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Gravity gradient tensor analysis to an active fault: a case study at the Togigawa Nangan fault, Noto Peninsula, central Japan
Earth, Planets and Space volume 71, Article number: 107 (2019)
Abstract
Gravity gradient tensor analysis has been a powerful tool for investigating subsurface structures and recently its application to a twodimensional fault structure has been developed. To elucidate the faulting type and spatial extent, specifically the continuity and the size, of the subsurface fault structure of an active fault through gravity gradient tensor analysis, we analyzed Bouguer anomalies, which were composed of dense gravity measurement data over the land and seafloor, and indices calculated from a gravity gradient tensor around the Togigawa Nangan fault (TNF), Noto Peninsula, central Japan. The features of Bouguer anomalies and their first horizontal and vertical derivatives demonstrate clearly that the TNF is a reverse fault dipping to the southeast. Furthermore, the combination of those derivatives and the dimensionality index revealed that the spatial extent of the subsurface fault structure is coincident with that of the surface fault trace and that it shows no evidence of connecting the TNF with surrounding active faults. Furthermore, the dip angle of the subsurface fault structure was estimated as 45°–60° from the minimum eigenvectors of the gravity gradient tensor. We confirmed that this result is coincident with the dip angle estimated using the twodimensional Talwani’s method. This high dip angle as a reverse fault suggests that the TNF has experienced inversion tectonics.
Introduction
Elucidating the subsurface fault structure of an active fault is important for understanding regional tectonics and seismic risks. Geophysical surveys are useful for investigating subsurface structures. Fault movements displace the basement, causing gravity anomalies around an active fault. Especially, vertical displacement of the basement causes a steep change in Bouguer anomalies across the fault. Therefore, the first horizontal derivative (HD) and the first vertical derivative (VD) of Bouguer anomalies are often used to highlight subsurface fault structures. Wada et al. (2017), based on the continuity of high HD and the zero isoline of VD for two active fault zones on the east margin of the Niigata Plain in central Japan, inferred that subsurface fault structures are continuous. Recently, other methods to investigate the subsurface fault structure, especially for the dip angle of a fault, have been developed using the gravity gradient tensor (Kusumoto 2015, 2017). For the 2016 Kumamoto earthquake in Japan, Kusumoto (2016) used eigenvectors of the gravity gradient tensor to estimate the dip angle of the KumamotoOoita tectonic line, which includes the source fault of the earthquake, as approximately 65° (Beiki and Pedersen 2010). Matsumoto et al. (2016) also analyzed gravity data around the 2016 Kumamoto earthquake source fault and discussed the faulting type and segmentation of the source fault through features obtained from the gravity gradient tensor. Nevertheless, reported applications of the gravity gradient tensor to analyses of the subsurface structure of active faults are few. More case studies must be conducted to examine its effectiveness.
The study area is the western Noto Peninsula, central Japan, where dense gravity surveys have been conducted mainly by Kanazawa University (Honda et al. 2012) (Fig. 1). The Noto Peninsula is composed mainly of Oligocene to Early Miocene volcanic rocks and post Oligocene sediment rocks (e.g., Kaseno 1993) (Fig. 2). These volcanic rocks erupted during the rifting event of the backarc basin of the Japanese islands. The rifting ceased during the Middle Miocene. This rifting formed normal faults around the Noto Peninsula. Some of the normal faults have been reactivated as reverse faults because of the compressive stress associated with forearc subduction (e.g., Katagawa et al. 2005).
Active Fault Research Group (1991) reported several active faults in this area, such as the Togigawa Nangan fault (TNF) (Figs. 1 and 2). Based on geomorphological features, Active Fault Research Group (1991) reported that the TNF is a reverse fault with uplift on the southeastern side. Imaizumi et al. (2018) extended the eastern end of the TNF through reevaluation of geomorphological features (Figs. 1 and 2). This fault is located along the boundary between late Pleistocene to Holocene sediments/sand dune deposits and Miocene andesite on the ground surface (Fig. 2).
This study conducted a dense gravity survey and created a detailed gravity anomaly map around the TNF. We elucidate features of gravity anomalies and indices derived from the gravity gradient tensor around the TNF and discuss the faulting type, the continuity and size, and the dip angle of the TNF.
Data and method
Gravity measurement, compilation, and corrections
Gravity data used for this study consist mainly of two datasets. The first comprises data measured on land; the second includes data of the seafloor (Fig. 1). We conducted a gravity survey on land, around TNF using a Scintrex CG3M gravimeter from February 26 through September 11 in 2018 and obtained 279 gravity data (Fig. 1). For analysis of the twodimensional density structure, we set a profile across the TNF and conducted a gravity survey with an interval of 25–50 m and to a maximum 173 m on the profile (Fig. 1). The positions of gravity measurement points were obtained from Global Navigation Satellite System (GNSS) observations. In the case of poor location of GNSS, that is, the solution is not fix, we used a 10m mesh digital elevation model (DEM), published by the Geospatial Information Authority of Japan, for locating. For the points on the profile, we used a total station for locating. Gravity measurement of the seafloor was conducted by Hokuriku Electric Power Company from May 20 through June 20 in 2018 (Ishida et al. 2018). They used a Scintrex INO ocean bottom gravity meter to obtain 275 gravity data in an approximately 40 km × 10 km area west of the Noto Peninsula (Additional file 1: Figure S1). The points presented in Fig. 1 do not cover all areas for which gravity measurements were conducted on the seafloor. These gravity data from the seafloor filled a clearly apparent gap left by earlier gravity measurement data published by the Geological Survey of Japan (2013) and Murata et al. (2018) for the sea area (Fig. 1).
In addition to the data described above, we compiled gravity data reported by the Geographical Survey Institute (2006), Yamamoto et al. (2011), Honda et al. (2012), and the Geological Survey of Japan (2013). Data of the Geological Survey of Japan (2013) include data of shipboard gravity measurements described above. We applied terrain correction with the 10m mesh DEM, and a plain trend correction, together with normal correction procedures (e.g., tide, drift, freeair, and Bouguer corrections), to the compiled gravity data. The values of the density used for the terrain and the Bouguer corrections are 2300 kg/m^{3} because we used Bouguer anomaly data created from the shipboard gravity measurements with correction density of 2300 kg/m^{3} (Geological Survey of Japan 2013). These values are close to the optimum correction density of 2350 kg/m^{3} in the large area including most of the Noto Peninsula (Murata et al. 2018). Furthermore, we applied a lowpass filter with a cutoff wavelength of 3000 m to the Bouguer anomalies as a Bouguer anomaly map for the analysis of the gravity gradient tensor (Fig. 1).
Estimation of gravity gradient tensor and related indices
The gravity gradient tensor is defined by the partial derivatives of the gravity vector (g_{x}, g_{y}, g_{z}) as
Assuming a Bouguer anomaly as g_{z}, as measured on the x–y plane, the gravity gradient tensor is calculated using the Fourier transform of g_{z} as proposed by Mickus and Hinojosa (2001). From the gravity gradient tensor, the first horizontal derivative (HD), the first vertical derivative (VD), and the normalized total horizontal derivative (TDX) (Cooper and Cowan 2006) are defined as
These indices are useful to detect a subsurface density discontinuity such as a fault structure. The strike and dip angles of a twodimensional causative body can be estimated from the minimum and maximum eigenvectors of a gravity gradient tensor (Beiki 2013). Kusumoto (2015) demonstrated that the dip angle of a fault plane can be estimated from the maximum eigenvector. Recently, Kusumoto (2017) demonstrated from a numerical simulation that the dip of the minimum eigenvector followed the dip of a reverse fault. Using the minimum eigenvector, he estimated the dip angle of a reverse fault in central Japan: the Kurehayama fault. He emphasized the importance of the selection of the eigenvector by consideration of the faulting type: a normal fault or a reverse fault. For a reverse fault, the dip angle defined by the minimum eigenvector of a gravity gradient tensor (\(\nu_{3x} , \nu_{3y} , \nu_{3z}\)) is given as
The geological setting of this study area is similar to that of Kusumoto (2017). We therefore used this formulation to estimate the TNF dip angle. The dimensionality index D_{i} is defined by using the eigenvalues \(\lambda_{1} , \lambda_{2} , \lambda_{3}\), of a gravity gradient tensor as
where \(I_{1} = \lambda_{1} \lambda_{2} + \lambda_{2} \lambda_{3} + \lambda_{1} \lambda_{3}\) and \(I_{2} = \lambda_{1} \lambda_{2} \lambda_{3}\) (Pedersen and Rasmussen 1990). D_{i} indicates whether the subsurface structure is approximately twodimensional (D_{i} approaches 0) or threedimensional (D_{i} approaches 1).
Twodimensional Talwani’s method
In addition to the gravity gradient tensor analysis, we applied the twodimensional (2D) Talwani’s method (Talwani et al. 1959) to verify the subsurface density structure of the TNF, especially for the dip angle, obtained through gravity gradient tensor analysis. The Bouguer anomaly data for the 2D density structure analysis were produced from the gravity data measured on the profile traversing the TNF (Fig. 1). We set a line across the TNF as shown in Fig. 1 and projected the observed Bouguer anomalies on the profile onto the line. After the projection, we smoothed and resampled the data with an interval of 100 m using the trend 1D command of Generic Mapping Tools (Wessel and Smith 1998) (Fig. 3a).
We assume for these analyses that the density structure mainly comprises two layers: andesite distributed widely in and around the analyzed area, and granite as the basement rock in the Noto Peninsula. In addition, a sediment layer lies on top of the geological features in and around the analyzed area (Fig. 2). To reduce tradeoff between the model parameters, we fix several parameters as follows. The andesite density is set as 2300 kg/m^{3}. That of granite is set as 2650 kg/m^{3}. Based on the boring data (Hokuriku Geological Information Utilization Meeting 2019), the sediment layer density and thickness are set, respectively, as 1700 kg/m^{3} and 20 m. Furthermore, the upheaved part of the basement is assumed to have a parallelogram shape. The model parameters of the 2D density structure are presented in Fig. 3b. Two boring data to the south of the analyzed area (Fig. 1) indicate that the basement depth is 1000 m (Sutou et al. 2004). Sutou et al. (2004) estimated the basement depth of the southern side of the analyzed area as 500–1000 m. The geological map shows that Funatsu granite, which is recognized as the basement in this region, is distributed on the ground to the north of the analyzed area (Fig. 2). Therefore, we set the maximum depth of the basement to be 1000 m for the following modeling. Search ranges and intervals of the model parameters are 200–1000 m and 100 m, respectively, for the depth of the basement in the nonupheaval part (Db), 100–800 m and 100 m for the depth of the basement in the upheaval part (Dt), 20°–80° and 5° for the dip angle (θ), and 1500–2500 m and 100 m for the horizontal length of the upheaval part (L). The optimum model is selected by minimizing the L2 norm between the resampled and calculated Bouguer anomalies, defined as \(\mathop \sum \nolimits_{i} \left {O_{i}  C_{i} } \right^{2}\), where at the ith point on the line, O_{i} is the resampled Bouguer anomaly on the line and C_{i} is the Bouguer anomaly calculated from a model using the 2D Talwani’s method. We estimate the 95% confidence ranges of the optimum parameters based on the Chi square distribution as well.
Results and discussion
Faulting type, continuity and size, and dip of the TNF
We discuss here the faulting type, the size, and the dip angle of the TNF from the features of the Bouguer anomalies and the indices derived from the gravity gradient tensor. Around the TNF, the Bouguer anomalies are high on the southeastern side and low in the northwestern side of the TNF, indicating that the basement depth of the southeastern side is shallower than that of the northwestern side (Fig. 1). For indices derived from the gravity gradient tensor, high HD (> 2 mGal/km) and high TDX (> 75°) are distributed parallel to the strike of the TNF mainly in the southeastern side of the TNF (Fig. 4). We recognize that VD is high on the southeastern side and low on the northwestern side of the TNF. This difference also indicates that the basement depth of the southeastern side is shallower than that of the northwestern side. Furthermore, the zero isoline of VD, which illustrates a subsurface geological discontinuity, lies parallel to the strike of the TNF mainly in the southeastern side. These features indicate that the TNF is a reverse fault dipping to the southeast. This fault type estimated from the indices is coincident with that based on geological and geomorphologic observations (Active Fault Research Group 1991; Imaizumi et al. 2018).
The spatial extent of high HD along the TNF is almost identical to that of the surface trace of the TNF reported by Imaizumi et al. (2018) (Fig. 4). The high TDX zone along the TNF is crossed by other high TDX zones with north–south orientation near the coast and at the northeastern extension of the TNF. The zero isoline of VD along the TNF also bends perpendicularly near the coast and at the northeastern extension of the TNF. Low D_{i} (< 0.5), which indicates that the subsurface structure is close to twodimensional one, is distributed over an almost identical range of the total length of the TNF and high D_{i} (> 0.5), which indicates that the subsurface structure is nearly threedimensional near both edges of the TNF. We infer from these features that the size of the subsurface fault structure of the TNF is comparable to that of the surface trace. It is also noteworthy that the TNF shows no continuous structure with surrounding active faults based on the indices calculated from the gravity gradient tensor.
To estimate a fault dip angle, Kusumoto (2016) proposed that \(\upbeta_{ \text{min} }\) of a fault structure should be evaluated in areas with high HD and low D_{i} because a twodimensional subsurface fault structure satisfies both these conditions. Figure 4 shows the distribution of \(\upbeta_{ \text{min} }\) in areas with HD ≥ 2 mGal/km and D_{i} < 0.5. We took the absolute value of \(\upbeta_{ \text{min} }\) for use in the plot because we are concerned about the dip angle. From \(\upbeta_{ \text{min} }\) along the TNF, we can estimate that the dip angle of the TNF is approximately 45°–60°.
Twodimensional density structure analysis
To assess the adequacy of the dip angle estimated from the gravity gradient tensor analysis in Subsect. “Faulting type, continuity and size, and dip of the TNF” section, this subsection presents estimation of the dip angle of the TNF using the 2D Talwani’s method. For calculation, we set the value of the resampled gravity anomaly on the fault trace, at Distance = 0 in Fig. 3a, as 0. Figure 3a compares the observed Bouguer anomalies projected onto the line across the TNF and the resampled ones to the synthetic ones calculated from the optimum subsurface density structure using the 2D Talwani’s method. The optimum parameters, which provide the minimum L2 norm, and those 95% confidence range in the parentheses of Db, Dt, θ, and L are, respectively, 800 m (600–1000 m), 200 m (100–300 m), 55° (40–65°), and 2000 m (1900–2100 m). The calculated Bouguer anomalies well reproduced the resampled ones. We also recognize the tradeoff between the parameters: L and θ become large and Db becomes small as Dt becomes small, and vice versa. The optimum parameters are essentially sensitive to the assumed density: those for the andesite density of 2200 kg/m^{3} are Db of 800 m, Dt of 300 m, θ of 60°, and L of 2000 m and those for the andesite density of 2400 kg/m^{3} are Db of 900 m, Dt of 100 m, θ of 55°, and L of 2000 m. It is important that a high dip angle is estimated as the optimum parameter irrespective of the assumed density of the andesite.
The optimum dip angle of 55° obtained using the 2D Talwani’s method is coincident with that estimated from the gravity gradient tensor analysis. This result supports not only the estimation of the dip angle of the gravity gradient tensor analysis but also the validity of the estimation of the dip angle of a reverse fault from the minimum eigenvector proposed by Kusumoto (2017). This result also shows that the gravity gradient tensor analysis is as useful as the 2D Talwani’s method for estimating the dip angle of a fault structure and has an advantage of estimating widely the distribution of the dip angle.
Implications for TNF formation processes
The TNF dip angle estimated as explained in the preceding two subsections is high for a reverse fault. We discuss here what this high dip angle means. The 2007 Noto Hanto earthquake (M_{JMA} 6.9) occurred on the Noto Peninsula about 15 km north of the TNF (Fig. 1). The source mechanism is a reverse fault with right lateral slip. Seismic and geodetic analyses indicate the dip angle of the fault plane as 60° (e.g., Hiramatsu et al. 2008; Kato et al. 2008; Sakai et al. 2008). Consequently, the estimated dip angle of the TNF, as a reverse fault with high dip angle, is coincident with that of the 2007 Noto Hanto earthquake. Furthermore, the strike of the TNF, with a northeast to southwest orientation, is the same as that of the 2007 Noto Hanto earthquake. A reverse fault with a high dip angle has been formed by inversion tectonics (e.g., Nakamura 1992). Previous reports have described that some active faults in sea areas around the Noto Peninsula, including the source fault of the 2007 Noto Hanto earthquake, have experienced inversion tectonics (Yoshikawa et al. 2002; Katagawa et al. 2005; Okamura 2007). In other words, those faults have been formed as normal faults accompanying the opening of the Sea of Japan. They have reactivated as reverse faults by crustal shortening initiated from the late Miocene. Inversion tectonics of this kind were inferred for the 2004 mid–Niigata Prefecture earthquake, which occurred in a similar tectonic setting in coastal areas of the Sea of Japan (Kato et al. 2006). In this case also, we infer that the TNF might have experienced the inversion tectonics.
Conclusions
We have conducted gravity anomaly and gravity gradient tensor analyses around the Togigawa Nangan fault (TNF) of the Noto Peninsula, central Japan. Indices such as the first horizontal and vertical derivatives derived from the gravity gradient tensor, as well as Bouguer anomalies, indicate that the TNF is a reverse fault dipping to southeast. We illustrate the subsurface fault structure as an area with a high first horizontal derivative and a low dimensionality index along the TNF. The spatial extent of the area is comparable to the total length of the surface trace of the TNF. We observe no continuity between the TNF and other surrounding active faults. The minimum eigenvectors of the gravity gradient tensor indicate the dip angle of the TNF as 45°–60°. Modeling using the 2D Talwani’s method supports this dip angle. Comparison of the dip angle of the TNF to those of the source fault of recent large earthquakes in/around the Noto Peninsula suggests that the TNF has experienced inversion tectonics.
Availability of data and materials
Datasets of gravity anomalies used for this study are available from the corresponding author on reasonable request.
Abbreviations
 TNF:

Togigawa Nangan fault
 HD:

first horizontal derivative
 VD:

first vertical derivative
 GNSS:

Global Navigation Satellite System
 DEM:

digital elevation model
 TDX:

normalized total horizontal derivative
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Acknowledgements
We used gravity data reported by Yamamoto et al. (2011), Geological Survey of Japan (2013), Geographical Survey Institute (2006), and Ishida et al. (2018). We also used the DEM with a 10 m mesh provided by Geospatial Information Authority of Japan and boring data provided by Hokuriku Geological Information Utilization Meeting. All figures were created using Generic Mapping Tools software (Wessel and Smith 1998). Constructive comments from anonymous reviewers are useful to improve the manuscript.
Funding
The analyses conducted for this study were partly supported by JSPS KAKENHI Grant Number 17K05629.
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YH and MH designed this study. AS, SI, WK, and MH took gravity measurements. YH and AS conducted analyses. YH drafted the manuscript. All authors read and approved the final manuscript.
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Correspondence to Yoshihiro Hiramatsu.
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Hiramatsu, Y., Sawada, A., Kobayashi, W. et al. Gravity gradient tensor analysis to an active fault: a case study at the Togigawa Nangan fault, Noto Peninsula, central Japan. Earth Planets Space 71, 107 (2019). https://doi.org/10.1186/s4062301910885
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Keywords
 Active fault
 Bouguer anomaly
 Dip angle
 Twodimensional Talwani’s method
 Inversion tectonics