout a hydrocarbon
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and the shear wave splitting measurements as a way of looking at what is in the box.
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of split shear-waves are fixed, parallel to cracks, or normal to spreading centers.
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is a real unit vector pointing in the displacement direction and contained in the
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R. Hoar; K. Stokoe (1978). "Generation and Measurement of Shear Waves In Situ".
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cracks opening and closing in response to changing stress conditions is called
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H. H. Hess (1964). "Seismic Anisotropy of the Uppermost Mantle under Oceans".
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In an isotropic homogeneous medium, the shear wave function can be written as
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of shear-wave splitting above small earthquakes can be improved by stacking.
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at a depth of 4,000 meters was used to record the splitting measurements.
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On October 27, 1998, during a four-year study of shear wave splitting in
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Icefield. This was the largest eruption in Iceland in several decades.
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stations, they were able to record both P-wave and S-wave arrivals from
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Ando (1980) focused on identifying shear-wave anisotropy in the upper
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Alfred Wegener Institute for polar and Marine Research(AWI)(Germany)
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The largest decrease occurred within two hours after the injection.
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always decreases with depth as fluid filled cracks are closed by
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is the angle between the polarization of the incident shear wave
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The splitting time to be very stable after the injection ceased.
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was the inferred level of fracture for the previous earthquake.
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and a time delay between them that may be up to a few seconds.
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An incident shear wave may enter an anisotropic medium from an
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Shear wave splitting measurements have been used to explore
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is the time delay between the slow and fast shear waves and
2623:{\displaystyle Det\left(\Gamma _{jk}-G\delta _{jk}\right)=0} 1958: 2278:{\displaystyle U^{\left(-1\right)}=U^{\left(-2\right)}=0} 3970:
The time delay increase at station BJA started at about
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disturbances during the period following the eruption.
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Figure 7 is a screen shot of the Matlab Demo output.
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A successfully stress-forecast earthquake in Iceland
4809:"Least-Squares Measurement of Shear-Wave Splitting" 4807:R. Bale; J. Li; B. Mattocks & S. Ronen (2006). 4263:Shear waves that propagate along the ray path at a 4840:E. LaBarre; T. Davis; R. Benson (March 19, 2008). 4164: 4075: 4036: 3999: 3884: 3855: 3826: 3806: 3767: 3612: 3583: 3538: 3371: 3334: 3279: 3155: 3107: 3030: 2966: 2936: 2890: 2831: 2799: 2769: 2749: 2707: 2622: 2543: 2480: 2277: 2203: 2160: 1964: 1415: 1250: 1162: 1107: 915: 855: 810: 777: 736: 4282:Even when propagating through parallel cracks or 4933:Geological Society, London, Special Publications 3632:corresponding to the two shear wave velocities. 3164:, indicates that the two shear waves have split. 3108:{\displaystyle G_{2}=G_{3}=\beta ^{2}p_{i}p_{i}} 2286:, and only the first component of the equation ( 403:media by encountering a change in the preferred 5304:"Wave-equation shear wave splitting tomography" 5162: 5160: 5158: 5156: 5154: 4665: 4663: 4661: 3169:Measurement of shear wave splitting parameters 4659: 4657: 4655: 4653: 4651: 4649: 4647: 4645: 4643: 4641: 4558: 4556: 4554: 342: 8: 5169:Physics of the Earth and Planetary Interiors 3863:and the polarization of the fast shear wave 1163:{\displaystyle f_{n}\left(\vartheta \right)} 444:Hess (1964) made the first measurements of 4869:"A successfully stress-forecast earthquake" 4867:S. Crampin; T.Volti; R. Stefánsson (1999). 3964:The increase persisted for nearly 4 months. 3031:{\displaystyle G_{1}=\alpha ^{2}p_{i}p_{i}} 2898:, which correspond to three eigenvalues of 2777:are the invariants of the symmetric matrix 5498:Information on Solids, Liquids, and Gasses 349: 335: 18: 5436: 5364: 5327: 5261: 5142: 5101: 5013: 4897: 4735: 4145: 4134: 4123: 4062: 4051: 4023: 4012: 3986: 3975: 3871: 3870: 3868: 3842: 3841: 3839: 3819: 3796: 3754: 3753: 3714: 3650: 3644: 3599: 3598: 3596: 3570: 3569: 3567: 3525: 3524: 3513: 3512: 3499: 3459: 3458: 3447: 3446: 3433: 3402: 3358: 3357: 3355: 3316: 3266: 3265: 3251: 3188: 3147: 3134: 3128: 3099: 3089: 3079: 3066: 3053: 3047: 3022: 3012: 3002: 2989: 2983: 2958: 2949: 2925: 2909: 2903: 2882: 2866: 2850: 2844: 2820: 2814: 2788: 2782: 2762: 2736: 2678: 2662: 2656: 2600: 2581: 2561: 2532: 2526: 2458: 2453: 2435: 2419: 2393: 2388: 2367: 2362: 2349: 2324: 2310: 2304: 2250: 2224: 2218: 2190: 2149: 2131: 2122: 2106: 2091: 2069: 2046: 2033: 2020: 2004: 1998: 1941: 1918: 1913: 1903: 1888: 1864: 1851: 1842: 1817: 1803: 1776: 1771: 1761: 1739: 1715: 1702: 1693: 1677: 1654: 1649: 1639: 1624: 1611: 1586: 1572: 1550: 1545: 1524: 1519: 1506: 1481: 1467: 1455: 1453: 1386: 1381: 1346: 1341: 1309: 1296: 1231: 1213: 1190: 1181: 1143: 1137: 1090: 1062: 1048: 1026: 1021: 1011: 1000: 976: 961: 955: 916:{\displaystyle t=\tau \left(x_{i}\right)} 903: 884: 838: 832: 802: 796: 770: 725: 710: 700: 693: 673: 658: 648: 633: 615: 602: 600: 5493:A lot of interesting seismic images(ASU) 4190:German Continental Deep Drilling Program 4184:Fluid-injection in Petroleum Engineering 4814:. CSPG / CSEG / CWLS Joint Conference. 4393: 3905:Applications, justification, usefulness 515:Crampin (1980) proposed the theory of 371:, is the phenomenon that occurs when a 30: 5488:Shear-wave splitting in Matlab(France) 4848:from the original on September 6, 2014 4415: 4404: 3335:{\displaystyle w\left(\omega \right)} 579:Mathematical Explanation(Ray theory) 7: 5117:S. Crampin; Lovell, John H. (1991). 4259:of split shear waves are orthogonal. 3636: 3394: 3180: 2648: 2553: 2296: 1990: 1445: 1288: 1173: 947: 876: 592: 2891:{\displaystyle g_{1},~g_{2},~g_{3}} 2708:{\displaystyle G^{3}-PG^{2}+QG-R=0} 945:) can be expressed as a ray series 5263:10.1111/j.1365-246x.1991.tb01401.x 5236:Crampin, S.; Lovell, J.H. (1991). 5144:10.1111/j.1365-246X.1991.tb01401.x 4821:from the original on July 19, 2011 4737:10.1111/j.1365-246x.1972.tb06147.x 4196:) deep drilling site in southeast 3725: 3404: 2817: 2785: 2578: 2529: 2416: 2346: 2142: 2134: 2001: 1934: 1906: 1857: 1853: 1708: 1704: 1670: 1642: 1503: 1012: 718: 697: 666: 651: 608: 604: 504:. If the magma chamber contained 14: 5344:Geophysical Journal International 5308:Geophysical Journal International 5302:Long, M. D.; Hoop, M. V. (2008). 5242:Geophysical Journal International 5123:Geophysical Journal International 4877:Geophysical Journal International 874:can be described by the equation 5411:Savage, M. K.; February (1999). 5366:10.1111/j.1365-246x.2009.04302.x 5329:10.1111/j.1365-246x.2007.03632.x 4985:G. Bokelmann; H. Harjes (2000). 4899:10.1046/j.1365-246x.1999.00891.x 3634:The resulting split waveform is 38: 5209:Journal of Geophysical Research 5025:from the original on 2011-07-21 4994:Journal of Geophysical Research 4967:from the original on 2009-05-21 4909:from the original on 2012-03-13 4774:Journal of Geophysical Research 4747:from the original on 2011-07-04 4007:and escalated to approximately 3156:{\displaystyle G_{2}\neq G_{3}} 2117: 2064: 5295:10.1016/j.wavemoti.2004.05.006 5076:M. K. Savage (February 1999). 4694:10.1016/j.wavemoti.2008.01.003 3876: 3847: 3759: 3604: 3575: 3530: 3518: 3464: 3452: 3363: 3271: 1: 5509:MATLAB Code for demonstration 4953:10.1144/GSL.SP.2003.212.01.09 4927:T. Volti; S. Crampin (2003). 2937:{\displaystyle G_{1},~G_{2},} 4632:10.1016/0165-2125(81)90026-3 3346:function (the result of the 2832:{\displaystyle \Gamma _{jk}} 2800:{\displaystyle \Gamma _{jk}} 2544:{\displaystyle \Gamma _{jk}} 5468:10.1016/j.tecto.2007.11.074 5404:10.1016/j.cageo.2013.01.012 5384:Computers & Geosciences 5045:Dynamic Geochemical Testing 4765:P. Silver; W. Chan (1991). 4455:10.1016/j.tecto.2008.01.021 4165:{\displaystyle 2ms/km/year} 3350:source time function), and 2506: 2504:To obtain the solution of ( 2288: 1439:where the vector operators 1282: 1276: 941: 484:. Using newly implemented 5570: 5189:10.1016/j.pepi.2006.06.002 4716:Geophys. J. R. Astron. Soc 3885:{\displaystyle {\hat {f}}} 3856:{\displaystyle {\hat {p}}} 3613:{\displaystyle {\hat {s}}} 3584:{\displaystyle {\hat {f}}} 3372:{\displaystyle {\hat {p}}} 2646:which can be rewritten as 1443:are given by the formula: 247:Coordinating Committee for 4332:developed for use in the 278:Adams–Williamson equation 4842:"Finding the sweet spot" 4780:(B10): 16, 429–16, 454. 4244:Common misunderstandings 4099:Temporal changes before 3807:{\displaystyle \delta t} 2839:has three eigenvectors: 856:{\displaystyle c_{ijkl}} 819:is the component of the 575:Mathematical explanation 226:Seismic intensity scales 221:Seismic magnitude scales 5229:10.1029/JB095iB08p12449 4076:{\displaystyle 10ms/km} 4037:{\displaystyle 10ms/km} 3115:corresponds to the two 1171:satisfies the relation 464:Mendocino Fracture Zone 4414:Cite journal requires 4353:hydrocarbon reservoirs 4338:predicting earthquakes 4308:Signal-to-noise ratios 4166: 4077: 4038: 4001: 4000:{\displaystyle 4ms/km} 3886: 3857: 3828: 3808: 3769: 3614: 3585: 3540: 3373: 3336: 3281: 3157: 3122:For anisotropic media, 3109: 3032: 2968: 2967:{\displaystyle ~G_{3}} 2938: 2892: 2833: 2801: 2771: 2751: 2709: 2624: 2545: 2482: 2279: 2205: 2162: 1966: 1417: 1252: 1164: 1109: 1016: 917: 857: 812: 779: 738: 548: 288:Earthquake engineering 5417:Reviews of Geophysics 5082:Reviews of Geophysics 4167: 4078: 4039: 4002: 3937:hydrocarbon reservoir 3911:earthquake prediction 3887: 3858: 3829: 3827:{\displaystyle \phi } 3809: 3770: 3615: 3586: 3541: 3374: 3337: 3282: 3158: 3110: 3033: 2978:For isotropic media, 2969: 2939: 2893: 2834: 2802: 2772: 2752: 2710: 2625: 2546: 2483: 2280: 2206: 2163: 1967: 1418: 1253: 1165: 1110: 996: 918: 858: 813: 811:{\displaystyle U_{j}} 780: 778:{\displaystyle \rho } 739: 588:Cartesian coordinates 546: 311:Earth Sciences Portal 283:Flinn–Engdahl regions 249:Earthquake Prediction 5554:Polarization (waves) 5015:10.1029/2000JB900207 5000:(B10): 23879–23894. 4296:lithostatic pressure 4122: 4050: 4011: 3974: 3867: 3838: 3818: 3795: 3643: 3624:of the polarization 3595: 3566: 3401: 3354: 3315: 3187: 3127: 3046: 2982: 2948: 2902: 2843: 2813: 2781: 2761: 2735: 2655: 2560: 2525: 2303: 2217: 2189: 2184:For the first order 1997: 1452: 1295: 1180: 1136: 954: 883: 831: 795: 769: 599: 362:Shear wave splitting 273:Shear wave splitting 5513:You can download a 5460:2008Tectp.462..137U 5429:1999RvGeo..37...65S 5396:2013CG.....56...62P 5357:2009GeoJI.179..601P 5320:2008GeoJI.172..311L 5287:2005WaMot..41...59C 5254:1991GeoJI.107..387C 5221:1990JGR....9512449A 5215:(B8): 12449–12473. 5181:2006PEPI..159....1C 5135:1991GeoJI.107..387C 5094:1999RvGeo..37...65S 5006:2000JGR...10523879B 4945:2003GSLSP.212..135V 4890:1999GeoJI.138....1X 4786:1991JGR....9616429S 4728:1972GeoJ...29....1C 4707:V. Cerveny (1972). 4686:2008WaMot..45..675C 4624:1981WaMot...3..343C 4579:1980Natur.286..874C 4529:1980Natur.286...43A 4484:1964Natur.203..629H 4447:2008Tectp.462..178V 3348:Fourier transformed 3119:traveling together. 3038:corresponds to the 2750:{\displaystyle P,Q} 2471: 2406: 2380: 2204:{\displaystyle n=0} 1931: 1789: 1667: 1563: 1537: 1131:where the function 1039: 821:displacement vector 173:Epicentral distance 16:Physical phenomenon 5521:movie by yourself 5517:code and create a 4342:volcanic eruptions 4334:petroleum industry 4162: 4101:volcanic eruptions 4073: 4034: 3997: 3929:petroleum industry 3882: 3853: 3824: 3804: 3765: 3610: 3581: 3536: 3369: 3332: 3277: 3153: 3105: 3040:compressional wave 3028: 2964: 2934: 2888: 2829: 2797: 2767: 2747: 2705: 2620: 2541: 2478: 2449: 2384: 2358: 2275: 2201: 2158: 1962: 1957: 1909: 1767: 1645: 1541: 1515: 1413: 1248: 1160: 1105: 1017: 913: 853: 808: 775: 734: 590:can be written as 584:equation of motion 549: 539:Physical mechanism 150:Induced seismicity 97:Remotely triggered 5438:10.1029/98rg02075 5103:10.1029/98RG02075 5053:10.1520/STP35669S 4794:10.1029/91JB00899 4573:(5776): 874–877. 4478:(4945): 629–631. 4321:radio propagation 3879: 3850: 3789: 3788: 3762: 3675: 3607: 3578: 3560: 3559: 3533: 3521: 3467: 3455: 3366: 3309:complex amplitude 3301: 3300: 3274: 3212: 2953: 2920: 2877: 2861: 2770:{\displaystyle R} 2731:where the values 2729: 2728: 2644: 2643: 2502: 2501: 2182: 2181: 2156: 2041: 2028: 1986: 1985: 1948: 1883: 1871: 1756: 1734: 1722: 1684: 1619: 1437: 1436: 1272: 1271: 1129: 1128: 939:The solution to ( 937: 936: 758: 757: 732: 680: 622: 533:elastic-constants 359: 358: 5561: 5471: 5454:(1–4): 137–148. 5442: 5440: 5407: 5378: 5368: 5333: 5331: 5298: 5267: 5265: 5232: 5193: 5192: 5164: 5149: 5148: 5146: 5114: 5108: 5107: 5105: 5073: 5067: 5066: 5040: 5034: 5033: 5031: 5030: 5024: 5017: 4991: 4982: 4976: 4975: 4973: 4972: 4924: 4918: 4917: 4915: 4914: 4908: 4901: 4873: 4864: 4858: 4857: 4855: 4853: 4837: 4831: 4830: 4828: 4826: 4820: 4813: 4804: 4798: 4797: 4771: 4762: 4756: 4755: 4753: 4752: 4746: 4739: 4713: 4704: 4698: 4697: 4667: 4636: 4635: 4605: 4599: 4598: 4587:10.1038/286874a0 4560: 4549: 4548: 4537:10.1038/286043a0 4510: 4504: 4503: 4492:10.1038/203629a0 4465: 4459: 4458: 4441:(1–4): 178–196. 4430: 4424: 4423: 4417: 4412: 4410: 4402: 4398: 4171: 4169: 4168: 4163: 4149: 4138: 4082: 4080: 4079: 4074: 4066: 4043: 4041: 4040: 4035: 4027: 4006: 4004: 4003: 3998: 3990: 3891: 3889: 3888: 3883: 3881: 3880: 3872: 3862: 3860: 3859: 3854: 3852: 3851: 3843: 3833: 3831: 3830: 3825: 3813: 3811: 3810: 3805: 3783: 3774: 3772: 3771: 3766: 3764: 3763: 3755: 3749: 3745: 3724: 3720: 3719: 3718: 3689: 3673: 3666: 3655: 3654: 3637: 3619: 3617: 3616: 3611: 3609: 3608: 3600: 3590: 3588: 3587: 3582: 3580: 3579: 3571: 3554: 3545: 3543: 3542: 3537: 3535: 3534: 3526: 3523: 3522: 3514: 3511: 3507: 3503: 3469: 3468: 3460: 3457: 3456: 3448: 3445: 3441: 3437: 3395: 3378: 3376: 3375: 3370: 3368: 3367: 3359: 3341: 3339: 3338: 3333: 3331: 3295: 3286: 3284: 3283: 3278: 3276: 3275: 3267: 3261: 3257: 3256: 3255: 3226: 3210: 3203: 3181: 3162: 3160: 3159: 3154: 3152: 3151: 3139: 3138: 3114: 3112: 3111: 3106: 3104: 3103: 3094: 3093: 3084: 3083: 3071: 3070: 3058: 3057: 3037: 3035: 3034: 3029: 3027: 3026: 3017: 3016: 3007: 3006: 2994: 2993: 2973: 2971: 2970: 2965: 2963: 2962: 2951: 2943: 2941: 2940: 2935: 2930: 2929: 2918: 2914: 2913: 2897: 2895: 2894: 2889: 2887: 2886: 2875: 2871: 2870: 2859: 2855: 2854: 2838: 2836: 2835: 2830: 2828: 2827: 2806: 2804: 2803: 2798: 2796: 2795: 2776: 2774: 2773: 2768: 2756: 2754: 2753: 2748: 2723: 2714: 2712: 2711: 2706: 2683: 2682: 2667: 2666: 2649: 2638: 2629: 2627: 2626: 2621: 2613: 2609: 2608: 2607: 2589: 2588: 2554: 2550: 2548: 2547: 2542: 2540: 2539: 2496: 2487: 2485: 2484: 2479: 2470: 2469: 2457: 2448: 2444: 2443: 2442: 2427: 2426: 2405: 2404: 2392: 2379: 2378: 2366: 2357: 2356: 2341: 2337: 2336: 2335: 2315: 2314: 2297: 2284: 2282: 2281: 2276: 2268: 2267: 2266: 2262: 2242: 2241: 2240: 2236: 2210: 2208: 2207: 2202: 2176: 2167: 2165: 2164: 2159: 2157: 2155: 2154: 2153: 2140: 2132: 2127: 2126: 2110: 2105: 2104: 2083: 2082: 2060: 2059: 2039: 2038: 2037: 2026: 2025: 2024: 2012: 2011: 1991: 1980: 1971: 1969: 1968: 1963: 1961: 1960: 1954: 1950: 1949: 1947: 1946: 1945: 1932: 1930: 1929: 1917: 1904: 1902: 1901: 1881: 1872: 1870: 1869: 1868: 1852: 1850: 1849: 1834: 1830: 1829: 1828: 1808: 1807: 1794: 1790: 1788: 1787: 1775: 1766: 1765: 1754: 1753: 1752: 1732: 1723: 1721: 1720: 1719: 1703: 1701: 1700: 1685: 1683: 1682: 1681: 1668: 1666: 1665: 1653: 1640: 1638: 1637: 1617: 1616: 1615: 1603: 1599: 1598: 1597: 1577: 1576: 1562: 1561: 1549: 1536: 1535: 1523: 1514: 1513: 1498: 1494: 1493: 1492: 1472: 1471: 1446: 1431: 1422: 1420: 1419: 1414: 1406: 1402: 1401: 1400: 1396: 1366: 1362: 1361: 1360: 1356: 1326: 1322: 1321: 1320: 1289: 1266: 1257: 1255: 1254: 1249: 1247: 1236: 1235: 1217: 1212: 1201: 1200: 1174: 1169: 1167: 1166: 1161: 1159: 1148: 1147: 1123: 1114: 1112: 1111: 1106: 1104: 1100: 1099: 1095: 1094: 1067: 1066: 1057: 1053: 1052: 1038: 1037: 1025: 1015: 1010: 992: 988: 981: 980: 966: 965: 948: 931: 922: 920: 919: 914: 912: 908: 907: 877: 862: 860: 859: 854: 852: 851: 817: 815: 814: 809: 807: 806: 784: 782: 781: 776: 752: 743: 741: 740: 735: 733: 731: 730: 729: 716: 715: 714: 705: 704: 694: 686: 682: 681: 679: 678: 677: 664: 663: 662: 649: 647: 646: 623: 621: 620: 619: 603: 593: 460:olivine crystals 351: 344: 337: 122:Earthquake swarm 42: 19: 5569: 5568: 5564: 5563: 5562: 5560: 5559: 5558: 5534: 5533: 5530: 5511: 5479: 5474: 5445: 5410: 5381: 5336: 5301: 5270: 5235: 5206: 5202: 5200:Further reading 5197: 5196: 5166: 5165: 5152: 5116: 5115: 5111: 5075: 5074: 5070: 5063: 5042: 5041: 5037: 5028: 5026: 5022: 4989: 4984: 4983: 4979: 4970: 4968: 4926: 4925: 4921: 4912: 4910: 4906: 4871: 4866: 4865: 4861: 4851: 4849: 4839: 4838: 4834: 4824: 4822: 4818: 4811: 4806: 4805: 4801: 4769: 4764: 4763: 4759: 4750: 4748: 4744: 4711: 4706: 4705: 4701: 4669: 4668: 4639: 4607: 4606: 4602: 4562: 4561: 4552: 4523:(5768): 43–46. 4512: 4511: 4507: 4467: 4466: 4462: 4432: 4431: 4427: 4413: 4403: 4400: 4399: 4395: 4390: 4385: 4361: 4329: 4246: 4233: 4186: 4120: 4119: 4104: 4048: 4047: 4009: 4008: 3972: 3971: 3954: 3949: 3907: 3898: 3896:Schematic model 3865: 3864: 3836: 3835: 3816: 3815: 3793: 3792: 3781: 3732: 3728: 3710: 3700: 3696: 3679: 3656: 3646: 3641: 3640: 3633: 3593: 3592: 3564: 3563: 3552: 3483: 3479: 3420: 3416: 3399: 3398: 3391: 3352: 3351: 3321: 3313: 3312: 3293: 3247: 3237: 3233: 3216: 3193: 3185: 3184: 3176: 3171: 3143: 3130: 3125: 3124: 3095: 3085: 3075: 3062: 3049: 3044: 3043: 3018: 3008: 2998: 2985: 2980: 2979: 2954: 2946: 2945: 2921: 2905: 2900: 2899: 2878: 2862: 2846: 2841: 2840: 2816: 2811: 2810: 2808: 2784: 2779: 2778: 2759: 2758: 2733: 2732: 2721: 2674: 2658: 2653: 2652: 2636: 2596: 2577: 2576: 2572: 2558: 2557: 2528: 2523: 2522: 2494: 2459: 2431: 2415: 2414: 2410: 2394: 2368: 2345: 2325: 2320: 2316: 2306: 2301: 2300: 2293: 2255: 2251: 2246: 2229: 2225: 2220: 2215: 2214: 2187: 2186: 2174: 2145: 2141: 2133: 2118: 2087: 2065: 2042: 2029: 2016: 2000: 1995: 1994: 1978: 1956: 1955: 1937: 1933: 1919: 1905: 1884: 1877: 1873: 1860: 1856: 1838: 1818: 1813: 1809: 1799: 1796: 1795: 1777: 1757: 1735: 1728: 1724: 1711: 1707: 1689: 1673: 1669: 1655: 1641: 1620: 1607: 1587: 1582: 1578: 1568: 1565: 1564: 1551: 1525: 1502: 1482: 1477: 1473: 1463: 1456: 1450: 1449: 1429: 1382: 1377: 1373: 1342: 1337: 1333: 1310: 1305: 1301: 1293: 1292: 1264: 1237: 1227: 1202: 1186: 1178: 1177: 1149: 1139: 1134: 1133: 1121: 1086: 1082: 1072: 1068: 1058: 1044: 1040: 1027: 972: 971: 967: 957: 952: 951: 929: 899: 895: 881: 880: 869: 864:represents the 834: 829: 828: 798: 793: 792: 767: 766: 750: 721: 717: 706: 696: 695: 669: 665: 654: 650: 629: 628: 624: 611: 607: 597: 596: 586:in rectangular 577: 541: 442: 397: 355: 303: 302: 268: 260: 259: 251: 248: 241: 231: 230: 211: 203: 202: 163: 162:Characteristics 155: 154: 135: 127: 126: 52: 17: 12: 11: 5: 5567: 5565: 5557: 5556: 5551: 5546: 5544:Wave mechanics 5536: 5535: 5510: 5507: 5506: 5505: 5500: 5495: 5490: 5485: 5478: 5477:External links 5475: 5473: 5472: 5448:Tectonophysics 5443: 5408: 5379: 5351:(1): 601–614. 5334: 5314:(1): 311–330. 5299: 5268: 5248:(3): 387–407. 5233: 5203: 5201: 5198: 5195: 5194: 5150: 5129:(3): 387–407. 5109: 5068: 5061: 5035: 4977: 4939:(1): 135–149. 4919: 4859: 4832: 4799: 4757: 4699: 4680:(6): 675–722. 4637: 4618:(4): 343–391. 4600: 4550: 4505: 4460: 4435:Tectonophysics 4425: 4416:|journal= 4392: 4391: 4389: 4386: 4384: 4383: 4378: 4373: 4368: 4362: 4360: 4357: 4328: 4325: 4312: 4311: 4300: 4299: 4280: 4279: 4269:phase velocity 4265:group velocity 4261: 4260: 4245: 4242: 4232: 4229: 4225: 4224: 4221: 4218: 4215: 4185: 4182: 4161: 4158: 4155: 4152: 4148: 4144: 4141: 4137: 4133: 4130: 4127: 4108:Gjalp Eruption 4103: 4097: 4085: 4084: 4072: 4069: 4065: 4061: 4058: 4055: 4045: 4033: 4030: 4026: 4022: 4019: 4016: 3996: 3993: 3989: 3985: 3982: 3979: 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2874: 2869: 2865: 2858: 2853: 2849: 2826: 2823: 2819: 2794: 2791: 2787: 2766: 2746: 2743: 2740: 2727: 2726: 2717: 2715: 2704: 2701: 2698: 2695: 2692: 2689: 2686: 2681: 2677: 2673: 2670: 2665: 2661: 2642: 2641: 2632: 2630: 2619: 2616: 2612: 2606: 2603: 2599: 2595: 2592: 2587: 2584: 2580: 2575: 2571: 2568: 2565: 2538: 2535: 2531: 2500: 2499: 2490: 2488: 2477: 2474: 2468: 2465: 2462: 2456: 2452: 2447: 2441: 2438: 2434: 2430: 2425: 2422: 2418: 2413: 2409: 2403: 2400: 2397: 2391: 2387: 2383: 2377: 2374: 2371: 2365: 2361: 2355: 2352: 2348: 2344: 2340: 2334: 2331: 2328: 2323: 2319: 2313: 2309: 2274: 2271: 2265: 2261: 2258: 2254: 2249: 2245: 2239: 2235: 2232: 2228: 2223: 2200: 2197: 2194: 2180: 2179: 2170: 2168: 2152: 2148: 2144: 2139: 2136: 2130: 2125: 2121: 2116: 2113: 2109: 2103: 2100: 2097: 2094: 2090: 2086: 2081: 2078: 2075: 2072: 2068: 2063: 2058: 2055: 2052: 2049: 2045: 2036: 2032: 2023: 2019: 2015: 2010: 2007: 2003: 1984: 1983: 1974: 1972: 1959: 1953: 1944: 1940: 1936: 1928: 1925: 1922: 1916: 1912: 1908: 1900: 1897: 1894: 1891: 1887: 1880: 1876: 1867: 1863: 1859: 1855: 1848: 1845: 1841: 1837: 1833: 1827: 1824: 1821: 1816: 1812: 1806: 1802: 1798: 1797: 1793: 1786: 1783: 1780: 1774: 1770: 1764: 1760: 1751: 1748: 1745: 1742: 1738: 1731: 1727: 1718: 1714: 1710: 1706: 1699: 1696: 1692: 1688: 1680: 1676: 1672: 1664: 1661: 1658: 1652: 1648: 1644: 1636: 1633: 1630: 1627: 1623: 1614: 1610: 1606: 1602: 1596: 1593: 1590: 1585: 1581: 1575: 1571: 1567: 1566: 1560: 1557: 1554: 1548: 1544: 1540: 1534: 1531: 1528: 1522: 1518: 1512: 1509: 1505: 1501: 1497: 1491: 1488: 1485: 1480: 1476: 1470: 1466: 1462: 1461: 1459: 1435: 1434: 1425: 1423: 1412: 1409: 1405: 1399: 1395: 1392: 1389: 1385: 1380: 1376: 1372: 1369: 1365: 1359: 1355: 1352: 1349: 1345: 1340: 1336: 1332: 1329: 1325: 1319: 1316: 1313: 1308: 1304: 1300: 1270: 1269: 1260: 1258: 1246: 1243: 1240: 1234: 1230: 1226: 1223: 1220: 1216: 1211: 1208: 1205: 1199: 1196: 1193: 1189: 1185: 1158: 1155: 1152: 1146: 1142: 1127: 1126: 1117: 1115: 1103: 1098: 1093: 1089: 1085: 1081: 1078: 1075: 1071: 1065: 1061: 1056: 1051: 1047: 1043: 1036: 1033: 1030: 1024: 1020: 1014: 1009: 1006: 1003: 999: 995: 991: 987: 984: 979: 975: 970: 964: 960: 935: 934: 925: 923: 911: 906: 902: 898: 894: 891: 888: 866:elastic tensor 850: 847: 844: 841: 837: 805: 801: 774: 756: 755: 746: 744: 728: 724: 720: 713: 709: 703: 699: 692: 689: 685: 676: 672: 668: 661: 657: 653: 645: 642: 639: 636: 632: 627: 618: 614: 610: 606: 576: 573: 540: 537: 456:oceanic basins 454:variations in 441: 438: 396: 393: 364:, also called 357: 356: 354: 353: 346: 339: 331: 328: 327: 326: 325: 323:Related topics 320: 314: 313: 305: 304: 301: 300: 295: 290: 285: 280: 275: 269: 266: 265: 262: 261: 258: 257: 252: 245: 242: 237: 236: 233: 232: 229: 228: 223: 218: 212: 209: 208: 205: 204: 201: 200: 195: 190: 185: 180: 175: 170: 164: 161: 160: 157: 156: 153: 152: 147: 142: 140:Fault movement 136: 133: 132: 129: 128: 125: 124: 119: 114: 109: 104: 99: 94: 89: 84: 79: 74: 69: 64: 59: 53: 48: 47: 44: 43: 35: 34: 28: 27: 15: 13: 10: 9: 6: 4: 3: 2: 5566: 5555: 5552: 5550: 5547: 5545: 5542: 5541: 5539: 5532: 5528: 5524: 5520: 5519:demonstration 5516: 5508: 5504: 5501: 5499: 5496: 5494: 5491: 5489: 5486: 5484: 5481: 5480: 5476: 5469: 5465: 5461: 5457: 5453: 5449: 5444: 5439: 5434: 5430: 5426: 5423:(1): 65–106. 5422: 5418: 5414: 5409: 5405: 5401: 5397: 5393: 5389: 5385: 5380: 5376: 5372: 5367: 5362: 5358: 5354: 5350: 5346: 5345: 5340: 5335: 5330: 5325: 5321: 5317: 5313: 5309: 5305: 5300: 5296: 5292: 5288: 5284: 5280: 5276: 5275: 5269: 5264: 5259: 5255: 5251: 5247: 5243: 5239: 5234: 5230: 5226: 5222: 5218: 5214: 5210: 5205: 5204: 5199: 5190: 5186: 5182: 5178: 5175:(1–2): 1–14. 5174: 5170: 5163: 5161: 5159: 5157: 5155: 5151: 5145: 5140: 5136: 5132: 5128: 5124: 5120: 5113: 5110: 5104: 5099: 5095: 5091: 5088:(1): 65–106. 5087: 5083: 5079: 5072: 5069: 5064: 5062:0-8031-0326-3 5058: 5054: 5050: 5046: 5039: 5036: 5021: 5016: 5011: 5007: 5003: 4999: 4995: 4988: 4981: 4978: 4966: 4962: 4958: 4954: 4950: 4946: 4942: 4938: 4934: 4930: 4923: 4920: 4905: 4900: 4895: 4891: 4887: 4883: 4879: 4878: 4870: 4863: 4860: 4847: 4843: 4836: 4833: 4817: 4810: 4803: 4800: 4795: 4791: 4787: 4783: 4779: 4775: 4768: 4761: 4758: 4743: 4738: 4733: 4729: 4725: 4721: 4717: 4710: 4703: 4700: 4695: 4691: 4687: 4683: 4679: 4675: 4674: 4666: 4664: 4662: 4660: 4658: 4656: 4654: 4652: 4650: 4648: 4646: 4644: 4642: 4638: 4633: 4629: 4625: 4621: 4617: 4613: 4612: 4604: 4601: 4596: 4592: 4588: 4584: 4580: 4576: 4572: 4568: 4567: 4559: 4557: 4555: 4551: 4546: 4542: 4538: 4534: 4530: 4526: 4522: 4518: 4517: 4509: 4506: 4501: 4497: 4493: 4489: 4485: 4481: 4477: 4473: 4472: 4464: 4461: 4456: 4452: 4448: 4444: 4440: 4436: 4429: 4426: 4421: 4408: 4397: 4394: 4387: 4382: 4379: 4377: 4374: 4372: 4369: 4367: 4366:Birefringence 4364: 4363: 4358: 4356: 4354: 4349: 4345: 4343: 4339: 4335: 4327:Future trends 4326: 4324: 4322: 4318: 4309: 4306: 4305: 4304: 4297: 4293: 4289: 4288: 4287: 4285: 4284:perpendicular 4277: 4276:Polarizations 4274: 4273: 4272: 4270: 4266: 4258: 4257:Polarizations 4255: 4254: 4253: 4251: 4243: 4241: 4237: 4230: 4228: 4222: 4219: 4216: 4213: 4212: 4211: 4208: 4206: 4203: 4199: 4195: 4191: 4183: 4181: 4177: 4175: 4159: 4156: 4153: 4150: 4146: 4142: 4139: 4135: 4131: 4128: 4125: 4115: 4113: 4109: 4102: 4098: 4096: 4094: 4089: 4070: 4067: 4063: 4059: 4056: 4053: 4046: 4031: 4028: 4024: 4020: 4017: 4014: 3994: 3991: 3987: 3983: 3980: 3977: 3969: 3966: 3963: 3962: 3961: 3959: 3951: 3947:Case examples 3946: 3944: 3942: 3938: 3934: 3930: 3925: 3923: 3918: 3916: 3912: 3904: 3902: 3895: 3893: 3873: 3844: 3821: 3801: 3798: 3785: 3778: 3776: 3756: 3750: 3746: 3742: 3739: 3736: 3733: 3729: 3721: 3715: 3711: 3707: 3704: 3701: 3697: 3693: 3690: 3686: 3683: 3680: 3676: 3670: 3667: 3663: 3660: 3657: 3651: 3647: 3639: 3638: 3635: 3631: 3627: 3623: 3601: 3572: 3556: 3549: 3547: 3527: 3515: 3508: 3504: 3500: 3496: 3493: 3490: 3487: 3484: 3480: 3476: 3473: 3470: 3461: 3449: 3442: 3438: 3434: 3430: 3427: 3424: 3421: 3417: 3413: 3410: 3407: 3397: 3396: 3393: 3389: 3385: 3382: 3360: 3349: 3345: 3328: 3325: 3322: 3318: 3310: 3306: 3297: 3290: 3288: 3268: 3262: 3258: 3252: 3248: 3244: 3241: 3238: 3234: 3230: 3227: 3223: 3220: 3217: 3213: 3207: 3204: 3200: 3197: 3194: 3190: 3183: 3182: 3179: 3173: 3168: 3163: 3148: 3144: 3140: 3135: 3131: 3121: 3118: 3100: 3096: 3090: 3086: 3080: 3076: 3072: 3067: 3063: 3059: 3054: 3050: 3041: 3023: 3019: 3013: 3009: 3003: 2999: 2995: 2990: 2986: 2977: 2976: 2975: 2959: 2955: 2931: 2926: 2922: 2915: 2910: 2906: 2883: 2879: 2872: 2867: 2863: 2856: 2851: 2847: 2824: 2821: 2792: 2789: 2764: 2744: 2741: 2738: 2725: 2718: 2716: 2702: 2699: 2696: 2693: 2690: 2687: 2684: 2679: 2675: 2671: 2668: 2663: 2659: 2651: 2650: 2647: 2640: 2633: 2631: 2617: 2614: 2610: 2604: 2601: 2597: 2593: 2590: 2585: 2582: 2573: 2569: 2566: 2563: 2556: 2555: 2552: 2536: 2533: 2521: 2517: 2513: 2509: 2508: 2498: 2491: 2489: 2475: 2472: 2466: 2463: 2460: 2454: 2450: 2445: 2439: 2436: 2432: 2428: 2423: 2420: 2411: 2407: 2401: 2398: 2395: 2389: 2385: 2381: 2375: 2372: 2369: 2363: 2359: 2353: 2350: 2342: 2338: 2332: 2329: 2326: 2321: 2317: 2311: 2307: 2299: 2298: 2295: 2291: 2290: 2285: 2272: 2269: 2263: 2259: 2256: 2252: 2247: 2243: 2237: 2233: 2230: 2226: 2221: 2211: 2198: 2195: 2192: 2178: 2171: 2169: 2150: 2146: 2137: 2128: 2123: 2119: 2114: 2111: 2107: 2101: 2098: 2095: 2092: 2088: 2084: 2079: 2076: 2073: 2070: 2066: 2061: 2056: 2053: 2050: 2047: 2043: 2034: 2030: 2021: 2017: 2013: 2008: 2005: 1993: 1992: 1989: 1982: 1975: 1973: 1951: 1942: 1938: 1926: 1923: 1920: 1914: 1910: 1898: 1895: 1892: 1889: 1885: 1878: 1874: 1865: 1861: 1846: 1843: 1839: 1835: 1831: 1825: 1822: 1819: 1814: 1810: 1804: 1800: 1791: 1784: 1781: 1778: 1772: 1768: 1762: 1758: 1749: 1746: 1743: 1740: 1736: 1729: 1725: 1716: 1712: 1697: 1694: 1690: 1686: 1678: 1674: 1662: 1659: 1656: 1650: 1646: 1634: 1631: 1628: 1625: 1621: 1612: 1608: 1604: 1600: 1594: 1591: 1588: 1583: 1579: 1573: 1569: 1558: 1555: 1552: 1546: 1542: 1538: 1532: 1529: 1526: 1520: 1516: 1510: 1507: 1499: 1495: 1489: 1486: 1483: 1478: 1474: 1468: 1464: 1457: 1448: 1447: 1444: 1442: 1433: 1426: 1424: 1410: 1407: 1403: 1397: 1393: 1390: 1387: 1383: 1378: 1374: 1370: 1367: 1363: 1357: 1353: 1350: 1347: 1343: 1338: 1334: 1330: 1327: 1323: 1317: 1314: 1311: 1306: 1302: 1298: 1291: 1290: 1287: 1285: 1284: 1279: 1278: 1268: 1261: 1259: 1244: 1241: 1238: 1232: 1228: 1224: 1221: 1218: 1214: 1209: 1206: 1203: 1197: 1194: 1191: 1187: 1183: 1176: 1175: 1172: 1170: 1156: 1153: 1150: 1144: 1140: 1125: 1118: 1116: 1101: 1096: 1091: 1087: 1083: 1079: 1076: 1073: 1069: 1063: 1059: 1054: 1049: 1045: 1041: 1034: 1031: 1028: 1022: 1018: 1007: 1004: 1001: 997: 993: 989: 985: 982: 977: 973: 968: 962: 958: 950: 949: 946: 944: 943: 933: 926: 924: 909: 904: 900: 896: 892: 889: 886: 879: 878: 875: 873: 867: 863: 848: 845: 842: 839: 835: 825: 822: 818: 803: 799: 789: 785: 772: 764:is the time, 763: 754: 747: 745: 726: 722: 711: 707: 701: 690: 687: 683: 674: 670: 659: 655: 643: 640: 637: 634: 630: 625: 616: 612: 595: 594: 591: 589: 585: 580: 574: 572: 570: 566: 562: 559: 554: 553:polarizations 545: 538: 536: 534: 530: 525: 523: 518: 513: 511: 510:birefringence 507: 503: 502:magma chamber 499: 494: 490: 489:seismographic 487: 483: 479: 478:Volcanic Area 476: 472: 467: 465: 461: 457: 453: 450: 447: 439: 437: 435: 434:polarizations 431: 427: 422: 417: 414: 411: 406: 402: 394: 392: 390: 386: 381: 377: 374: 370: 369:birefringence 367: 363: 352: 347: 345: 340: 338: 333: 332: 330: 329: 324: 321: 319: 316: 315: 312: 309: 308: 307: 306: 299: 296: 294: 291: 289: 286: 284: 281: 279: 276: 274: 271: 270: 264: 263: 256: 253: 250: 244: 243: 240: 235: 234: 227: 224: 222: 219: 217: 214: 213: 207: 206: 199: 196: 194: 191: 189: 188:Seismic waves 186: 184: 181: 179: 176: 174: 171: 169: 166: 165: 159: 158: 151: 148: 146: 143: 141: 138: 137: 131: 130: 123: 120: 118: 115: 113: 110: 108: 105: 103: 100: 98: 95: 93: 90: 88: 85: 83: 80: 78: 75: 73: 70: 68: 65: 63: 60: 58: 55: 54: 51: 46: 45: 41: 37: 36: 33: 29: 25: 21: 20: 5512: 5451: 5447: 5420: 5416: 5387: 5383: 5348: 5342: 5311: 5307: 5281:(1): 59–77. 5278: 5272: 5245: 5241: 5212: 5208: 5172: 5168: 5126: 5122: 5112: 5085: 5081: 5071: 5044: 5038: 5027:. Retrieved 4997: 4993: 4980: 4969:. Retrieved 4936: 4932: 4922: 4911:. Retrieved 4884:(1): F1–F5. 4881: 4875: 4862: 4850:. Retrieved 4835: 4823:. Retrieved 4802: 4777: 4773: 4760: 4749:. Retrieved 4719: 4715: 4702: 4677: 4671: 4615: 4609: 4603: 4570: 4564: 4520: 4514: 4508: 4475: 4469: 4463: 4438: 4434: 4428: 4407:cite journal 4396: 4381:Seismic wave 4350: 4346: 4330: 4313: 4301: 4281: 4262: 4247: 4238: 4234: 4226: 4210:They found: 4209: 4193: 4187: 4178: 4116: 4105: 4090: 4086: 3955: 3941:hydrocarbons 3926: 3919: 3908: 3899: 3790: 3779: 3622:eigenvectors 3561: 3550: 3304: 3302: 3291: 3177: 3123: 2730: 2719: 2645: 2634: 2551:are needed, 2516:eigenvectors 2505: 2503: 2492: 2287: 2213: 2185: 2183: 2172: 1987: 1976: 1440: 1438: 1427: 1281: 1275: 1274:Substitute ( 1273: 1262: 1132: 1130: 1119: 940: 938: 927: 827: 823: 791: 765: 761: 759: 748: 581: 578: 550: 526: 514: 498:seismometers 468: 443: 430:upper mantle 418: 415: 398: 395:Introduction 361: 360: 272: 267:Other topics 72:Blind thrust 5274:Wave Motion 4844:. E&P. 4722:(1): 1–13. 4673:Wave Motion 4611:Wave Motion 4250:seismograms 4231:Limitations 4112:Vatnajökull 3630:eigenvalues 3390:direction. 3388:propagation 3117:shear waves 2809:The matrix 2512:eigenvalues 2292:) is left. 493:earthquakes 421:homogeneous 405:orientation 380:anisotropic 255:Forecasting 216:Seismometer 210:Measurement 183:Shadow zone 32:Earthquakes 5549:Seismology 5538:Categories 5029:2010-05-11 4971:2010-05-11 4913:2010-05-11 4751:2010-05-11 4388:References 4315:angle and 4292:anisotropy 3915:reservoirs 3384:orthogonal 517:earthquake 506:elliptical 486:telemetric 410:orthogonal 408:sometimes 378:enters an 376:shear wave 298:Seismology 239:Prediction 178:Hypocenter 112:Supershear 92:Megathrust 87:Intraplate 82:Interplate 67:Aftershock 5529:website. 5527:MathWorks 5390:: 62–68. 5375:2122/5499 4961:129113171 3933:reservoir 3922:dilatancy 3877:^ 3848:^ 3822:ϕ 3799:δ 3760:^ 3751:⋅ 3740:δ 3734:ϕ 3726:Γ 3708:ω 3702:− 3694:⁡ 3684:ω 3661:ω 3605:^ 3576:^ 3531:^ 3519:^ 3494:δ 3491:ω 3485:− 3477:⁡ 3465:^ 3453:^ 3428:δ 3425:ω 3414:⁡ 3405:Γ 3364:^ 3326:ω 3272:^ 3263:⋅ 3245:ω 3239:− 3231:⁡ 3221:ω 3198:ω 3141:≠ 3077:β 3000:α 2818:Γ 2786:Γ 2694:− 2669:− 2598:δ 2591:− 2579:Γ 2530:Γ 2433:δ 2429:− 2417:Γ 2382:− 2347:Γ 2257:− 2231:− 2143:∂ 2138:τ 2135:∂ 2112:ρ 2002:Γ 1935:∂ 1907:∂ 1879:ρ 1858:∂ 1854:∂ 1844:− 1840:ρ 1730:ρ 1709:∂ 1705:∂ 1695:− 1691:ρ 1671:∂ 1643:∂ 1539:− 1504:Γ 1391:− 1351:− 1328:− 1242:ϑ 1222:ϑ 1207:ϑ 1154:ϑ 1080:τ 1077:− 1013:∞ 998:∑ 893:τ 872:wavefront 773:ρ 719:∂ 698:∂ 691:ρ 667:∂ 652:∂ 609:∂ 605:∂ 522:dilatancy 449:azimuthal 401:isotropic 389:black box 373:polarized 168:Epicenter 145:Volcanism 107:Submarine 62:Foreshock 57:Mainshock 5047:: 3–29. 5020:Archived 4965:Archived 4904:Archived 4846:Archived 4816:Archived 4742:Archived 4359:See also 4336:and for 4205:recorder 4202:borehole 4174:magmatic 4093:geophone 3174:Modeling 1280:) into ( 561:crystals 452:velocity 318:Category 293:Seismite 24:a series 22:Part of 5456:Bibcode 5425:Bibcode 5392:Bibcode 5353:Bibcode 5316:Bibcode 5283:Bibcode 5250:Bibcode 5217:Bibcode 5177:Bibcode 5131:Bibcode 5090:Bibcode 5002:Bibcode 4941:Bibcode 4886:Bibcode 4852:June 5, 4825:May 12, 4782:Bibcode 4724:Bibcode 4682:Bibcode 4620:Bibcode 4595:4237223 4575:Bibcode 4545:4306931 4525:Bibcode 4500:4292928 4480:Bibcode 4443:Bibcode 4317:azimuth 4198:Germany 3958:Iceland 3791:Where 3386:to the 3344:wavelet 3342:is the 3307:is the 2510:), the 788:density 786:is the 558:olivine 440:History 366:seismic 117:Tsunami 77:Doublet 5515:MATLAB 5059:  4959:  4593:  4566:Nature 4543:  4516:Nature 4498:  4471:Nature 4376:P-wave 4371:S-wave 4290:Crack 3674:  3626:matrix 3562:where 3303:where 3211:  2952:  2919:  2876:  2860:  2520:matrix 2294:Thus, 2040:  2027:  1988:where 1882:  1755:  1733:  1618:  826:, and 760:where 565:liquid 471:mantle 446:P-wave 198:S wave 193:P wave 134:Causes 5023:(PDF) 4990:(PDF) 4957:S2CID 4907:(PDF) 4872:(PDF) 4819:(PDF) 4812:(PDF) 4770:(PDF) 4745:(PDF) 4712:(PDF) 4591:S2CID 4541:S2CID 4496:S2CID 3628:with 3381:plane 3042:and 2212:, so 1441:N,M,L 529:crust 482:Japan 475:Chubu 426:crust 419:In a 385:crack 50:Types 5523:here 5057:ISBN 4854:2012 4827:2010 4420:help 4340:and 3927:The 3620:are 3591:and 2944:and 2757:and 2514:and 582:The 428:and 102:Slow 5525:on 5464:doi 5452:462 5433:doi 5400:doi 5371:hdl 5361:doi 5349:179 5324:doi 5312:172 5291:doi 5258:doi 5246:107 5225:doi 5185:doi 5173:159 5139:doi 5127:107 5098:doi 5049:doi 5010:doi 4998:105 4949:doi 4937:212 4894:doi 4882:138 4790:doi 4732:doi 4690:doi 4628:doi 4583:doi 4571:286 4533:doi 4521:286 4488:doi 4476:203 4451:doi 4439:462 4319:of 4194:KTB 4110:in 3691:exp 3474:exp 3411:exp 3228:exp 2518:of 1286:), 569:gas 567:or 480:in 5540:: 5462:. 5450:. 5431:. 5421:37 5419:. 5415:. 5398:. 5388:56 5386:. 5369:. 5359:. 5347:. 5341:. 5322:. 5310:. 5306:. 5289:. 5279:41 5277:. 5256:. 5244:. 5240:. 5223:. 5213:95 5211:. 5183:. 5171:. 5153:^ 5137:. 5125:. 5121:. 5096:. 5086:37 5084:. 5080:. 5055:. 5018:. 5008:. 4996:. 4992:. 4963:. 4955:. 4947:. 4935:. 4931:. 4902:. 4892:. 4880:. 4874:. 4788:. 4778:96 4776:. 4772:. 4740:. 4730:. 4720:29 4718:. 4714:. 4688:. 4678:45 4676:. 4640:^ 4626:. 4614:. 4589:. 4581:. 4569:. 4553:^ 4539:. 4531:. 4519:. 4494:. 4486:. 4474:. 4449:. 4437:. 4411:: 4409:}} 4405:{{ 4344:. 4054:10 4015:10 3917:. 3782:12 3553:11 3311:, 3294:10 2974:. 2807:. 2473:== 2408:== 870:A 868:. 790:, 512:. 26:on 5470:. 5466:: 5458:: 5441:. 5435:: 5427:: 5406:. 5402:: 5394:: 5377:. 5373:: 5363:: 5355:: 5332:. 5326:: 5318:: 5297:. 5293:: 5285:: 5266:. 5260:: 5252:: 5231:. 5227:: 5219:: 5191:. 5187:: 5179:: 5147:. 5141:: 5133:: 5106:. 5100:: 5092:: 5065:. 5051:: 5032:. 5012:: 5004:: 4974:. 4951:: 4943:: 4916:. 4896:: 4888:: 4856:. 4829:. 4796:. 4792:: 4784:: 4754:. 4734:: 4726:: 4696:. 4692:: 4684:: 4634:. 4630:: 4622:: 4616:3 4597:. 4585:: 4577:: 4547:. 4535:: 4527:: 4502:. 4490:: 4482:: 4457:. 4453:: 4445:: 4422:) 4418:( 4298:. 4192:( 4160:r 4157:a 4154:e 4151:y 4147:/ 4143:m 4140:k 4136:/ 4132:s 4129:m 4126:2 4071:m 4068:k 4064:/ 4060:s 4057:m 4044:. 4032:m 4029:k 4025:/ 4021:s 4018:m 3995:m 3992:k 3988:/ 3984:s 3981:m 3978:4 3874:f 3845:p 3802:t 3784:) 3780:( 3757:p 3747:) 3743:t 3737:, 3730:( 3722:] 3716:0 3712:T 3705:i 3698:[ 3687:) 3681:( 3677:w 3671:A 3668:= 3664:) 3658:( 3652:s 3648:u 3602:s 3573:f 3555:) 3551:( 3528:s 3516:s 3509:] 3505:2 3501:/ 3497:t 3488:i 3481:[ 3471:+ 3462:f 3450:f 3443:] 3439:2 3435:/ 3431:t 3422:i 3418:[ 3408:= 3361:p 3329:) 3323:( 3319:w 3305:A 3296:) 3292:( 3269:p 3259:] 3253:0 3249:T 3242:i 3235:[ 3224:) 3218:( 3214:w 3208:A 3205:= 3201:) 3195:( 3191:u 3149:3 3145:G 3136:2 3132:G 3101:i 3097:p 3091:i 3087:p 3081:2 3073:= 3068:3 3064:G 3060:= 3055:2 3051:G 3024:i 3020:p 3014:i 3010:p 3004:2 2996:= 2991:1 2987:G 2960:3 2956:G 2932:, 2927:2 2923:G 2916:, 2911:1 2907:G 2884:3 2880:g 2873:, 2868:2 2864:g 2857:, 2852:1 2848:g 2825:k 2822:j 2793:k 2790:j 2765:R 2745:Q 2742:, 2739:P 2724:) 2722:9 2720:( 2703:0 2700:= 2697:R 2691:G 2688:Q 2685:+ 2680:2 2676:G 2672:P 2664:3 2660:G 2639:) 2637:9 2635:( 2618:0 2615:= 2611:) 2605:k 2602:j 2594:G 2586:k 2583:j 2574:( 2570:t 2567:e 2564:D 2537:k 2534:j 2507:8 2497:) 2495:8 2493:( 2476:0 2467:) 2464:0 2461:( 2455:k 2451:U 2446:) 2440:k 2437:j 2424:k 2421:j 2412:( 2402:) 2399:0 2396:( 2390:j 2386:U 2376:) 2373:0 2370:( 2364:k 2360:U 2354:k 2351:j 2343:= 2339:) 2333:) 2330:0 2327:( 2322:U 2318:( 2312:j 2308:N 2289:5 2273:0 2270:= 2264:) 2260:2 2253:( 2248:U 2244:= 2238:) 2234:1 2227:( 2222:U 2199:0 2196:= 2193:n 2177:) 2175:7 2173:( 2151:i 2147:x 2129:= 2124:i 2120:p 2115:, 2108:/ 2102:l 2099:k 2096:j 2093:i 2089:c 2085:= 2080:l 2077:k 2074:j 2071:i 2067:a 2062:, 2057:l 2054:k 2051:j 2048:i 2044:a 2035:l 2031:p 2022:i 2018:p 2014:= 2009:k 2006:j 1981:) 1979:6 1977:( 1952:) 1943:l 1939:x 1927:) 1924:n 1921:( 1915:k 1911:U 1899:l 1896:k 1893:j 1890:i 1886:a 1875:( 1866:i 1862:x 1847:1 1836:= 1832:) 1826:) 1823:n 1820:( 1815:U 1811:( 1805:j 1801:L 1792:) 1785:) 1782:n 1779:( 1773:k 1769:U 1763:l 1759:p 1750:l 1747:k 1744:j 1741:i 1737:a 1726:( 1717:i 1713:x 1698:1 1687:+ 1679:l 1675:x 1663:) 1660:n 1657:( 1651:k 1647:U 1635:l 1632:k 1629:j 1626:i 1622:a 1613:i 1609:p 1605:= 1601:) 1595:) 1592:n 1589:( 1584:U 1580:( 1574:j 1570:M 1559:) 1556:n 1553:( 1547:j 1543:U 1533:) 1530:n 1527:( 1521:k 1517:U 1511:k 1508:j 1500:= 1496:) 1490:) 1487:n 1484:( 1479:U 1475:( 1469:j 1465:N 1458:{ 1432:) 1430:5 1428:( 1411:0 1408:= 1404:) 1398:) 1394:2 1388:n 1384:( 1379:U 1375:( 1371:L 1368:+ 1364:) 1358:) 1354:1 1348:n 1344:( 1339:U 1335:( 1331:M 1324:) 1318:) 1315:n 1312:( 1307:U 1303:( 1299:N 1283:1 1277:3 1267:) 1265:4 1263:( 1245:) 1239:( 1233:n 1229:f 1225:= 1219:d 1215:/ 1210:) 1204:( 1198:1 1195:+ 1192:n 1188:f 1184:d 1157:) 1151:( 1145:n 1141:f 1124:) 1122:3 1120:( 1102:) 1097:) 1092:i 1088:x 1084:( 1074:t 1070:( 1064:n 1060:f 1055:) 1050:i 1046:x 1042:( 1035:) 1032:n 1029:( 1023:k 1019:U 1008:0 1005:= 1002:n 994:= 990:) 986:t 983:, 978:i 974:x 969:( 963:k 959:U 942:1 932:) 930:2 928:( 910:) 905:i 901:x 897:( 890:= 887:t 849:l 846:k 843:j 840:i 836:c 824:U 804:j 800:U 762:t 753:) 751:1 749:( 727:2 723:t 712:j 708:U 702:2 688:= 684:] 675:l 671:x 660:k 656:U 644:l 641:k 638:j 635:i 631:c 626:[ 617:i 613:x 350:e 343:t 336:v

Index

a series
Earthquakes

Types
Mainshock
Foreshock
Aftershock
Blind thrust
Doublet
Interplate
Intraplate
Megathrust
Remotely triggered
Slow
Submarine
Supershear
Tsunami
Earthquake swarm
Fault movement
Volcanism
Induced seismicity
Epicenter
Epicentral distance
Hypocenter
Shadow zone
Seismic waves
P wave
S wave
Seismometer
Seismic magnitude scales

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