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首页> 外文期刊>Tectonophysics: International Journal of Geotectonics and the Geology and Physics of the Interior of the Earth >Crustal structure in the Changbaishan volcanic area, China, determined by modeling receiver functions
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Crustal structure in the Changbaishan volcanic area, China, determined by modeling receiver functions

机译:中国长白山火山区地壳结构,通过模拟接收器函数确定

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During 1998-1999, we installed a temporary broadband seismic network in the Changbaishan volcanic region, NE China. We estimated crustal structure using teleseismic seismograms collected at the network. We detected a near surface region of strong anisotropy directly under the main volcanic edifice of the volcanic area. We modeled 109 receiver functions from 19 broadband stations using three techniques. First we used a "slant-stacking" method to model the principal crustal P reverberation phases to estimate crustal thickness and the average crustal P to S speed ratio (nu(p)u(s)), assuming an average P-wave velocity in the crust. We then estimated crustal S-wave velocity (nu(s)) and nu(p)u(s) profiles by modeling stacked receiver functions using a direct search. Finally, we inverted several receiver functions recorded at stations closest to the main volcanic edifice using least squares to estimate nu(s) velocity profiles, assuming a nu(p)u(s) value. The results from the three estimation techniques were consistent, and generally we found that the receiver functions constrained estimates of changes in wave speeds better than absolute values. We resolved that the crust is 30-39 km thick under the volcanic region and 28-32 km thick away from the volcanic region, with a midcrust velocity transition at about 10-15 km depth. We estimated that the average crust P-wave velocity is about 6.0-6.2 km/s surrounding the main volcanic region, while it is slightly lower in the vicinity of the main volcanic edifice. The estimates of nu(p)u(s) were more ambiguous, but we inferred that the bulk crustal Poisson's ratio (which is related to nu(p)u(s)) ranges between 0.20 and 0.30, with a suggestion that the Poisson's ratio is lower under the central volcanic region compared to the surrounding areas. We resolved low S-wave velocities (down to about 3 km/s) in the middle crust in the region of the main volcanic edifice. The low velocity anomaly extends from about 5-10 to 15-25 km below the surface, probably indicating a region of elevated temperatures. We were unable to determine if partial melt is present with the data we considered in this paper. (C) 2004 Elsevier B.V. All rights reserved.
机译:在1998-1999年期间,我们在中国东北的长白山火山区安装了一个临时的宽带地震网。我们使用网络收集的远震地震图估算了地壳结构。我们在火山区的主火山大厦正下方检测到一个强各向异性的近地表区域。我们使用三种技术对来自19个宽带站的109个接收器功能进行了建模。首先,我们使用“倾斜叠加”方法对主要的地壳P混响阶段建模,以估计地壳厚度和平均地壳P与S速度比(nu(p)/ nu(s)),并假设平均P波速度在地壳里。然后,我们通过使用直接搜索对堆积的接收器函数进行建模,估计了地壳S波速度(nu(s))和nu(p)/ nu(s)剖面。最后,假设nu(p)/ nu(s)的值,​​我们使用最小二乘法反转记录在最接近主火山大厦的站点的几个接收器函数,以估计nu(s)速度剖面。三种估计技术的结果是一致的,通常我们发现接收器功能比绝对值更好地限制了波速变化的估计。我们确定,火山区下方的地壳厚度为30-39 km,距火山区的厚度为28-32 km,中地壳速度转换的深度约为10-15 km。我们估计主火山区周围的平均地壳纵波速度约为6.0-6.2 km / s,而在主火山构造附近则略低。 nu(p)/ nu(s)的估计值比较不明确,但我们推断,地壳的泊松比(与nu(p)/ nu(s)有关)在0.20到0.30之间,建议与周围地区相比,中部火山区的泊松比更低。我们解决了主要火山构造区域中地壳的低S波速度(低至约3 km / s)。低速异常从地表以下大约5-10 km延伸到15-25 km,这可能表明温度升高了。我们无法确定本文所考虑的数据是否存在部分熔融。 (C)2004 Elsevier B.V.保留所有权利。

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