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ORIGINAL RESEARCH article

Front. Earth Sci., 20 January 2023
Sec. Structural Geology and Tectonics
This article is part of the Research Topic Measuring and Modeling the Ground Deformation of Geological Disasters Using Modern Geodesy View all 11 articles

Present-day activity and seismic potential of the north Qinling fault, southern ordos block, central China, as revealed from GPS data and seismicity

Chenyi YangChenyi Yang1Lingyun Ji
Lingyun Ji2*Yihai YangYihai Yang1Lina SuLina Su1Ying WangYing Wang1Huiren ShiHuiren Shi1
  • 1Shaanxi Earthquake Agency, Xi’an, China
  • 2The Second Monitoring and Application Center, China Earthquake Administration, Xi’an, China

The North Qinling Fault, located at the boundary of the North China Block and the South China Block, represents an important tectonic structure between the Weihe Basin and the Qinling Mountains, and controls the subsidence and expansion of the Weihe Basin. This fault has been highly active and has caused strong earthquakes since the Holocene and in a pre-seismic stage currently, as indicated by the many paleoearthquake traces found along it. To determine the present-day activity and seismic potential of the North Qinling Fault, by inverting GPS data, we produced fault locking depth, slip rate, and regional strain fields maps; moreover, based on seismicity, we produced a seismic b-value map. Combining this information with modern seismicity, we were able to comprehensively analyze the seismic potential of different fault segments. Our inversion of GPS data showed that the slip rate of the western segment of the fault (Qingjiangkou–Xitangyu) and the correspondent locking depth are 1.33 mm/a and 13.54 km, respectively, while the slip rate of the middle segment (Xitangyu–Fengyukou) and the correspondent locking depth are 0.45 mm/a and 8.58 km, respectively; finally, the slip rate of the eastern segment (Xitangyu–Daiyu) and the correspondent locking depth are 0.36 mm/a and 21.46 km, respectively. The locking depths of the western and middle segments of the fault are shallower than 90% of the seismic cutoff depth, while the locking depth of the eastern segment of the fault is similar to 90% of the seismic cutoff depth, indicating that “deep creep” occurs in the western and middle segments, while the eastern segment is locked. Modern small earthquakes have involved the western and middle segments of the fault, while the eastern segment has acted as a seismic gap with weak seismicity, characterized by a higher shear strain value and a lower b-value. These characteristics reflect the relationship between the locking depth and seismicity distribution. The results of our comprehensive analysis, combined with field geological surveys, show that the eastern segment of the North Qinling Fault has a strong seismic potential and is presently locked.

1 Introduction

Strong earthquakes (MS > 7) often occur at the boundary of active blocks in the mainland (Deng et al., 2003; Xu, 2006; Zhang et al., 2013). The North Qinling Fault, an active fault located at the boundary between the North China Block and the South China Block (i.e., first order blocks in Chinese mainland), can produce strong earthquakes (Figure 1). Specifically, the North Qinling Fault lies at the southern boundary of the Weihe Basin, which has been, historically, a strong seismically active area. Three M > 7 earthquakes have been recorded here, the most representative being the 1556 M 8¼ Huaxian earthquake, which caused > 840,000 deaths (https://data.earthquake.cn). Active faults are developed in the basin, among them, the North Qinling Fault is the largest, deepest and the most active fault (Zhang et al., 1990, 1991; Shaanxi Earthquake Agency, 1996; Bai, 2018).

FIGURE 1
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FIGURE 1. Tectonic setting of the North Qinling Fault and of the Weihe Basin. The fault data mainly refer to Deng et al. (2002) and Xu et al. (2016), while the seismic data were obtained from the National Earthquake Data Center (https://data.earthquake.cn). NCB, North China Block; SCB, South China Block; TP, Tibetan Plateau; WRB, Western Region Block; NAB, Northeast Asia Block; NQF, North Qinling Fault; THF, Taochuan–Huxian Fault; TBF, Taibai Fault; TLZF, Tieluzi Fault; LQMF, Longxian–Qishan-Mazhao Fault; QBF, Qianyang–Biaojiao Fault; WHF, Weihe Fault; LCF, Lintong –Chang’an Fault; LSF, Lishan Fault; WHSF, West Huashan Fault; WPF, Weinan Plateau Fault; HSF, Huashan Fault; JWF, Jingyang–Weinan Fault; HCF, Hancheng Fault; SLF, Shuangquan–Linyi Fault; LQF, Liquan Fault; NWF, North Weihe Fault; KGF, Kouzhen–Guanshan Fault.

Although there are few records of historical earthquakes along the North Qinling Fault, there are still many traces of ancient earthquakes, landslides, and barrier lakes, implying a number of strong earthquakes should have been caused by this fault since the beginning of the Holocene, demonstrating its earthquake generating ability. Paleoearthquake trenching dating has revealed that strong earthquakes occur about every 3,000 years along the North Qinling Fault, and that we might now be close to the end of the recurrence period: in a pre-seismic stage (Shaanxi Earthquake Agency, 1996; Bai, 2018). Considering these major earthquake hazard conditions, it is ungently needed to study the present-day activity and seismic potential of the North Qinling Fault.

Since the 1980s, detailed studies based on geological exploration have been carried on the North Qinling Fault to understand its geometry, kinematics, dynamics, structural evolution, and seismic ability (Zhang et al., 1990, 1991; Shentu et al., 1991; Bai, 2018; Huang et al., 2020; Yang, 2022). However, previous research has mainly focused on paleoearthquake events and normal faulting along the fault, while, quantitative analyses of the present-day seismic potential associated to current motion (particularly the strike-slip movement of the fault) have not been conducted.

Modern geodetic monitoring (especially GPS monitoring) is an effective and widely method used to recognize ongoing crustal movements. It can be applied to obtain the fault slip rate, locking depth, and strain field, which provide information on the earthquake cycle stage of the fault (Segall and Davis, 1997; Meade and Hager, 2005; Vigny et al., 2005; Papanikolaou et al., 2005; Huang et al., 2019; Chen et al., 2020; Li et al., 2021; Song et al., 2022). Numerous high-resolution analyses of geodetic observations along the active fault have been conducted to identify any connections with seismicity distribution and, hence, the current seismotectonic behavior (Sykes, 1971; Perez and Jacob, 1980; Zhang et al., 2003; Becker et al., 2005; Fialko, 2006; Parsons, 2006; Wen et al., 2007, 2008, 2013; Du et al., 2009, 2010, 2018; Wang et al., 2015; Liu et al., 2016; Li et al., 2020; Yin et al., 2020; Zhou et al., 2022).

In this study, we aimed to determine the present-day seismic potential associated with fault strike-slip movement and seismic activity along the North Qinling Fault, based on GPS data and seismicity. Firstly, we divided the North Qinling Fault into three segments from W to E (as in Zhang et al., 1991, Shaanxi Earthquake Agency, 1996 and Bai, 2018), and selected a total of three GPS profiles along the vertical direction of the fault strike (one for each segment). Based on GPS data, we inverted the slip rates, the locking depths, and the strain fields of the segments. Then, we determined any variations in the statistical properties of microseismicity (i.e., b-values and focal depth-frequency), identifying a seismic gap. The earthquake generating capacity of the fault was estimated by calculating the moment magnitude. Finally, we discussed the present-day activity and the seismic potential of the North Qinling Fault segments. The outcome of this study is vital to assess the seismic hazards and earthquake prediction in the densely populated Weihe Basin.

2 Geological setting

The North Qinling Fault is located in the northeastern part of the Tibetan Plateau, at the southern Ordos Block, central China (Figure 1). This fault formed due to multi-stage tectonic movements, which controlled the subsidence and evolution of the Weihe Basin to the N and the uplift of the Qinling Mountains to the S, since the Cenozoic. The fault dips northward (60–80°) and strikes W–E, extending from Qingjiangkou to Xitangyu, Fengyukou, and finally terminates at Daiyu, for a total length of 220 km. The N and S walls of the fault correspond to the loess plateau of the Weihe Basin and to the Qinling Mountains, respectively. Satellite images show clear linear feature for the fault; additionally, Bouguer gravity anomaly and aeromagnetic clearly indicate the occurrence of a density gradient zone along the fault (Peng et al., 1992, 2017). The North Qinling Fault can be divided into three segments according to its geometric characteristics and tectonic landforms. The western segment extends from Qingjiangkou to Xitangyu, is about 73 km long, and its approximate strike direction is SE; the middle segment extends from Xitangyu to Fengyukou, is about 90 km long, and its approximate strike direction is E–W; finally, the eastern segment extends from Fengyukou to Daiyu, is about 47 km long, and its approximate strike direction is E–W; (Zhang et al., 1991, Shaanxi Earthquake; Agency, 1996; Bai, 2018).

Previous research mainly focused on the vertical component of the North Qinling Fault. Under a of normal fault movement, the N wall has been descending, while the S wall has been ascending since the beginning of the Tertiary. Fault scarps of different scales and vertical offsets> 10 km were observed along the fault (Han et al., 2001; Liu et al., 2013; Huang et al., 2020). Regarding present-day fault activity, both the slip rate and the locking depth of the eastern segment are larger than those of the western-middle segments (Cui et al., 2019). Notably, the North Qinling Fault also shows obvious traces of sinistral strike-slip movements, which have horizontally offset rivers and terraces located in front of the Qinling Mountains (Shentu et al., 1991; Peng et al., 1992; Liu et al., 2013.; Ma, 2020).

3 Data and methods

3.1 GPS data

The GPS data used in this study come from Wang and Shen (2020). Our study mainly considered data from campaign and continuous GPS sites included in the Crustal Movement Observation Network of China (CMONOC) I and II project. Data from the continuous GPS sites, the campaign GPS sites of CMONOC I, and the continuous GPS sites, the campaign GPS sites of CMONOC II covered the following time spans: 1999–2016 and 1999–2015, 2009–2016 and 2009–2015, respectively. As detailed in Wang and Shen (2020), the raw GPS data obtained from 100 globally distributed IGS sites were processed all together using the GAMIT (Herring et al., 2010) software to ensure solutions of high quality and homogeneity. Particularly, the post-seismic and co-seismic deformation caused by large earthquakes have been modeled using the QOCA software (https://gipsy.jpl.nasa.gov/∼qoca). In this study, the co-seismic offsets and effects of the 2005 Sumatra, 2008 Wenchuan, and 2011 Tohoku–Oki earthquakes were considered and corrected. Meanwhile, the stations with low quality (observated by the GeoTracer receiver/antenna during 1999 and 2000) and disturbed by anthropogenic activities (such as ground water and oil pumping, coal mining, etc.,) are discarded.

3.2 Viscoelastic coupling model

GPS velocity field refers to the velocities occurring parallelly and perpendicularly to a fault: they represent the strike-slip rate and the compression rate, respectively, and quantify crust activity. According to the characteristics of the GPS station and our fault segmentation, we selected three velocity profiles along the North Qinling Fault that were orthogonal to the fault strike (Figure 2). The GPS rates were decomposed into fault-parallel and fault-perpendicularly components to obtain the correspondent projection values (Figure 3). Then, the velocity component parallel to the fault strike (i.e., the strike-slip rate of the fault) was inverted. According to the viscoelastic coupling model, considering the locking depth as a dividing line, no slip movement should occur between the surface and the locking depth, but rather below the locking depth. The basic relationship among the locking depth, the long-term slip rate, and the surface movement during the horizontal slipping of the fault was obtained based on the traditional dislocation model (Savage and Burford, 1973; Savage et al., 1999):

Vzx=bobiπarctanxxihi

where Vz(x) is the pre-seismic slip rate of the surface, b0 the adaptability constant, bi is the long-term slip rate, x is the fault depth, and hi is the locking depth at xi. The thickness of the elastic plastic transition zone in the upper lower crust is determined to be 0 km. The determined slip rates and locking depths are shown in Table 1.

FIGURE 2
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FIGURE 2. Distribution of the GPS velocity profiles across the North Qinling Fault. The black boxes indicate the profiles used for the computation of fault slip rate and locking depth. HYF, Haiyuan Fault; WQF, West Qinling Fault; KLF, Kunlun Fault; LMSF, Longmenshan Fault; ANF, Anninghe Fault; NQF, North Qinling Fault. The fault data were sourced from Zhang et al. (2013).

FIGURE 3
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FIGURE 3. GPS velocity profiles. The top graphs refer to the direction parallel to the fault strike, while the bottom graphs refer to the direction perpendicular to the fault strike.

TABLE 1
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TABLE 1. Comparison between different segments of the North Qinling Fault.

3.3 Strain field calculation

We collected GPS velocity field data published recently (Wang and Shen, 2020) and selected those with errors< 1.5 mm/a. The improved least-square collocation method, which has a good resolution and reliability, was employed here to calculate the regional strain fields (Zhang et al., 1998; Wu et al., 2009; Shen et al., 2015). In the calculation process, it was fundamental to identify the best smoothing factor D, as well as to select a suitable interval distance range (0–500 km) and step length (1 km), in order to meet the following conditions:

W=n=1#sta*2Zi*LiWt

where L is the weight of the distance correlation and Z is the weight of the spatial site distribution. In the calculation process, the data points over the threshold Lmax = 10 × D km (from the calculation point) are excluded, and the optimal smoothing factor D is obtained under the condition of satisfying Wt, as well as the velocity and strain tensors [Ux, Uy, τx, τxy, τy, ω] T of all the GPS stations. In case of a sparse station distribution, the selection function L(i) = 1/(1+ΔRi2/D2) is used instead, where ΔR is the distance between the station and the interpolation point. Station distribution and distance weighting were both considered to ensure the reliability and accuracy of the strain fields (see Figure 4).

FIGURE 4
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FIGURE 4. Shear strain, principal strain, active fault and modern earthquake distribution in the Weihe Basin (relocated earthquakes from January 1970 to May 2022).

3.4 Seismic b-value calculation

Data on modern earthquakes (that occurred between January 1970 and May 2022) were obtained from the China Earthquake Networks Center. The time series change of the minimum magnitude of completeness (Mc) in the Weihe Basin was qualitatively analyzed according to the magnitude-order method (Ogata et al., 1991) and the entire magnitude range (EMR) method (Woessner and Wiemer, 2005). The earthquake catalog of the Weihe Basin was analyzed starting from 1970, and Mc was determined considering it equal to ML2.0. Earthquakes ≥ Mc were selected and the least square method was used to calculate the b-values. Gridding was performed considering an interval of 0.2°, and earthquakes in the circular statistical unit with a radius of 30 km were selected. The number of events in each grid node had to be ≥ 20 in order to be considered for the calculations. For statistical grid nodes that could not meet the criteria, the statistical radius was increased to 50 km. If, after this, the number of samples was still < 20, the b-values were not calculated. The b-values are shown in Figure 5.

FIGURE 5
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FIGURE 5. Seismic b-values and active fault distribution in the Weihe Basin.

4 Results

4.1 Locking depths and slip rates

The distribution of GPS velocity field shows that the movement direction of the Weihe Basin is roughly SE–E. Additionally, the GPS velocity component profile fitting curve parallel to the fault is characterized by sinistral shear strain accumulation, while there is no obvious transverse compression deformation (Figure 3). The accumulation of horizontal shear strain varies along different segments, and the accumulated shear strain decreases from W to E. Detailed features were identified for each segment. 1) The GPS velocities obtained for the western segment of the fault (Qingjiangkou–Xitangyu), parallel to the fault strike, suggest an obvious sinistral strike-slip movement. The inversion results indicate a sinistral strike-slip velocity of 1.33 mm/a and a locking depth of 13.54 km. 2) The GPS velocities obtained for the middle segment of the fault (Xitangyu–Fengyukou), parallel to the fault strike, indicate an obvious sinistral strike-slip movement. The correspondent inversion results indicate a sinistral strike-slip velocity of 0.45 mm/a and a locking depth of 8.58 km. 3) The GPS velocities obtained for the eastern segment of the fault (Fengyukou–Daiyu), parallel to the fault strike, indicate an inapparent sinistral strike-slip movement. The correspondent inversion results indicate a sinistral strike-slip velocity of 0.36 mm/a and a locking depth of 21.46 km. 4) The GPS data obtained for the direction vertical to the fault strike indicate the absence of obvious tensions along the three segments.

4.2 Strain fields

Our GPS inversions showed that, in the Weihe Basin, strains have been controlled by the fault distribution, and been induced by the main fault activity; moreover, they are related to modern seismicity distribution (Figure 4).

4.2.1 Shear and principal strains in the Weihe Basin

The shear strain rate is overall higher in the eastern region and lower in the western region. A low-value area (< 1 × 10–8/a) was identified in the Xi’an Sag, in the southern-central part of the Weihe Basin: it is bounded by the North Qinling Fault to the S, the Lintong–Chang’an Fault to the E, and the Weihe Fault to the N. A median-value area (± 2 × 10–8/a) was instead identified in correspondence of the Lishan uplift: it is bounded by the North Qinling Fault to the S, the Lintong–Chang’an Fault to the W, and the Lishan Piedmont Fault to the N. Finally, a high-value area (> 4 × 10–8/a) was found in the Gushi Sag, in the northeastern part of the basin, where many modern small earthquakes have occurred. This corresponds to the intersection area of the Weihe Fault with the Kouzhen–Guanshan Fault, the North Weihe Fault, and the Weinan Plateau Fault. Changes in the principal strain rate and in the direction are regulated by active faults in the Weihe Basin. The western margin of the basin is mainly controlled by the Longxian–Qishan–Mazhao Fault; here, the approximate direction of the principal compressive strain is NE–E. The southern margin of the basin is instead mainly controlled by the North Qinling Fault, which induces a principal compressive strain in the W–E direction. Meanwhile, the western–middle segment of the North Qinling Fault is subjected to the W–E principal compressive strain (consistent with the fault strike direction). The eastern segment of the fault is instead affected by a fault zone characterized with a N–NE strike (which includes the Lintong–Chang’an Fault and the West Huashan Fault), and the direction of the principal compressive strain is also N–NE. In the northeastern part of the North Weihe Fault, the main compressive strain occur in the NE–E direction. Meanwhile, in the Gushi Sag, it occurs in the N–NW direction, and its high principal strain rate corresponds to the region characterized by a high concentration of modern earthquakes.

4.2.2 Shear and principal strains along the North Qinling Fault

The shear strain rate shows an obvious gradient at the intersection of the Weihe Basin with the Qinling Mountains, controlled by the North Qinling Fault. Along this fault, the shear strain rate in the N wall is lower than that in the S wall; moreover, the shear strain rate changes considerably along the fault strike. The shear strain rate values in the western-middle segments are lower than that in the eastern segment and quite constant. A high value was noted at the intersection of the eastern segment of North Qinling Fault with the Lintong-Chang’an Fault: here, the maximum observed shear strain rate is 4 × 10–8/a. The principal strain direction in the southern part of the basin is controlled by the North Qinling Fault and by the N–NE fault zone located to the E of it. The principal strain rate gradually increases from W to E along the North Qinling Fault, reaching its maximum value at the intersection of the North Qinling Fault with the Lintong–Chang’an Fault, where modern small earthquakes have not are rather weak.

4.3 Seismic b-values

The b-value distribution in the Weihe Basin is clearly shown in Figure 5. Higher and lower b-values occur in the eastern and western parts of the Weihe Basin, respectively. Along the North Qinling Fault, the b-values also differ significantly from W to E, and the eastern part has the lowest b-values in the Weihe Basin. The average b-values for the eastern segment of the North Qinling Fault and Weihe Basin (0.6 ± 0.1 and 0.8 ± 0.1, respectively) are both lower than the average b-values for the western–middle segment of the North Qinling Fault (1.0 ± 0.1) over the same period.

5 Discussion

5.1 Stability analysis

5.1.1 Locking depths

Cui et al. (2019) proposed locking depths of 7.7 ± 3.58 km and 10 ± 4.47 km for the study region, which are different from those determined in this study (13.54 km, 8.58 km, and 21.46 km). Most of the difference might be explained as follows. First, it is important to note that different data sources were used in Cui et al. (2019) and in this study: those authors utilized multi-stage precise leveling data across the North Qinling Fault, while we calculated the locking depths based on GPS horizontal velocities. The influence of large earthquakes on fault movement by the leveling data was not deducted. Meanwhile, during the processing of GPS data, the co-seismic deformation caused by large earthquakes was considered, and troublesome epochs derived from the horizontal velocities were corrected. In this case, the GPS velocity could in fact reflect the crustal deformation by fault movements. Second, the locking depths inversed by considering different fault movements in Cui et al. (2019) and in this study: the leveling data and the GPS data were influenced by the normal faulting and strike-slip movement, respectively. In Shi et al. (2020), inversion of GPS data was applied to investigate a back-arc fault in the Central Andes. In that instance it was demonstrated that, even when data and processing methods are consistent, the calculated locking depths of horizontal and vertical movements can be different. In addition, the ranges and source locations of data used in Cui et al. (2019) and in our study were different. Cui et al. (2019) used two leveling lines that crossed the fault at the intersection of its western and middle segments, as well as the intersection of its middle and eastern segments. While, we selected GPS sites distributed along the whole fault, selecting three profiles according to fault segmentation. In summary, though a variety of factors may influence the correlation between the locking depths from these two methods, the locking depths inverted from the horizontal (i.e., GPS data) and vertical (i.e., leveling data) movements are generally consistent: a greater locking depth is determined for the eastern section of the fault.

5.1.2 GPS and geological slip rates

GPS and geological slip rates provide information on the fault vertical and horizontal movements, respectively (Table 1). Therefore, it is difficult to directly compare the slip rates of different motion types by GPS inversion and geological methods. Besides, geological and GPS slip rates are constrained by different influential factors. GPS measurement involves transient (i.e., generally elastic and some viscous) and permanent (i.e., plastic) components in the present day, whereas geological records only include permanent strain (Meade and Hager, 2005) and depend on the reliability of offset measurements and geochronological data (Cowgill, 2007). Thus, the GPS slip rates tends to differ from geological slip rates along the North Qinling Fault. Below, we discuss fault GPS and geological slip rates separately.

The inversion of GPS data indicates that the slip rate is equal to the velocity below the locking depth currently, and that the slip rate decrease eastwards (Table 1). Notably, the slip rate of the West Qinling Fault is 2.5 ± 0.3 mm/a (Li et al., 2021): larger than that of the North Qinling Fault. This is consistent with the current dynamic background, in which the uplift of the Tibetan Plateau is causing a large-scale sinistral strike-slip movement. The North Qinling Fault, characterized by lower slip rates, is located at the end of the eastward spreading zone. The higher slip rate of the western segment might indicate that this segment is still in a post-seismic stage and is not locked at present. Overall, the GPS and geological slip rates are in the same order of magnitude, supporting and confirming the reliability of methods applied in this study. For the geological evidence, instead, provides information on the strength of single tectonic events in relation to fault activity, and suggests that the slip rate in the western segment is lower than in the middle-eastern segments (Table 1): fault activity and earthquake seismicity should be weaker in the western segment.

5.1.3 Prominence of the North Qinling Fault

The North Qinling Fault is a major structure in a boundary zone characterized by active tectonic blocks (i.e., the North China Block and the South China Block) in mainland China (Figure 2, Zhang et al., 2013), and separates the Weihe Basin from the Qinling Mountains. We collected evidence that the North Qinling Fault is the most active and largest structure in the Weihe Basin, and it subjects the area to a high earthquake hazard. The crust structure determined based on the receiving function and deep seismic reflection, clearly indicates that the North Qinling Fault cuts off the Moho, reaching a depth of about 40 km, while the other faults occurring in the basin cut off only the upper crust (Xu et al., 2014; Guo and Chen, 2016; Si et al., 2016; Li et al., 2017; Shen et al., 2022; Zhang et al., 2022). Besides, the results of a geological survey suggest these other faults, characterized by lower geological slip rates and activities, are capable of generating only moderate earthquakes, differently from the North Qinling Fault (Shaanxi Earthquake Agency, 1996). According to the above information, we can infer that the North Qinling Fault has a much higher activity and seismic potential than nearby (shallower cutting) faults. Therefore, our inversion results should mainly reflect the slip rates and locking depths of the North Qinling Fault.

5.2 Strike-slip movement of the North Qinling Fault

Some scholars argued that, since the Late Miocene–Quaternary, normal faulting has been predominant in the North Qinling Fault, which bounds the southern part of the Weihe Basin and controls its subsidence and sedimentation (Wang, 1965; Liu et al., 1981; Wang, 1986; Xie et al., 1991; Zhang et al., 1991; Li, 1992; Peng et al., 1992; Shaanxi Earthquake Agency, 1996; Han et al., 2001; Xie, 2011; Ren et al., 2012, 2013; Rao et al., 2014; Meng, 2017). Still, other studies suggest that the North Qinling Fault is currently characterized by a large-scale sinistral strike-slip movement, due to a NW–SE tensile stress affecting the Weihe Basin and caused by the eastward spreading of the Tibetan Plateau (Molnar and Tapponnier, 1975; Peltzer et al., 1985; Tapponnier et al., 1986; Zhang et al., 1995; Zhang et al., 1998; Zhang et al., 1999; Zhang et al., 2005; Zhang et al., 2019; Sun, 2005; Zhang et al., 2006; Sun and Xu, 2007; Liu et al., 2013).

In this study, the inversion of principal strain obtained from GPS data (Figure 4) indicate that strike-slip has been the primary movement mode of the North Qinling Fault for decades. Below, we discuss information suggesting that the North Qingling Fault is a sinistral strike-slip fault, whose shearing and tension control the formation of a pull-apart basin (i.e., the Weihe Basin) (Figure 6).

FIGURE 6
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FIGURE 6. A Structural model of the Weihe Basin. B Model of the pull-apart basin.

1) Geological survey has provided evidence of recent horizontal offset along most active faults in the Weihe Basin, and especially along the North Qinling Fault (Shentu et al., 1991; Peng et al., 1992; Liu et al., 2013.; Bai, 2018; Ma, 2020; Ma, 2020). 2) Prospecting and artificial seismic exploration have demonstrated that the crust in correspondence of the Weihe Basin is characterized by a large-scale “negative flower structure” (Zhang et al., 2021), resulting from shearing and tension. 3) Cenozoic sediments have a large thickness (> 7500 m) in the Weihe Basin, and the Quaternary sedimentary rate is high (465 m/Ma) (Sun and Xu, 2007). These are characteristics correspond to those typical of pull-apart basins. 4) The GPS velocity field suggests NW-SE movements in the Weihe Basin (England and Houseman, 1989; Clark and Royden, 2000; Qu et al., 2016), moreover, the stress field constrained by seismic activity and focal mechanism solutions indicates that the maximum horizontal principal stress direction is nearly EW along the North Qinling Fault (Yu et al., 2022), which is consistent with our studies.

5.3 Seismicity along the North Qinling Fault

5.3.1 Modern seismicity

To analyze modern seismicity along the North Qinling Fault, we selected relocated earthquakes from the period January 1970–May 2022 with the epicenter within 20 km from the reference profile following the direction of the fault strike, and drew the seismic depth transect along the North Qinling Fault (Figure 7). Although earthquakes involved in the transect refer to other faults, such as the Taochuan–Huxian Fault, the Lintong–Chang’an Fault and other secondary faults. Among them, the Taochuan–Huxian Fault can be regarded as a branch of the North Qinling Fault. Moreover, there is no explicit evidence that the Lintong–Chang’an Fault is a Holocene active fault. Hence, our seismic profile basically reflects the current seismicity along the North Qinling Fault.

FIGURE 7
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FIGURE 7. Elevation and seismic depth along the North Qinling Fault. A seismic gap can be identified in the area with sparse earthquakes.

The focal depth of the North Qinling Fault is generally within 30 km, but it is unevenly distributed along the fault. Notably, modern earthquakes have occurred mainly along the western and middle segments of the fault. In particular, a relatively high concentration of earthquakes was identified in the shallow layer (0–3 km) of the western and middle segments, while a clear seismic gap was revealed in the eastern segment. These facts highlight a sharp contrast in the seismicity of the western-middle and eastern segments.

5.3.2 Paleoearthquake

Although historical and modern earthquakes and rather weak along the North Qinling Fault, there is sufficient evidence of paleoearthquakes, prehistoric landslides, and barrier lakes caused by strong earthquakes along the fault (Bai, 2018; Huang et al., 2020; Yang, 2022). Paleoearthquake information can make up for deficiencies in historical and modern seismicity information and can be used to explore the occurrence regularity of strong earthquakes along active faults over long time scales (McCalpin, 1996; Caputo and Helly, 2008). Previous studies have shown that, along the North Qinling Fault, the average recurrence interval of prehistorical earthquakes is about 3,000 years (Zhang et al., 1990; Shaanxi Earthquake Agency, 1996; Bai, 2018). By combining this information with the occurrence time of the last major earthquake, we can infer that the fault is now in a pre-seismic stage: it is approaching the recurrence period of large earthquakes.

5.4 Seismic potential of the North Qinling Fault

5.4.1 Segmentation characteristics

In this study, we adopted a segmentation that reflects the geometry of the fault, as determined from the geological survey (Zhang et al., 1991; Shaanxi Earthquake Agency, 1996; Bai, 2018). Inversions of GPS data and b-values were used to define the diversity between segments. The eastern segment, having the deepest locking depth, the highest shear and principal strain rates, the lowest b-values, and presenting a seismic gap, is the most unique. These differences suggest that, even under a homogeneous tectonic background, different segments would experience discrepant geological and present-day activities. This justifies our choice of the segmentation method, which is able to provide detailed spatial information on fault activity. On this basis, we conducted a comprehensive analysis of the fault seismic potential and timing.

5.4.2 b-values and strain fields

The b-value is typically inversely related with effective stress and closely related to the fault asperity. Large earthquakes usually occur in areas characterized by low b-values, and where a higher amount of stress is accumulated (Wiemer and Wyss, 1997; Wyss et al., 2004; Yi et al., 2006; Zhu and Huang., 2022). Thus, we employed the seismic b-value as an indicator of accumulated stress to further discuss the seismic potential of the fault. The lower average b-values of the eastern segment (Figure 5), compared to those of the other segments, indicates that a higher amount of stress is accumulated here and hence, that this area has a higher seismic potential.

The shear and principal strains typically reflect the current stress state of the crust. We noted that the shear strain and principal strain rates are both higher in the eastern segment than in the western-middle segments of the North Qinling Fault: the highest strain rates are registered at the intersection of the North Qinling Fault with the Lintong–Chang’an Fault. However, unlike the Gushi Sag (in the northeastern part of the basin), the eastern segment of the North Qinling Fault is not a seismically active area (Figure 4). Overall, the high strain rates (Figure 4) and low average b-values (Figure 5) of the eastern segment, as well as the occurrence of a seismic gap (Figure 7), indicate that a large amount energy should have accumulated in this area.

5.4.3 Moment magnitude and focal depth-frequency

Extensive research has been conducted on the relationship between earthquake moment magnitude and surface rupture length (Tocher, 1958; Slemmos, 1977; Long et al., 2006; Ran et al., 2011). In this paper, according to the empirical relationship between moment magnitude (MW) and rupture length (L) in global strike-slip faults (MW = 5.16 + 1.12 L gL, where L is in km) (Wells and Coppersmith, 1994), as well as the empirical relationship MW = 2/3 (lgMo−16.1) (Chen and Liu, 2018), we calculated the moment magnitude and the seismic moment of the western, middle, and eastern segments of the North Qinling Fault. Our statistical results (Table 1) indicate that this fault has the capability of generating earthquakes with MW > 7.

Our calculation demonstrates a strong earthquake capacity for the North Qinling Fault. The western-middle segments have shallower locking depths (i.e., 13.54 km and 8.58 km, respectively) than the eastern segment (i.e., 21.46 km) and present earthquake clustering, implying energy release. This information, combined with other results obtained in this study, implies that the eastern segment may be locked. Below, this issue is discussed quantitatively by considering the focal depth.

Previous research has demonstrated a good correspondence between the 90% seismic cutoff focal depth and the locking depth (Miller and Furlong, 1988; Williams, 1996; Richards and Shearer, 2000; Bonner et al., 2003). A comparative analysis of these depths can thus help clarifying the seismic potential of a fault. When the locking depth is shallower than the 90% seismic cutoff focal depth, “deep creep” occurs between the locking depth and the focal depth layers; in this case, stress mainly accumulates above the locking depth and major earthquakes are unlikely. When the locking depth is close to the 90% seismic cutoff depth, however, the fault is locked (Wdowinski, 2009; Schmittbuhl et al., 2015). Here, we discuss the seismic potential of the Qinling Fault by comparing the 90% seismic cutoff focal depth (within a width of 20 km and for different segments) with the locking depth (Figure 8; Table 1). The result indicates that the locking depth of the western segment should be 13.54 km [shallower than the 90% seismic cutoff depth (18.4 km)], suggesting the occurrence of “deep creep” in the layer between 13.45 and 18.4 km. The locking depth of the middle segment should be 8.58 km [only half of the 90% seismic cutoff depth (16.97 km)], suggesting the occurrence of “deep creep” in the layer between 8.58 and 16.97 km. Finally, the locking depth of this eastern segment should be 21.46 km [similar to the 90% seismic cutoff depth (24 km)], indicating that this segment is locked.

FIGURE 8
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FIGURE 8. Focal depth distribution along the North Qinling Fault. The orange, green, and purple lines represent the 90%, 95%, and 99% seismic cutoff depths, respectively.

Overall, the results of our analyses suggest that the North Qinling Fault is presently in a pre-seismic stage and exhibits significant segmentation characteristics: the eastern segment, characterized by higher strain rates and accumulated stress, is obviously locked and capable of generating strong earthquakes in the near future.

6 Conclusion

Based on GPS data and seismic activity, we inverted slip rate, locking depth, shear and principal strain fields to determine the present-day activity and seismic potential of the North Qinling Fault. Our main findings are summarized below.

The North Qinling Fault, characterized by a sinistral strike-slip movement, is currently in a pre-seismic stage and makes the Weihe Basin an area of high earthquake hazard. This fault can in fact potentially generate MW > 7 earthquakes. Its eastern segment, where the locking depth is close to the 90% seismic cutoff focal depth, has relatively higher shear and principal strain rates, low b-values, and presents a seismic gap. These traits collectively suggest that the eastern segment is currently locked, and that it has a strong seismic potential that might be expressed in the near future. Therefore, a continuous, careful monitoring of this area is required.

Data availability statement

The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.

Author contributions

CY: Conceptualization, formal analysis, funding acquisition, methodology, software, visualization, writing—original draft. LJ: Formal analysis, methodology, writing—review and editing. YY: Conceptualization, writing—review and editing, funding acquisition. LS: Conceptualization, software. YW: Software. HS: Conceptualization.

Funding

This work was jointly supported by the Natural Science Basic Research Program of Shaanxi Province (Grant No. 2022JQ-298), the National Natural Science Foundation of China (Grant No. 42004048), and the Seismological Research Tracking Project of China Earthquake Administration (Grant No. 2022010212). Most figures were generated by using the Generic Mapping Tools software (Wessel and Smith, 1995). The relocated earthquake catalogue was provided by Liu C. and Zhang E. H.

Acknowledgments

The authors are grateful to Shi F. Q. for helpful discussion, and to Zhang W. T. and Chen X. X. for software assistance.

Conflict of interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Publisher’s note

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Keywords: North Qinling Fault, GPS velocity field, locking depth, slip rate, seismicity distribution, seismic potential

Citation: Yang C, Ji L, Yang Y, Su L, Wang Y and Shi H (2023) Present-day activity and seismic potential of the north Qinling fault, southern ordos block, central China, as revealed from GPS data and seismicity. Front. Earth Sci. 10:1058243. doi: 10.3389/feart.2022.1058243

Received: 30 September 2022; Accepted: 29 November 2022;
Published: 20 January 2023.

Edited by:

Xinjian Shan, Institute of Geology, China Earthquake Administration, China

Reviewed by:

Zhongtai He, Ministry of Emergency Management, China
Dongliang Liu, Chinese Academy of Geological Sciences (CAGS), China

Copyright © 2023 Yang, Ji, Yang, Su, Wang and Shi. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.

*Correspondence: Lingyun Ji, amlsaW5neXVuQHNtYWMuYWMuY24=

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