Using the integrated geophysical methods detecting active faults: a case study in Beijing, China Wang Zhihui, Cai Xiangmin, Yan Jiayong, Wang Jiming, Liu Yu, Zhang Lei PII: DOI: Reference:
S0926-9851(17)30101-5 doi:10.1016/j.jappgeo.2017.01.030 APPGEO 3200
To appear in:
Journal of Applied Geophysics
Received date: Revised date: Accepted date:
4 May 2016 28 September 2016 24 January 2017
Please cite this article as: Zhihui, Wang, Xiangmin, Cai, Jiayong, Yan, Jiming, Wang, Yu, Liu, Lei, Zhang, Using the integrated geophysical methods detecting active faults: a case study in Beijing, China, Journal of Applied Geophysics (2017), doi:10.1016/j.jappgeo.2017.01.030
This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.
ACCEPTED MANUSCRIPT Using the integrated geophysical methods detecting active faults: a case study in Beijing, China
faults,
methods,
Beijing,
seismic
reflection,
TE
D
Abstract
geophysical
MA
Keywords: active paleomagnetism
NU
SC R
IP
T
Wang Zhihui1,2, Cai Xiangmin3,4, Yan Jiayong1,2*, Wang Jiming3, Liu Yu4, Zhang Lei4 1 MLR Key Laboratory of Metallogeny and Mineral Assessment, Institute of Mineral Resources, Chinese Academy of Geological Sciences, Beijing 100037, China 2 China Deep Exploration Center-SinoProbe Center, Chinese Academy of Geological Sciences, Beijing 100037, China 3 Beijing Bureau of Geology and Mineral Exploration and Development, Beijing 100195, China 4 Beijing Institute of geological survey, Beijing 102206, China
AC
CE P
Active faults in urban have a potential damage to citizens, because they can induce not only earthquakes, but also damage pavements, utilities, homes, businesses, factories and other manmade structures because of the slow, secular and differential slippage. Consequently, the researches of detecting active faults are of great significance. This paper proposes a set of geophysical methods to detect active faults by an example in Beijing, including gravity, controlled source audio-frequency magnetotellurics(CSAMT), seismic reflection, DC resistivity and paleomagnetism (Natural remanent magnetization in rocks) to locate faults and discuss their activities. In proposed methods, gravity interpretation helps us obtain the distribution and characteristics of buried faults beneath the plain, the results of CSAMT, seismic reflection and DC resistivity reveal features and characteristics of faults from the deep to shallow part; paleomagnetism associated with radiocarbon dating help us analyze the fault slip rate; 3D seismic reflection interpretation shows the structure of two faults in the three-dimensional subsurface and the interaction of each other. Also, a few acquisition parameters, data processing methods and significant suggestions are mentioned.
ACCEPTED MANUSCRIPT Introduction
AC
CE P
TE
D
MA
NU
SC R
IP
T
The concept of the active fault was put forward by Lawson et al. (1908), Wool(1916), Willis(1923) and Lee(1926) successively. From then on, it has been paid more attention by a few of scholars from different countries. Apart from inducing earthquake, active faults are the source of heavy damage to pavements, utilities, homes, businesses, factories and other manmade structures (Saribudak, 2006). Traditional methods to identify these faults include aerial photographs and field mapping, subsurface borehole data on both the footwall and hanging wall of the faults. However active faults are generally covered by different thickness of Quaternary unconsolidated sediments in the basin or plain, the objects of detecting are buried faults. In this case, those traditional methods are usually out of work, but geophysical exploration such as resistivity, gravity, magnetics, conductivity and seismic reflection play an important tool for detecting active faults. Active faults are closely related to land subsidence, ground fissures (Jia and Guo, 2007) and karst collapse in Beijing. Some of faults are currently active and distributing throughout the Beijing plain (Wang et al., 1990; Xu et al., 1992; Che et al., 1994; Xiang et al., 1996; Jiang et al., 2000; Zhao et al., 2004; Qiu et al., 2007; Zhang et al., 2008; Li et al., 2010; He et al., 2013; Zhao et al., 2015; Jiao et al., 2006; Bai et al. 2014; Zhang et al., 2014a, 2014b, 2014c). And many authors have proposed geophysical methods in detecting active faults in Beijing (Shao and Zhang, 1979; Su et al., 2000; Zhang et al., 2006; Gao et al., 2007; Wang et al., 2007; Zhang and Zhao, 2007; Li et al., 2008; Liu et al., 2010; Hu et al., 2011; Hou et al., 2011; Wang et al., 2011; Yang et al., 2011; He, 2013; Xia et al., 2013; Zhao C. B. et al., 2013; Zhao Y. et al., 2013; Dong et al., 2014; Li et al., 2014; Tian, 2014; Yong et al., 2014). In this paper, we choose some typical profiles to discuss the results and applicability of different geophysical methods in the project of special geological survey and monitoring active faults in Beijing plain.
ACCEPTED MANUSCRIPT
AC
CE P
TE
D
MA
NU
SC R
IP
T
Geological setting and background
Figure 1. Seismological setting overlaid with survey areas and lines. The historical earthquake data (date from A.D.294 to A.D.2014) were loaded from China Seismic Network Website ( http://www.ceic.ac.cn)
The Beijing plain is located in the northwestern part of the North China Plain and surrounded by the Yanshan Mountains to the north and the Taihang Mountains to the west. The long histories of development and evolution in tectonics have formed the features of basin-range tectonics and multi-sets of fault systems with different ranges. Generally, they can be divided as NNE-NE, NNW-NW and approximately E-W trending basins and faults (Ran et al., 2001). The most prominent active-faults trend in the northeast and extend about tens of kilometers. Then, it is the NW-trending active faults which are perpendicular to the former and smaller on the surface than the former and discontinuous. These faults control the regional tectonic-geomorphology, Quaternary geology and neotectonics, and caused several historically strong earthquakes (Figure 1).
NU
SC R
IP
T
ACCEPTED MANUSCRIPT
Figure 2. Different geophysical methods survey line(area) location
MA
Geophysical methods 1. Gravity
AC
CE P
TE
D
Gravity exploration is usually used for obtaining the characteristics of tectonic and geological setting, especially on the greenfield, due to the relatively large density differences between Quaternary and others strata. In our survey, gravity explorations were conducted to obtain the overview of distribution and characteristics of active faults in Beijing plain. In data processing of extracting structural information, we attribute such effort to the edge enhancement and detection of gravitational fields (Yan et al., 2015). Figure 3 gives an overview of the structural edge from the shallow to the deep in the whole plain. It shows the dip angle at the different part and the dynamical process, and also gives the suggestion with gravity profile (point spacing 50m) to arrange others geophysical methods’ lines. As indicated by red rectangle in Figure 3, Xiadian faults have low dip angle structures in the northeast and southwest part, but steep dip angle structures in the middle segment. Another representative survey was conducted on the intersection of two faults. The object is to gain the horizontal characteristics and intersected relationship of the two faults, simultaneously, contribute to assign the 3D seismic survey area and decrease the survey area, because 3D seismic is so expensive for engineering geological investigation. Figure 4 represents Bouger gravity (a) and its first vertical derivative (b), obviously, Huangzhuang-Gaoliying fault were truncated by Nankou-Sunhe fault and the strike in the intersection has been changed from North-North-East to South-North direction, which certified the previous research result and also was certified by the following 3D seismic reflection results.
CE P
TE
D
MA
NU
SC R
IP
T
ACCEPTED MANUSCRIPT
AC
Figure 3. Multi-scale edge detection of gravity anomalies in Beijing plain and its neighborhoods
Figure 4. The result of gravity exploration overlaid with interpreted faults. Bouger gravity (a) and its first vertical derivative
ACCEPTED MANUSCRIPT 2. CSAMT
AC
CE P
TE
D
MA
NU
SC R
IP
T
CSAMT is a frequency-domain electromagnetic sounding technique (Goldstein and Strangway, 1975) which uses a fixed grounded dipole or horizontal loop as an artificial signal source. And it is similar to the natural-source magnetotellurics (MT) and audio-frequency magnetotellurics (AMT) techniques; the chief differences center around the use of the artificial CSAMT signal source at a finite distance (Zonge and Hughes, 1991). As CSAMT can provide a stable, dependable signal, and greater detecting depth than DC resistivity, it is applied to map the subsurface structures of less than 2km to 3km depth in detecting active faults after gravity exploration. In our survey, we adapted scalar measurements with equatorial dipole array (Edwards, 1977) and simultaneously measured the electric field in x-direction (Ex) and the magnetic field in y-direction (Hy) with the electrode distance of 50m. Figure 5 illustrates the resistivity inversion result together with a geological interpretation and two drills profiles. The horizontal coordinate indicates station number, while the vertical coordinate represents the detection depth. It is obviously observed that the value of resistivity increases with the depth, low-resistivity in shallow part and high-resistivity in deep part. On the right hand of station 158, the resistivity cross section shows two different layers. The upper layer represents unconsolidated sediments in the Quaternary formation and the thickness of the upper layer varies from 500m to 900m. The resistivity anomaly in the lateral variations indicates that sediments are inhomogeneous in horizon and suddenly changes at station 198, which shows that a fault (F1) exists. The lower layer is a high-resistivity layer, composed of bedrock of Ji-xian formation. On the left hand of station 158, the resistivity cross section shows three different layers. The upper layer as well as the right represents unconsolidated sediments in the Quaternary formation, and the thickness varies slightly, from 300m to 350m. As the thickness on both sides of station 158 is apparently different, the other fault (F2) was suggested. Two holes (one at station 120 and the other at station 204) had been drilled after the 2D resistivity inversion analysis was executed. The results of two cores verified the CSAMT interpretation of the Quaternary thickness and improved the interpretation accuracy of detecting faults. As to geological interpretation of Jurassic and Ji-xian formation depicted in Figure 4, we referred to the previous geological knowledge. The result also indicates that the crustal in the region was uplifted and some strata are eroded before the Jurassic period and the subsidence on the leftward of station 158 occurred at the Jurassic period and was uplifted again before the Cretaceous period. Until the Quaternary, the whole region occurred subsidence. Because of the difference of sedimentation rate, the sag was formed between station 158 and 198 and controlled by the two faults.
SC R
IP
T
ACCEPTED MANUSCRIPT
Figure 5. CSAMT resistivity inversion section and geologic interpretation map
3. Seismic reflection
CE P
TE
D
MA
NU
Seismic reflection exploration has been proved to be the most effective geophysical tool for active faults exploration in China (Liu et al., 2010; Wang et al. 2011). Compared with other geophysical methods, it has a higher precision and resolution in horizontal and vertical direction and the detecting depth attained from deep seismic reflection profiling (Sato et al., 2009; Liu et al, 2009 and 2010) to ultra-high resolution seismic reflection profiling (Karastathis et al., 2007; Kaiser et al., 2009). In our survey, a few hundred of 2D profiles across main faults were conducted to locate active faults accurately above bedrock surface after CASMT exploration and a few square kilometers of true-3D seismic reflection were conducted to solve the two faults’ intersection relationship and retrieve three-dimensional structures. The acquisition parameters and data processing scheme of 2D and 3D seismic reflection are showed in Table 1, Table 2 and Table 3, respectively. Subsequently, some typical results are chosen to illustrate the detection effects. Table 1. Seismic acquisition parameters of 2D seismic reflection for active faults 96
Minimum/Maximum offset
20m/495m
AC
Number of active channels Nominal source interval
20m
Receiver spacing
5m
Recording length
1s
Sampling rate
0.5ms
Source type
One vibroseis (28 tons)
Geophone type
Three cascade vertical 60Hz per set
ACCEPTED MANUSCRIPT Table 2. Seismic acquisition parameters of 3D seismic reflection for active faults Survey Grid Design
Orthogonal (8 receiver lines and 12 5m×10m
Number of active channels
96×8
Maximum offset
1046.95m
Nominal source interval
20m
Shot line interval
80m
Receiver spacing
10m
SC R
IP
Bin size
T
shots)
Receiver line interval
60m
Maximum inline offset
475m
Maximum crossline offset
10m
NU
Recording length Sampling rate Source type
MA
Geophone type
2s
0.5ms Two set of vibroseis (28 tons) 6 Vertical 60Hz(three cascade and two parallel)
Table 3. 2D and 3D seismic reflection data processing scheme for active faults
D
2D scheme
TE
Prestack Trace editing Top mute F-K filter
CE P
AGC
3D Scheme Prestack Trace editing AGC Refraction statics Surface-consistent amplitude compensation Frequency filter and F-K filter
Adaptive filter
Top mute
Refraction statics
Deconvolution
AC
Deconvolution
Velocity analysis
Velocity analysis
NMO correction
NMO correction
Residual statics
Residual statics
CMP stacking
DMO velocity analysis
Poststack Signal enhancement Band-pass filter
DMO stacking Random noise attenuation Migration Time-variant filter Amplitude balance
3.1 2D seismic reflection A profiling across Shunyi fault is chosen to illustrate the accomplishment of seismic reflection in detecting active faults. As indicated in Figure 6, seismic reflections from Quaternary have well continual appearances, however, the discontinuity exists at station 770 and the displacement between hanging wall and footwall happens as a fault (F1) slipped. Obviously, there is a high-amplitude reflection at 0.6s and it represents
ACCEPTED MANUSCRIPT
MA
NU
SC R
IP
T
the bottom of Quaternary interface. At station 534, reflections from both sides have different characteristics in amplitude and phase. Seismic reflections are also disconnecting and have 0.1s time movement. An interesting seismic wave is indicated by white arrow between 0.8 and 1.0s at the lower left corner of Figure 5. We prefer to interpret it as seismic diffraction from the F2 fault plane, because seismic reflections on both sides of have a better continuity on the stack profiling and we can exclude it from seismic reflections according to the prior geological knowledge. However, “diffraction” is not visible in shot records and time- or depth-migration are not applied for this profiling, so it maybe also reflection wave from the side of survey line and can been solved only in 3D seismic survey.
AC
CE P
TE
D
Figure 6. 2D seismic reflection profiling and geologic interpretation map 3.2 3D seismic reflection 3D seismic reflection exploration has been widely used for oil, gas and coal exploration and has got better results in imaging subsurface structure. Fortunately, we also got supported funds to accomplish this project to solve the two faults’ intersection relationship and retrieve three-dimensional structures. According to the previous seismic geometry and data processing scheme stated, we attained the data volume of pre-time migration (Figure 7a, 7c). Compared to 2D survey line, the view of subsurface in all directions is retrieved and faults are easy to be identified. In order to interpret exactly and get the relation between seismic reflections and strata, a synthetic seismogram based on acoustic logging and density logging was made. As illustrated in Figure 7b, different seismic reflections (T01-T08) correspond to different strata interfaces and have a strong resemblance with seismic record. Although the core did not intersect bedrock, the interface of Quaternary and bedrock can be tracked easily, because strong impedance difference generates high-amplitude.
CE P
TE
D
MA
NU
SC R
IP
T
ACCEPTED MANUSCRIPT
Figure 7. 3D seismic pre-migration data volume(a), synthetic seismogram(b) and the volume sliced at
AC
the interpreted bedrock depth (c)
Two faults can be identified in Figure 8, one fault strike extends towards northwest and the other nearly towards north-south. Also, the north-south fault was intersected by the northwest one, the sag was formed in the northeast of area due to the jointed settlement. Time slices revealed the space configuration of structure and the variation of lithology, for example, the west segment of the northwest fault in time slices of 200ms and 250ms is less distinct than in time slices of 300ms, 350ms and 400ms, and disappears in the time slice of 500ms, which can been interpreted that the lithology varied in depth and seismic reflections originated from Quaternary, bedrock and the interior of bedrock respectively. Whereas a set of reflection wave originate from the interface of Quaternary and bedrock in the time slice of 550ms shows stronger amplitude than others slices. As the white arrow shows in the time slice of 550ms, the high-amplitude from different time slice can locate faults in different depth. The 3D seismic results are not only accordance with gravity exploration and retrieve the subsurface structures, but provide the formation mechanism of the sag in the northeast, which have a great significance to the prevention of geological disasters in this area. Some interesting circular structures indicated by grey arrows are identified in time slices
ACCEPTED MANUSCRIPT
TE
D
MA
NU
SC R
IP
T
of 300ms, 500ms and 550ms, which are considered to be related to buried hill. If it was true, the result will contribute to understand the kinematics mechanism of the two faults.
CE P
Figure 8. The different time slices with 50ms interval
4. DC resistivity
AC
The multi-electrode resistivity system has been widely applicable to address a variety of hydrogeological, geotechnical and environmental applications (Toll and Hassan, 2012). Compared with traditional instruments, it has several desired advantages (Tsourlos, 1995; Dahlin, 2001): (1) speed up data acquisition process; (2) improve the resolution and confidence through collecting large data sets to construct 2D and 3D images; (3) offer the flexibility to choose a suitable electrode arrangement for a particular problem, which in turn reduces the efforts and laborious electrodes switching using manual systems. Taking into account these advantages and the shortness of seismic reflection imaging at the depth shallower than 50m, we take the multi-electrode resistivity system as a complement of seismic exploration to track the buried growth fault in the shallow part. A series of trials were conducted to choose geometry, electrode spacing and cable length. To balance the resolution and penetration depth, we ultimately chose Wenner geometry, 2m electrode spacing and 120 electrodes. Figure 9 illustrates a typical example, the horizontal coordinate also indicates station number and the vertical coordinate represents the detection depth. It is easy to make out that there are two electrical layers in this section and the value of resistivity increases with the depth. Moreover, electrical characteristics happen to change at station 294. On the left hand, the upper low-resistivity layer and lower high-resistivity
ACCEPTED MANUSCRIPT
MA
NU
SC R
IP
T
layer are good in appearance; on the right hand, the lower high-resistivity layer has an irregular shape and the anomaly center is lower than the left one. These all attribute to the fault existed at station 294. However, DC resistivity prospecting as well as others geophysical methods based on potential field theory has the volume effect which decreases the detecting resolution in depth. By numerical modeling of the buried growth fault, we conclude that the interface of different stratum does not just site on the interface of different resistivity values, but below the interface a little. Although this qualitative analysis is not complete in theory and has a certain resolution error, it has got a better detecting depth and resolution than seismic reflection exploration in shallow part.
Figure 9. The resistivity inversion section and geologic interpretation map
D
5. Paleomagnetism
AC
CE P
TE
All geophysical methods stated above are intent to locate the fault and unable to provide the information of the fault slip rate. Paleomagnetism associated with radiocarbon dating has been certified as an effective tool for researching the fault slip rate (Zhao et al., 2013; Zhang et al., 2014a, 2014b, 2014c; Bai et al., 2014) To get the vertical displacement between hanging wall and footwall at different periods and discuss the mechanics of the fault since Quaternary, two cores at least are usually conducted on the hinging wall and the foot wall respectively after locating faults accurately using the integrated geophysical methods. We take drill 17 and drill 18 as an example. The sample, test and thermal demagnetization have been depicted by Zhang et.al (2014b). The contrast of drill 17, drill 18 and the geomagnetic polarity time scale (Cande and Kent, 1992) is shown in Figure 10. The Late Miocene-Early Pleistocene boundary (M/G) depth of drill 17 (hinging wall) and drill 18 (foot wall) are 309m and 192.5m respectively; the Early-Middle Pleistocene boundary (B/M) depth is 98m and 68m. Based on the result of Optically Stimulated Luminescence (OSL) and the sediment characteristics, the lower boundary of the Late Pleistocene of drill 17 and drill 18 are defined at the depth of 25.7m and 21.6m respectively; the Pleistocene–Holocene boundary at the depth of 1.0m and 0.8m. Accordingly, we got a conclusion that Nankou-Sunhe fault moved vertically at the speed of 0.065mm/a, 0.046 mm/a, 0.03mm/a, and 0.11mm/a during the Early, Middle, Late Pleistocene and the Holocene, which shows the fault slip rate is accelerating. Some attention should been paid on this fault and some actions should been taken to reinforce buildings and protect Infrastructures across this fault. As the slip rate is calculated relative to the differential movement of the hanging wall and footwall, It is important to exclude others uncertainties to ensure the accuracy of the calculation. The first and the most important are to ensure the number of samples
ACCEPTED MANUSCRIPT
AC
CE P
TE
D
MA
NU
SC R
IP
T
and testing accuracy. Then, the comparative analysis of lithology of borehole section should be careful, especially for the alluvial fan area. Because the sediment source with the same lithology may be different. The last is to eliminate uncertainties caused by geological structure, for example, the calculation is not exact when the stratum is not horizontal. A method to degrade this effect is that decreasing the distance between bores.
Figure 10. Geomagnetic polarity timescale and polarity events of drill 17 and drill 18(after Zhang et al., 2014b)
ACCEPTED MANUSCRIPT Discussion
MA
NU
SC R
IP
T
The integrated method helped us to solve the involved problem, but there are some problems and suggestions to be discussed as follow yet. (1) Seismic reflection has better resolution than other geophysical methods, but is limited by the exploration depth range due to the absence of deep seismic reflection profiling and ultra-shallow seismic reflection profiling. This mainly attribute to the shortage of supported funds and dynamite forbidden in Beijing. Many papers published have proven that the shallow information can been gained by little receiver spacing (20cm) and a specific explosive device (hundreds of frequency) used in exploration. The result equivalent to the ground-penetrating radar can image in the subsurface of 1m to 6m range (Barlach F., 2015). (2) There are less physical properties of rock sample from Quaternary, so we cannot confirm and constrain each geophysical interpretation result. (3) Survey lines are not usually orthogonal with faults strike because of manmade structures, which obstacles the interpretation accuracy. (4) We like to take faults as a tree, and it usually has some secondary faults as branches. To research the activity of a fault, we must get the deep structure and its dynamic characteristics to make sure the extent of the fault in the ground and locate the main fault and each fracture, rather than detecting merely the shallow part.
TE
D
Conclusion
AC
CE P
We propose a series of geophysical methods to locate faults from region/depth to local/shallow area and discussed the activity of main faults by paleomagnetism associated with radiocarbon dating. In the basis of these results, (1) we improve the accuracy of locating active faults and re-locate some faults, (2) make a great deal of insight into the structure and tectonic of main faults, especially for the intersection of Nankou-Sunhe fault and Huangzhuang-Gaoliying fault. (3) draw the conclusion that different faults are accelerating to slip since the Holocene.However, some methods still have the potential to be improved as mentioned in the previous section and the processing technology of denoising in a heavily urban environment should be improved. There are all forward us to do better in the future.
Acknowledgement Thanks are firstly given two anonymous reviewers and editors for their help comments on this manuscript. Then we would like to express our gratitude to Prof. Luo Shuiyu, Xu Mingcai and Huang Lijun from Institute of Geophysical and Geochemical Exploration, Chinese Academy of Geological Science, Prof. Xu Deshu from Beijing Explo-Tech Engineering Co., Ltd., Liu Guimei from Surveying and Maping Co., Ltd of Hebei Jiuhua, Niu pengcheng from Research Institute of Coal Geophysical Exploration of China National Administration of Coal Geology, Ding Lianjing from Beijing Institute of Geo-exploration Technology, and others who were involved in the whole process of geophysical data acquisition and processing. Thanks are also given to all staff from Beijing Institute of Geological Survey for their support to complete this manuscript. This work is supported by the National Natural Science Foundation of China under Grant 41574133 and
ACCEPTED MANUSCRIPT 41104061, and the project of special geological surveying and monitoring of active faults in Beijing plain( Grant No. [2009]038).
IP
T
Reference
SC R
Barlach F., 2015, Coincident GPR and ultra‐shallow seismic imaging in the Arkansas River Valley, Great Bend, Kansas: SEG Technical Program Expanded Abstracts, 859-861 L.
Y.,
Zhang
Cai
time
X.
M.,
framework
et
al.,
2014,Quaternary
constraints
on
activity
MA
magentostratigraphic
L.,
NU
Bai
chracteristics of the Shunyi Fault, Beijng Plain: Geoscience, 28(6),
D
1234-1242 (in Chinese with English Abstract)
TE
Cande S. C., Kent D. V., 1992, A new geomagnetic polarity time scale for
CE P
the Late Cretaceous and Cenozoic: Journal of Geophysical Research, 97(10), 13917-13951
AC
Che Z. H., 1994, Study of the activity of Nankou-Sunhe fault: Seismolgy and Geology, 16(2), 115-120 (in Chinese with English Abstract) Dahlin T., 2001, The development of DC resistivity imaging techniques: Computers and Geosciences, 27, 1019-1029. Dong Y. H., Liu X., Han Y. P., 2014, Gravity inversion of active parameters of main active fault in Beijing area: Journal of Seismological Research,37(3), 379-394 (in Chinese with English Abstract) Goldstein, M. A., and Strangway, D. W., 1975, Audio-frequency magnetotellurics with a grounded electric dipole source: Geophysics, 40,
ACCEPTED MANUSCRIPT 669-83. Gao J. H., Xu M. C., Rong L. X., et al., 2007, The shallow seismic method
IP
T
for detecting city fault activity: Geophysical & Geochemical Exploration,
SC R
31, 4-8 (in Chinese with English Abstract)
He F. B., Bai L. Y., Wang J. M., 2013, Deep structure and Quaternary activities of the Xiadian fault zone: Seismology and Geology, 35(3),
NU
490-505 (in Chinese with English Abstract)
MA
He Z. T., 2013, The application of low-frequency ground penetrating radar to active fault detection: Bulletin of the Institute of Crustal
D
Dynamics, 25, 116-124 (in Chinese with English Abstract)
TE
Hou Z. H., Zhong N. K., Hao Y. J., et al., 2011, Detecting Nankou-Sunhe
CE P
buried faulty by high density resistivity method: J. of Disaster-Prevention Science and Technology, 13(1), 1-6 (in Chinese with English Abstract)
AC
Hu P., Liu B. J., Bai L. X., et al., 2011, Synthetic exploration of the buried faults in Olympic park area: Chinese J. Geophys., 53(6): 1486-1494 (in Chinese with English Abstract) Jiao Q., Qiu Z. H., 2006, The main active faults Progress in Beijing plain: Tectonic and Crustal Stress Anthology, (18), 72-84 (in Chinese with English Abstract) Jia
S.
M.,
Guo
M.,
2007,
The
relationship
between
Huangzhuang-Gaoliying fault and by Gaoliying trench and earth fissure: Urban Geology, 2(7), 24-28 (in Chinese with English Abstract)
ACCEPTED MANUSCRIPT Jiang W. L., Hou Z. H., Su Y. Z., 2000, Quantitative study of Holocene activity of main active faults in the Beijing plain and prediction of future
IP
T
seismic danger: Tectonic and Crustal Stress Anthology, 13, 1-15 (in
SC R
Chinese with English Abstract)
Kaiser A. E., Green A. G., Campbell F. M., et al., 2009, Ultrahigh‐ resolution seismic reflection imaging of the Alpine Fault, New Zealand:
NU
Journal of Geophysical Research Solid Earth, 114(B11): 292-310
MA
Karastathis V. K., Ganas A., Makris J., et al., 2007, The application of shallow seismic techniques in the study of active faults: The Atalanti
TE
62(3):215-233
D
normal fault, central Greece: Journal of Applied Geophysics,
CE P
Lawson, A. C., Leuschner, A. O., Gilbert, G. K., et al., 1908, The California earthquake of april 18, 1906 : report of the state earthquake
AC
investigation commission: Journal of Geology, 18 Li D. Q., Di Q. Y., Wang G. J., 2008, Fault detection by CSAMT and its application to new district planning in Beijing: Progress in Geophysics, 23(6), 1963-1969 (in Chinese with English Abstract) Li L. and Chen Q. F., 2010, Slip rates at depth along the buried faults in Beijing plain area estimated from repeating micro earthquakes: Seismology and Geology, 32(3), 508-519 (in Chinese with English Abstract) Li Y. G., Jiang Z. Z., Liu Z. L., et al., 2014, Joint P-wave and S-wave seismic
ACCEPTED MANUSCRIPT reflection to investigate the Quaternary blind fault near surface, 6, 692-699 (in Chinese with English Abstract)
IP
T
Liu B. J., Hu P., Meng Y. Q., et al., 2009, Research on fine crustal structure
SC R
using deep seismic reflection profile in Beijing region: Chinese J. Geophys., 52(9), 2264-2272 (in Chinese with English Abstract) Liu B. J., Hu P., Chen Y., et al., 2010, The crustal shallow structures and
NU
buried active faults revealed by seismic reflection profiles in
MA
northwestern area of Beijng: Chinese J. Geophys., 52(8), 2015-2025 (in Chinese with English Abstract)
D
Qiu Z. H., Tang L., Kan B. X., et al., 2007, Study of modern fault activities
TE
in Beijing area using bore strain observations: Seismology and Geology,
CE P
29(4), 716-728 (in Chinese with English Abstract) Ran Y. K., Chen L. C., Xu X. W., et al., 2001, Quantitative data about active
AC
tectonics and possible locations of strong earthquakes in the future in the northwestern Beijing: Acta Seimologica Sinica, 14(5), 534-546 Saribudak M., 2006, Integrated geophysical studies over an active growth fault in Houston: Leading Edge, 25(3):332-334. Sato H., Ito K., Abe S., et al., 2009, Deep seismic reflection profiling across active reverse faults in the Kinki Triangle, central Japan: Tectonophysics, 472, 86–94 Shao X. Z., Zhang J. R., 1979, An experimental study of deep structures along the Kangzhuang-Dachang profile near Peking by observing
ACCEPTED MANUSCRIPT converted waves of earthquakes: Acta Seimologica Sinica, 1(1), 50-61 (in Chinese with English Abstract)
IP
T
Su P., Tian Q. J., Li W. Q., et al., 2000, Application of ground penetrating
SC R
radar in the study of active faults: Technology for Earthquake Disaster Prevention, 10(2), 281-290 (in Chinese with English Abstract) Toll D. G., Hassan A., 2012, Development of Automated Multi-electrode
NU
Resistivity System for Laboratory Measurements: Istanbul 2012 -
MA
International Geophysical Conference and Oil & Gas Exhibition, 1-4 L. S. Edwards, 1977, A MODIFIED PSEUDOSECTION FOR RESISTIVITY AND
P.,
1995,
Modelling
TE
Tsourlos
D
IP: GEOPHYSICS, 42(5), 1020-1036
interpretation
and
inversion
of
CE P
multielectrode resistivity survey data: Ph.D. thesis, University of York Tian Z. B., 2014, Application of CSAMT for active fault exploration in new
AC
district of Changpin, Beijing: Jilin University Wills, B., 1923, Earthquake risk in California: Bulletin of the Seismological Society of America, 4,147-154 (in Chinese with English Abstract) Wang L. M., Xue J., Huang X. M. et al., 1990, An analysis of the tectonic activities in Beijing down-wapped basin: Earthquake Research in China, 6(2), 25-36 (in Chinese with English Abstract) Wang Z. H., Han L. G., He W. J., et al. , 2011, The advantage of prestack depth migration technique in urban active fault detection: Urban Geology, 06(1), 52-55 (in Chinese with English Abstract)
ACCEPTED MANUSCRIPT Wang P. D., Li C. L., Wetzig E., et al., 2007, Seismic active faults in the northwestern Beijing by seismic tomography: Acta Seimologica Sinica,
IP
T
29(1), 11-19 (in Chinese with English Abstract)
SC R
Wood, H. O., 1916, The earthquake problem in the western United States: Bulletin of The Seismological Society of America, 6,181-217 Xia X. Y., Li Y., Wang S. L., et al., 2013, The application of CSAMT
NU
Exploration to detecting urban concealed faults: Geophysical &
MA
Geochemical Exploration, 37(4), 687-691 (in Chinese with English Abstract)
D
Xiang H. F., Fang Z. J., Zhang W. X., et al., 1996, Join profile survey of
TE
active features for the Late Quaternary subsurface faults in Beijing plain
CE P
region: Journal of Seismological Research, 18(1), 75-79 (in Chinese with English Abstract)
AC
Xu J., Wang L. M., Fang Z. T., 1992, Prelimlnary analysis of the tectonic activities of Baboshan and Huangzhang-Gaoliying faults in Beijing area: North China earthquake sciences, 10(3), 2-11 (in Chinese with English Abstract) Yan J. Y., Lü Q. T., Chen M. C. et al., 2015, Identification and extraction of geological structure information based on multi-scale edge detection of gravity and magnetic fields: An example of the Tongling ore concentration area: Chinese J. Geophys., 58(12), 4450-4464 (in Chinese with English Abstract)
ACCEPTED MANUSCRIPT Yang C. X., Yu S. N., Zhao J. X., et al., 2011, A Preliminary study of the great Late Tertiary NE-trending strike-slipping faults in Beijng
IP
T
area-Interpretation of the flower structures from seismic sounding data
SC R
equivalent body-forces and static deformation: Bulletin of the Institute of Crustal Dynamics, 23, 68-76 (in Chinese with English Abstract) Yong F., Jiang Z. Z., Luo S. Y., et al. , 2014, The seismic reflection study on
NU
high-resolution profile of shallow structure in north part of Xiadian fault:
MA
Chinese Journal of Engineering Geophysics, 11(6), 832-836 (in Chinese with English Abstract)
D
Zhang L., Bai L. Y., Cai X. M., et al., 2014a, Study on the position of
TE
northwest section of Nankou-Sunhe fault in Beijing and its activity:
CE P
Geoscience, 28(1), 234-242 (in Chinese with English Abstract) Zhang L., Bai L. Y., Cai X. M., et al., 2014b, Magnetostratigraphy study on
AC
the south segment of Nankou-Sunhe Fault at Beijing pain and its implications for the fault activity during quaternary: Quaternary science: 34(2), 381-390 (in Chinese with English Abstract) Zhang L., Bai L. Y., Cai X. M., et al., 2014c, An analysis of the activity of the northwest part of Nankou-Sunhe fault: Geology in China, 41(3), 902-911 (in Chinese with English Abstract) Zhang S. M., Wang D. D., Liu X. D., et al. , 2008, Using borehole core analysis to reveal Late Quaternary paleoearthquakes along the Nankou-Sunhe fault, Beijing: Science in China(series D), 38(7), 881-895
ACCEPTED MANUSCRIPT (in Chinese with English Abstract) Zhao C. B., Liu B. J., Ji J. F., et al., 2013, Fine crustal structure in the south
IP
T
of Beijing revealed by deep seismic reflection profiling: Chinese J.
SC R
Geophys., 56(4), 1168-1176 (in Chinese with English Abstract) Zhao X. J., Liu X. D, 2004, The main features of the latest active faults in Beijing area: Seismology, 24(3), 69-77 (in Chinese with English Abstract)
NU
Zhang X., Zhao L., Liu T. Y., 2006, Multi-scale wavelet separation of
MA
aero-magnetic anomaly and study of faults in Beijing area: Acta Seimologica Sinica, 28(5), 504-512 (in Chinese with English Abstract)
D
Zhang X., Zhao L., 2007, A test study of urban faults using analytical
TE
method of magnetic anomaly: Seismology and Geology, 29(2), 336-353
CE P
(in Chinese with English Abstract) Zhao Y., Cai X. M., Wang, J. M., 2015, The division of ‘small blocks’ of
AC
structure in Beijing plain and a discussion on the activity of micro block in Quaternary period: Geology in China, 42(6), 1876-1884 (in Chinese with English Abstract) Zhao Y., Wang Z. H., Luo S. Y., et al., 2013, The application of comprehensive geophysical exploration technique to buried fault detection in piedmont plain of Beijing: Urban Geology, 8(2), 38-41 (in Chinese with English Abstract) Zonge K. L., Hughes L. J., 1991, 9. Controlled source audio-frequency magetotellurics: Electromagnetic Methods in Applied Geophysics, 713-810