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1.
Based on the short period surface wave recorded by DSS of Project 85009, the Rayleigh wave dispersion of phase velocity is determined with the periods from 0.3s to 1.07s in Lücan-Fanxian Profile in this paper. The profile is divided into 7 sections by their dispersion characteristics, and the shallow velocity structure is inversed for each section. It shows that velocity obviously increases at the bottom of Neogene in the eastern region of the profile; that not only does Rayleigh wave velocity evidently decreases but also its waveform conspiciously changes across Neihuang fault, Changyuan fault and Liaolan fault respectively, by which the corresponding surface positions of these faults can be exactly determined; and that not only is S wave velocity between Changyuan fault and Liaolan fault smaller than that of its two sides, but also the buried depth of Neogene bottom is obviously larger than that of the two sides.  相似文献   

2.
用瞬态多道瑞利波法,对夏垫隐伏断裂附近的浅层速度结构进行了调查研究,利用f-k域分析方法提取瑞利波频散曲线,分别用遗传算法和半波长方法反演,得到断裂附近的横波速度结构和瑞利波相速度分布剖面。反演结果与钻孔资料的对比表明,瞬态瑞利波法对于探测上断点埋深较浅的隐伏断裂是有效和可靠的。  相似文献   

3.
The velocity structure of the crust beneath Liaoning province and the Bohai sea in China was imaged using ambient seismic noise recorded by 73 regional broadband stations. All available three-component time series from the 12-month span between January and December 2013 were cross-correlated to yield empirical Green's functions for Rayleigh and Love waves. Phasevelocity dispersion curves for the Rayleigh waves and the Love waves were measured by applying the frequencytime analysis method. Dispersion measurements of the Rayleigh wave and the Love wave were then utilized to construct 2D phase-velocity maps for the Rayleigh wave at8–35 s periods and the Love wave at 9–32 s periods,respectively. Both Rayleigh and Love phase-velocity maps show significant lateral variations that are correlated well with known geological features and tectonics units in the study region. Next, phase dispersion curves of the Rayleigh wave and the Love wave extracted from each cell of the 2D Rayleigh wave and Love wave phase-velocity maps,respectively, were inverted simultaneously to determine the3 D shear wave velocity structures. The horizontal shear wave velocity images clearly and intuitively exhibit that the earthquake swarms in the Haicheng region and theTangshan region are mainly clustered in the transition zone between the low-and high-velocity zones in the upper crust, coinciding with fault zones, and their distribution is very closely associated with these faults. The vertical shear wave velocity image reveals that the lower crust downward to the uppermost mantle is featured by distinctly high velocities, with even a high-velocity thinner layer existing at the bottom of the lower crust near Moho in central and northern the Bohai sea along the Tanlu fault, and these phenomena could be caused by the intrusion of mantle material, indicating the Tanlu fault could be just as the uprising channel of deep materials.  相似文献   

4.
东濮拗陷地区地震震相特征分析   总被引:1,自引:0,他引:1  
东濮拗陷位于河北平原地震带东南部,南邻河淮地震带,东与郯庐地震带相望。东濮拗陷受控于新北东向的聊兰断裂、黄河断裂和长垣断裂,对该区的地质构造特征、地震特征、震相特征等进行了研究。指出,东濮拗陷区的地震属浅源地震,该区有康氏面存在,地震台可记到清晰的康氏面反射波P^*。  相似文献   

5.
中国东北地区地壳上地幔三维S波速度结构   总被引:12,自引:9,他引:3       下载免费PDF全文
收集了中国东北地区159个固定地震台2011年1月至2012年6月和27个流动地震台2011年1月至2011年6月间的垂向连续记录,根据噪声成像方法得到研究区(105°E-135°E, 39°N-52°N)较短周期(8~30 s)的瑞雷波群速度和相速度频散资料,再结合该区已有的天然地震长周期瑞雷波(36~145 s)的群速度频散资料,我们反演得到了中国东北地区200 km以浅深度范围内的三维壳幔S波速度结构,并得到了该区的岩石圈厚度分布图.结果表明:研究区中、下地壳S波速度结构的横向分布,在重力梯度带两侧有很大的不同,以东地区显示为大范围的高速,以西地区则呈现为大面积的低速;松辽盆地下方岩石圈地幔表现为显著的高速,岩石圈地幔底界面深度可能在90~100 km,薄的岩石圈盖层暗示东北地区的岩石圈可能发生了减薄;郯庐大断裂下方呈现出大范围的比较显著的低速特征,断裂下方上地幔顶部可能有热物质活动.  相似文献   

6.
The multichannel analysis of surface wave (MASW) method has been effectively used to determine near-surface shear- (S-) wave velocity. Estimating the S-wave velocity profile from Rayleigh-wave measurements is straightforward. A three-step process is required to obtain S-wave velocity profiles: acquisition of a multiple number of multichannel records along a linear survey line by use of the roll-along mode, extraction of dispersion curves of Rayleigh waves, and inversion of dispersion curves for an S-wave velocity profile for each shot gather. A pseudo-2D S-wave velocity section can be generated by aligning 1D S-wave velocity models. In this process, it is very important to understand where the inverted 1D S-wave velocity profile should be located: the midpoint of each spread (a middle-of-receiver-spread assumption) or somewhere between the source and the last receiver. In other words, the extracted dispersion curve is determined by the geophysical structure within the geophone spread or strongly affected by the source geophysical structure. In this paper, dispersion curves of synthetic datasets and a real-world example are calculated by fixing the receiver spread and changing the source location. Results demonstrate that the dispersion curves are mainly determined by structures within a receiver spread.  相似文献   

7.
东北地区背景噪声的Rayleigh和Love波相速度层析成像   总被引:5,自引:2,他引:3       下载免费PDF全文
本文利用中国数字地震台网位于东北地区的122个宽频地震台站的18个月记录的三分量连续地震噪声数据,采用互相关方法提取了Rayleigh和Love波经验格林函数,并利用时频自动分析技术获取了相应的相速度频散曲线.通过反演频散曲线,获得了Rayleigh和Love波周期为8~35s的二维相速度分布.结果表明,东北地区相速度的分布存在横向和垂向的不均匀性.短周期的相速度分布同地表地质构造密切相关,松辽盆地及山间沉积盆地呈现低速异常,而大兴安岭、小兴安岭及东部的一些山岭显示高速异常.随着周期的增加,位于中间的松辽盆地变为高低速相间,两侧的造山带呈现低速异常.这种异常的转变,可能是受构造活动或者莫霍面深度的影响.另外,在周期为20~35s频段内,Rayleigh和Love波同一周期的相速度在松辽盆地和位于吉林地区的郯庐断裂带表现不一致,表明可能存在径向各向异性.  相似文献   

8.
In the free state, Rayleigh waves are assumed to travel in the form of planar wavefronts. Under such an assumption, the propagation behaviour of the modes of Rayleigh waves in layered half‐spaces is only frequency dependent. The frequency behaviour, which is often termed as dispersion, is determined by the shear wave velocity profile of layered soils within the depth related to wavelength (or frequency). According to this characteristic, the shear wave velocity profile can be back‐analysed from the dispersion. The technique is widely used in the surface wave testing. However, the wavefronts of Rayleigh waves activated by the surface sources are non‐planar. The geometric discrepancy could result in Rayleigh waves manifesting distance‐dependent behaviour, which is referred to as spatial behaviour in this paper. Conventional analysis ignoring this spatial behaviour could introduce unexpected errors. In order to take the effects of sources on the propagation behaviour into account, a new mathematical model is established for Rayleigh waves in layered elastic media under vertical disc‐like surface sources using the thin‐layer method. The spatial behaviour of the activated modes and the apparent phase velocity, which is the propagation velocity of Rayleigh waves superposed by the multiple modes, are then analysed. Aspects of the spatial behaviour investigated in this paper include the equilibrium path, the particle orbit, and the geometric attenuation of the activated Rayleigh waves. The results presented in this paper can provide some guidelines for developing new inverse mathematical models and algorithms.  相似文献   

9.
缅甸弧及邻区的壳幔S波速度结构与动力学过程   总被引:10,自引:4,他引:6       下载免费PDF全文
用适配滤波频时分析技术处理了锡龙(SHIO)、清迈(CHTO)、昆明(KMI)和拉萨LSA)台记录的长周期数字化面波记录,获取了穿过缅甸弧及周边地区的530条路径的Rayleigh波频散,这些频散的周期范围为10.45~105.03 s.在此基础上,以分格频散反演方法从混合路径频散中提取了1°×1°网格内的纯路径频散,并且由网格内的纯路径频散反演出深达200 km的S波速度结构,最后重建了缅甸弧及周边地区的S波速度三维结构.所得结果表明:大致以实皆断裂为分界,其东部地壳波速较低,其西部地壳波速较高.印度-缅甸地区岩石圈厚度为110~130 km,上地幔顶部S波速度为43~4.4 km/s;而缅甸弧东侧的滇缅泰地块下方为一低速地幔柱上涌区,其宽度为150~200 km左右,这里的岩石圈厚度为70~80 km,上地幔顶部S波速度为41~4.2 km/s.另外,S波速度结构还反映出这一构造格局呈南北向的空间展布,并且与该区地震震源分布、断裂走向、火山分布有很好的对应关系.  相似文献   

10.
本文采用基于数据驱动的深度降噪自编码网络构建了瑞雷面波群速度、相速度频散特性与地壳厚度的正反演函数关系,并利用最新频散模型反演了中国大陆的地壳厚度.对于神经网络架构体系的评价,除了考虑传统意义上的测试误差、训练误差之外,本文还用已知物理原理的正演结果与网络预测结果进行比较;在设计网络构架时,同时考虑地球模型和面波频散的...  相似文献   

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