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An anisotropic shear velocity model of the Earth's mantle using normal modes, body waves, surface waves and long-period waveforms

机译:使用法向模态、体波、表面波和长周期波形的地幔各向异性剪切速度模型

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We use normal-mode splitting functions in addition to surface wave phase anomalies, body wave traveltimes and long-period waveforms to construct a 3-D model of anisotropic shear wave velocity in the Earth's mantle. Our modelling approach inverts for mantle velocity and anisotropy as well as transition-zone discontinuity topographies, and incorporates new crustal corrections for the splitting functions that are consistent with the non-linear corrections we employ for the waveforms. Our preferred anisotropic model, S362ANI+M, is an update to the earlier model S362ANI, which did not include normal-mode splitting functions in its derivation. The new model has stronger isotropic velocity anomalies in the transition zone and slightly smaller anomalies in the lowermost mantle, as compared with S362ANI. The differences in the mid- to lowermost mantle are primarily restricted to features in the Southern Hemisphere. We compare the isotropic part of S362ANI+M with other recent global tomographic models and show that the level of agreement is higher now than in the earlier generation of models, especially in the transition zone and the lower mantle. The anisotropic part of S362ANI+M is restricted to the upper 300 km in the mantle and is similar to S362ANI.When radial anisotropy is allowed throughout the mantle, large-scale anisotropic patterns are observed in the lowermostmantle with v_(SV) >v_(SH) beneath Africa and South Pacific and vSH > vSV beneath several circum-Pacific regions. The transition zone exhibits localized anisotropic anomalies of ~3 per cent v_(SH) > v_(SV) beneath North America and the Northwest Pacific and ~2 per cent v_(SV) > v_(SH) beneath South America. However, small improvements in fits to the data on adding anisotropy at depth leave the question open on whether large-scale radial anisotropy is required in the transition zone and in the lower mantle. We demonstrate the potential of mode-splitting data in reducing the trade-offs between isotropic velocity and anisotropy in the lowermost mantle for the even-degree variations. Spurious anisotropic variations in the mid-mantle are also suppressed with the addition of mode-splitting data.
机译:除了表面波相位异常、体波传播时间和长周期波形外,我们还使用正模分裂函数来构建地幔中各向异性横波速度的三维模型。我们的建模方法反演了地幔速度和各向异性以及过渡带不连续性形貌,并结合了新的地壳校正,用于分裂函数,这与我们对波形采用的非线性校正一致。我们首选的各向异性模型 S362ANI+M 是对早期模型S362ANI的更新,该模型在其推导中不包括正常模式分裂函数。与S362ANI相比,新模型在过渡带具有更强的各向同性速度异常,在最下层地幔的异常略小。中下地幔的差异主要局限于南半球的特征。我们将S362ANI+M的各向同性部分与其他最近的全球断层扫描模型进行了比较,并表明现在的一致性水平高于上一代模型,特别是在过渡带和下地幔。S362ANI+M的各向异性部分被限制在地幔的上部300 km,与S362ANI相似。当允许整个地幔呈径向各向异性时,在最下层的地幔中观察到大规模的各向异性模式,其中 v_(SV) >v_(SH) 位于非洲和南太平洋下方,vSH > vSV 位于几个环太平洋区域下方。过渡带在北美和西北太平洋下方表现出~3%的局部各向异性异常,v_(SH)> v_(SV)在南美洲下方~2%的v_(SV)> v_(SH)。然而,在深度添加各向异性的数据拟合方面的小幅改进使过渡带和下地幔是否需要大规模径向各向异性的问题悬而未决。我们证明了模式分裂数据在减少偶数度变化的最下层地幔中各向同性速度和各向异性之间的权衡方面的潜力。地幔中部的杂散各向异性变化也通过添加模式分裂数据而受到抑制。

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