Abstract
The southeast coastal areas in China have distributed lots of granite outcrops of different periods. Previous research has shown that granite geothermal reservoirs are also distributed under sedimentary basins in these areas, such as in Zhangzhou basin. Therefore, granites with fractures buried in deep can be used as a potential deep geothermal reservoir in these areas. In order to study geological conditions of the deep granite reservoir and discuss the genesis of the deep granite geothermal system, rock geochemistry and zircon U-Pb chronology from outcrop and parts of the drilling cores of granitic rocks have been analyzed, combined with the anatomy of the deep seismic data and electromagnetic detection data in selected area. Based on the results of geochemistry and zircon U-Pb chronology, most granites in this area are of Yanshanian periods. Based on the seismic data, the thickness of the overlying strata on granite in Huangshadong area of Huizhou City is up to 1.5 km. According to the regional geological survey, multi-stage joints are developed in the granite, and most of hot springs rise from intersection of fracture with different directions to the surface. The heat source in the study area mainly comes from the mantle carried up by the deep NNE-trending faults. There are a large number of thermal springs at the intersection of the surface and the NW-trending fault, and the NW-trending fault provides the drainage conditions for the upwelling of underground thermal springs. There is a huge amount of deep granite geothermal resources in the southeast coastal area. The analysis of deep granite geological conditions and genetic models can provide guidance for the evaluation of deep granite geothermal resources and the further optimization of favorable zones in these areas.
Introduction
Geothermal resources, as a renewable and clean energy, have been widely used globally in recent years, and the utilization has been increasing year by year (; ; ). Recently, most of the geothermal resources under exploitation and utilization are hydrothermal geothermal resource, which is widely distributed in southeastern areas of China (). Deep geothermal resources are considered as an important part of future energy supply due to their huge thermal energy storage and reserves. Most of the deep geothermal reservoir are granite (), and Metamorphic rocks () beneath the sedimentary basins and numerous studies have shown that the granite radioactive heat production has significant contribution to the heat source, such as Australia Cooper basin geothermal field caused by granites with intrusion age less than 0.5 Ma (), Rose-manowes geothermal field in England due to Early Permian granite heat generation (), the Soultz geothermal field in France due to Late Paleozoic granite heat generation ().
In the southeast coastal area of China, ground or near surface geothermal manifestations are widely distributed, such as hot springs and other surface heat. They are mainly located in the fractures within igneous rock, such granites. Granites in South China are widely distributed, with an outcropping area of 20,000 km2, accounting for about 1/5 of the area, and it is considered to be formed in three phases, i.e., Caledonian, Indosinian and Yanshanian period () (Figure 1). Radioactive elements from those granites such as U, Th, K, are important radioactive elements to generate heat by atom decaying. Meanwhile, Southeast coastal areas in China is the second largest region with high heat flow value (). analyzed the gravity anomaly in Guangdong province and concluded that the decay of thermal elements in granite may be an important part of the geothermal heat sources in the southeast coastal areas. The region is rich in geothermal resources, covering medium-low temperature, medium-high temperature and high-temperature geothermal resources.
FIGURE 1
In order to further study geological conditions of the deep granite reservoir and discuss the genesis model of the deep granite geothermal system, this paper adopted rock samples from outcrops and parts of the drilling core rocks to analyze the formation background of granite and discuss its geothermal significance to the southeast region in China.
Geological Setting
Geologically, the southeast coastal region of China is part of the Cathaysia block (
Granite reservoirs are distributed among the southeastern coastal areas, such as in Zhangzhou, Fuzhou, Fengshun, Yangjiang, and southern Hainan Province. In these areas, the distribution of reservoir is mainly controlled by NE-trending faults. Most of these granites were formed during the Yanshanian period. There are two types of heat source: Crust source originating from radiogenic heat from K-, Th- and U-bearing minerals of granites and mantle source connecting to the nearby ground by the deep faults. In the Quaternary, most of the radiogenic heat of granite was lost along the fault zone and could not constitute a source of geothermal heat in the fault. Therefore, it is easy to form deep fracture zone and become the channel for hot water to migrate from the deep mantle. In southeast coastal area, 74% of hot springs are located in fault zone or lithological contact zone in magmatic plutons.
The distribution of most granite geothermal fields are mainly located in basins, such as Fuzhou basin, Zhangzhou basin, Sanshui basin (Figure 1). They are mainly controlled by the deep and large fault in NE direction, and most of them are along the Neo-Cathaysian faults. The zone has experienced many strong tectonic movements and multiple periods of magma intrusion, resulting in secondary faults, rock mass fragmentation and joint fractures near the fault zone, providing space and channels for the storage and migration of geothermal fluids. At the same time, the tectonic activities of deep and large faults not only promote the formation of heat storage space, but also communicate the spatial connection between deep geothermal fluids and shallow geothermal reservoirs, becoming an important heat transfer channel in geothermal fields. From the regional analysis, most of the geothermal fields are linear distribution along the fault zone, mainly exposed on the deep fault axis. The rest are mostly distributed among the deep and large faults, which are locally influenced by the secondary NW tensioned water-conducting faults or pinnate faults. The distribution of heat flow in South China is shown in Figure 2. It contains three obvious thermal structure divisions: Eastern, central and southwestern regions. The eastern and southwestern regions are characterized by high heat flow, while the heat flow in the central region is relatively lower. The heat flow in the eastern and southwestern regions are generally higher than 70 mW/m2, while that in the central region is lower than 60 mW/m2. In the eastern region, there are 2 NE-trending high value abnormal belts along the Fuzhou-Zhangzhou zone. These two anomaly zones are characterized by high heat flow values (>80 mW/m2, locally up to 220 mW/m2). The average heat flow in northern Jiangsu Basin is 71.2 mW/m2, while that in southern Jiangsu and southern Anhui areas is 62.7 mW/m2. In the central region, from Baise to Dabie Mountains, lower heat flow is distributed along the NE-direction. In the southwestern region, the higher heat flow is concentrated only in southwestern Yunnan. The average of heat flow in the north of Sichuan Basin is 53.6 mW/m2, while that in southern Yunnan is 76.7 mW/m2. In the middle of northern Jianghan Basin, the heat flow is lower in the north and higher in the south. The average heat flow in the north of the fault is 47.8 mW/m2, and that in the south is 61.6 mW/m2. The average heat flow value of 64.2 mW/m2 in southern China is higher than that of 61 mW/m2 in other mainland parts in China (Wang et al., 1990), which is close with that of the globe for 65 mW/m2 (Yuan, 2006). The abnormally high value areas in South China are mainly distributed in the suture zone or regional deep fault zone. Some granite geothermal reservoirs in typical areas in South China have been studied by previous researchers, including Fuzhou, Zhangzhou, Huizhou, Yangjiang areas (Zhu 2015; Yang 2016; Zhang et al., 2021; Zhou, 2015). The Fujian granite geothermal reservoir is located around Fuzhou basin (Figure 3A). Most of them are Yanshanian granites. Early detailed geothermal resource exploration shows that the geothermal reservoir is an area of 9 km2 with a north-south length of about 5 km and an east-west width of about 2 km. The basement consists of Yanshanian granodiorite, intrusions of medium-coarse biotite granite and fine-grained granite, as well as a large number of intermediate-acid and intermediate-basic dike rocks (Zhu 2015). Zhangzhou granite geothermal reservoir is located around Zhangzhou Basin (Figure 3B). The Quaternary sediments on granite are a set of Marine and continental deposits with a thickness of 20 m–30 m. There are several granite rock masses, such as Zhangzhou granite, Chengxi granite and Maping granite, which are around Zhangzhou geothermal field (Yang, 2016). In Huizhou area, Huangshadong geothermal field is located in the northeast of Huizhou city (Figure 3C). This area has experienced several periods of intense magmatic events since the Paleozoic. The granites include Caledonian granodiorite, Indo-Chinese granites, Yanshanian granites and Neogene tholeiitic basaltic dikes (Zhang et al., 2021). Xinzhou complex granite is located in the coastal area of west Guangdong, Yunkai block geologically, on the southwest Cathaysia block, with a total outcropping area of 350 km2. The rock is composed of medium-coarse-grained macro porphyritic biotite monzonite and fine-grained porphyritic biotite quartz syenite, surrounded by the Proterozoic Yunkai Group plagioclase gneiss. The latest outcropped strata around this area are Late Cretaceous sandstone and conglomerate, distributed with NE direction. Xinzhou complex granite mainly includes Xinzhou granite, Dongping granite and Naqin rock granite (Zhou, 2015).
FIGURE 2

The Heat flow map distribution of the study area (Modified after
FIGURE 3

Simplified geological map of selected regions in Southeast Coastal Area: (A) Fuzhou area; (B) Zhangzhou area; (C) Huizhou area (Modified after Zhu 2015; Yang 2016; Zhang et al., 2021).
Favorable granite geothermal reservoir is distributed in the exposed magmatic rock mass, near the late intrusive dike or the contact zone between rock mass and surrounding rock mass. The distribution of geothermal field is not only related to the fracture and fracture development of primary rock mass and contact zone rock due to the multi-stage intrusion of magma or the influence of deep fault structure, but also related to the geological age of intrusive rock.
Sample Description and Analitical Methods
In order to interpret magmatism in the study area of granite, a total of 20 samples of magmatic rocks were collected in the selected areas, such as Fuzhou, Zhangzhou and Huizhou area (Figure 3).and they were measured by principal trace element analysis, and zircon U-Pb dating analysis was conducted for six granite samples.
The granite samples collected were mainly distributed along a line of about 1,300 km with an exposed area of about 10–784 square kilometers. These granites are mainly granitic (Figure 4), with a few being orthogonality, quartz dimorphism and granitic diorite, with granular structure of different thickness and fineness (Figure 5). The mineralogy of these samples is relatively simple, consisting mainly of plagioclase (30–42%), potash feldspar (30–8%), quartz (20–30%), biotite (5%), and a small amount of amphibole (2–10%). Accessory minerals include sphere, zircon, and titanium-iron oxides.
FIGURE 4

Photograph showing outcrops of granites in different areas, (A) granite outcrop with fractures in Minhou, Fuzhou area; (B) granite outcrops in Qinqian, Fuzhou area; (C) granites with fractures in Huizhou; (D) granites in Zhangzhou.
FIGURE 5

Microphotographs showing mineral assemblage of representative granites. The abbreviations are: Pl-plagioclase, Qz-quartz, Bt-biotite, Kfs-K-feldspar, Amp-amphibole.
U-Pb dating and trace element analyses of zircon were conducted synchronously by LA-ICP-MS at the State Key Laboratory of Geological Processes and Mineral Resources, China University of Geosciences, Wuhan. Detailed operating conditions for the laser ablation system and the ICP-MS instrument and data reduction are the same as description by Liu et al. (2010). Laser sampling was performed using a GeoLas 2005. An Agilent 7500a ICP-MS instrument was used to acquire ion-signal intensities. A “wire” signal smoothing device is included in this laser ablation system, by which smooth signals are produced even at very low laser repetition rates down to 1 Hz (Hu et al., 2012b). Helium was applied as a carrier gas. Argon was used as the make-up gas and mixed with the carrier gas via a T-connector before entering the ICP. Nitrogen was added into the central gas flow (Ar + He) of the Ar plasma to decrease the detection limit and improve precision (Hu et al., 2008a; Liu et al., 2010). Each analysis incorporated a background acquisition of approximately 20–30 s (gas blank) followed by 50 s of data acquisition from the sample. The Agilent Chemstation was utilized for the acquisition of each individual analysis. Off-line selection and integration of background and analyze signals, and time-drift correction and quantitative calibration for trace element analyses and U-Pb dating were performed by ICPMS DataCal (
Zircon 91,500 was used as external standard for U-Pb dating, and was analyzed twice every five analyses. Time-dependent drifts of U-Th-Pb isotopic ratios were corrected using a linear interpolation (with time) for every five analyses according to the variations of 91,500 (i.e., two zircon 91,500 + 5 samples +2 zircon 91,500) (Liu et al., 2010). Preferred U-Th-Pb isotopic ratios used for 91,500 are from Wiedenbeck et al. (1995). Uncertainty of preferred values for the external standard 91,500 was propagated to the ultimate results of the samples. Concordia diagrams and weighted mean calculations were made using Isoplot/Exver3 (
Results
U-Pb Dating
The concordance ages and analysis results of typical zircons of six samples are shown in Figure 5. They are collected from different areas, such as Fuzhou area (GA02, QQ02) (Figure 3A), Zhangzhou area (ZZ02, ZZ07, ZZ11) (Figure 3B) and Huizhou area (HZ05) (Figure 3C). It can be seen from the CL image that the zircons generally have good autogenesis (Figure 6). Most of them are columnar or long-column-cone shaped with a length of 50–360 m. The aspect ratio of most of them is about 1.5:1–3:1, which is similar to the characteristics of magmatic zircons (Wu Yuanbao and Zheng Yongfei, 2004). The dating results of six samples show that the rock mass in the study area has a wide age distribution, ranging from 94.7 to 138.4 Ma. The LA-ICP-MS U-Pb zircon analysis spots are presented in Table 1, and the results are illustrated in Figure 6.
FIGURE 6

The 206Pb/238U-207Pb/235U concordia plot and the weighted mean age of representative zircons of the granites.
TABLE 1
| Spot | Element content | Isotope ratio | Age (Ma) | ||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| 232Th | 238U | Th/U | 207Pb/206Pb | 1sigma | 207Pb/235U | 1sigma | 206Pb/238U | 1sigma | 207Pb/206Pb | 1sigma | 207Pb/235U | 1sigma | 206Pb/238U | 1sigma | |
| GA02-01 | 200 | 175 | 1.14 | 0.0537 | 0.0042 | 0.1365 | 0.0095 | 0.0186 | 0.0004 | 366.72 | 177.76 | 129.95 | 8.46 | 118.81 | 2.23 |
| GA02-02 | 131 | 150 | 0.87 | 0.0528 | 0.0049 | 0.1334 | 0.0106 | 0.0188 | 0.0004 | 320.43 | 212.94 | 127.11 | 9.49 | 120.27 | 2.29 |
| GA02-03 | 114 | 142 | 0.80 | 0.0530 | 0.0047 | 0.1313 | 0.0105 | 0.0182 | 0.0004 | 327.84 | 197.20 | 125.29 | 9.44 | 116.08 | 2.33 |
| GA02-04 | 114 | 134 | 0.85 | 0.0494 | 0.0053 | 0.1269 | 0.0125 | 0.0187 | 0.0003 | 164.90 | 301.81 | 121.30 | 11.23 | 119.25 | 2.17 |
| GA02-07 | 147 | 170 | 0.86 | 0.0521 | 0.0052 | 0.1271 | 0.0110 | 0.0182 | 0.0004 | 300.06 | 223.12 | 121.51 | 9.94 | 116.25 | 2.30 |
| GA02-08 | 112 | 124 | 0.90 | 0.0465 | 0.0045 | 0.1144 | 0.0092 | 0.0181 | 0.0004 | 20.47 | 218.49 | 109.96 | 8.39 | 115.86 | 2.61 |
| GA02-10 | 370 | 318 | 1.16 | 0.0467 | 0.0032 | 0.1182 | 0.0071 | 0.0183 | 0.0003 | 31.58 | 155.54 | 113.40 | 6.45 | 116.81 | 1.81 |
| GA02-11 | 128 | 149 | 0.86 | 0.0476 | 0.0048 | 0.1126 | 0.0083 | 0.0179 | 0.0004 | 76.02 | 225.89 | 108.33 | 7.53 | 114.63 | 2.29 |
| GA02-12 | 125 | 138 | 0.91 | 0.0491 | 0.0039 | 0.1237 | 0.0076 | 0.0185 | 0.0004 | 153.79 | 174.05 | 118.47 | 6.83 | 118.41 | 2.76 |
| GA02-13 | 164 | 183 | 0.90 | 0.0513 | 0.0044 | 0.1271 | 0.0084 | 0.0184 | 0.0004 | 253.77 | 199.98 | 121.49 | 7.59 | 117.54 | 2.44 |
| GA02-14 | 119 | 135 | 0.88 | 0.0515 | 0.0050 | 0.1316 | 0.0115 | 0.0188 | 0.0004 | 261.18 | 225.90 | 125.50 | 10.33 | 119.89 | 2.51 |
| GA02-15 | 121 | 143 | 0.84 | 0.0492 | 0.0043 | 0.1254 | 0.0095 | 0.0186 | 0.0004 | 166.75 | 187.01 | 119.93 | 8.61 | 118.66 | 2.46 |
| GA02-16 | 142 | 157 | 0.90 | 0.0486 | 0.0041 | 0.1228 | 0.0086 | 0.0185 | 0.0004 | 127.87 | 188.86 | 117.58 | 7.80 | 118.29 | 2.31 |
| GA02-17 | 164 | 172 | 0.96 | 0.0520 | 0.0042 | 0.1280 | 0.0082 | 0.0185 | 0.0004 | 283.40 | 185.16 | 122.33 | 7.39 | 118.47 | 2.39 |
| GA02-18 | 106 | 125 | 0.85 | 0.0465 | 0.0048 | 0.1162 | 0.0099 | 0.0186 | 0.0004 | 33.43 | 224.04 | 111.59 | 9.02 | 118.91 | 2.36 |
| GA02-19 | 108 | 128 | 0.85 | 0.0475 | 0.0045 | 0.1144 | 0.0092 | 0.0179 | 0.0004 | 76.02 | 211.08 | 109.99 | 8.35 | 114.62 | 2.44 |
| GA02-20 | 225 | 226 | 0.99 | 0.0480 | 0.0041 | 0.1188 | 0.0088 | 0.0184 | 0.0003 | 98.24 | 201.82 | 114.02 | 8.00 | 117.53 | 2.18 |
| GA02-22 | 144 | 159 | 0.90 | 0.0545 | 0.0048 | 0.1380 | 0.0099 | 0.0188 | 0.0004 | 394.50 | 202.75 | 131.25 | 8.79 | 119.92 | 2.65 |
| GA02-23 | 219 | 225 | 0.98 | 0.0526 | 0.0040 | 0.1296 | 0.0086 | 0.0184 | 0.0004 | 309.32 | 174.05 | 123.74 | 7.73 | 117.63 | 2.50 |
| GA02-24 | 134 | 148 | 0.90 | 0.0482 | 0.0045 | 0.1223 | 0.0096 | 0.0187 | 0.0004 | 109.35 | 207.38 | 117.15 | 8.70 | 119.21 | 2.42 |
| GA02-25 | 146 | 161 | 0.91 | 0.0467 | 0.0043 | 0.1160 | 0.0094 | 0.0183 | 0.0004 | 35.28 | 207.38 | 111.39 | 8.56 | 116.70 | 2.30 |
| GA02-26 | 118 | 132 | 0.89 | 0.0481 | 0.0056 | 0.1165 | 0.0110 | 0.0185 | 0.0005 | 105.65 | 261.08 | 111.88 | 10.03 | 118.35 | 2.92 |
| GA02-27 | 191 | 204 | 0.94 | 0.0527 | 0.0044 | 0.1299 | 0.0090 | 0.0185 | 0.0004 | 322.28 | 186.09 | 124.02 | 8.13 | 117.97 | 2.29 |
| GA02-28 | 102 | 126 | 0.81 | 0.0532 | 0.0056 | 0.1314 | 0.0121 | 0.0187 | 0.0004 | 344.50 | 243.49 | 125.34 | 10.89 | 119.43 | 2.54 |
| GA02-29 | 139 | 157 | 0.88 | 0.0523 | 0.0042 | 0.1322 | 0.0092 | 0.0187 | 0.0004 | 298.21 | 183.31 | 126.04 | 8.22 | 119.65 | 2.53 |
| GA02-30 | 181 | 182 | 0.99 | 0.0514 | 0.0043 | 0.1288 | 0.0093 | 0.0187 | 0.0003 | 257.47 | 190.72 | 123.04 | 8.40 | 119.45 | 2.21 |
| QQ02-02 | 246 | 439 | 0.56 | 0.0467 | 0.0028 | 0.1122 | 0.0063 | 0.0177 | 0.0003 | 35.28 | 137.03 | 107.98 | 5.77 | 113.18 | 1.76 |
| QQ02-03 | 261 | 552 | 0.47 | 0.0505 | 0.0028 | 0.1249 | 0.0071 | 0.0179 | 0.0002 | 216.74 | 129.61 | 119.54 | 6.39 | 114.57 | 1.51 |
| QQ02-04 | 261 | 501 | 0.52 | 0.0469 | 0.0025 | 0.1146 | 0.0058 | 0.0180 | 0.0003 | 42.69 | 122.21 | 110.18 | 5.31 | 114.70 | 1.68 |
| QQ02-05 | 291 | 495 | 0.59 | 0.0465 | 0.0025 | 0.1099 | 0.0057 | 0.0173 | 0.0002 | 33.43 | 112.95 | 105.87 | 5.23 | 110.46 | 1.46 |
| QQ02-06 | 210 | 388 | 0.54 | 0.0485 | 0.0031 | 0.1186 | 0.0075 | 0.0177 | 0.0003 | 124.16 | 140.72 | 113.76 | 6.81 | 113.13 | 1.84 |
| QQ02-07 | 317 | 530 | 0.60 | 0.0465 | 0.0024 | 0.1137 | 0.0054 | 0.0179 | 0.0003 | 33.43 | 112.95 | 109.37 | 4.96 | 114.10 | 1.65 |
| QQ02-08 | 251 | 433 | 0.58 | 0.0472 | 0.0031 | 0.1124 | 0.0067 | 0.0176 | 0.0003 | 61.21 | 148.13 | 108.20 | 6.10 | 112.40 | 1.90 |
| QQ02-09 | 265 | 532 | 0.50 | 0.0461 | 0.0025 | 0.1094 | 0.0056 | 0.0172 | 0.0003 | 400.05 | 272.19 | 105.40 | 5.15 | 109.75 | 1.68 |
| QQ02-10 | 176 | 469 | 0.38 | 0.0503 | 0.0026 | 0.1256 | 0.0064 | 0.0182 | 0.0003 | 209.33 | 120.35 | 120.11 | 5.75 | 116.29 | 2.11 |
| QQ02-11 | 254 | 386 | 0.66 | 0.0481 | 0.0031 | 0.1166 | 0.0064 | 0.0179 | 0.0003 | 105.65 | 148.13 | 111.97 | 5.82 | 114.61 | 1.97 |
| QQ02-12 | 236 | 542 | 0.44 | 0.0470 | 0.0023 | 0.1154 | 0.0053 | 0.0179 | 0.0002 | 55.65 | 105.55 | 110.92 | 4.80 | 114.54 | 1.58 |
| QQ02-13 | 373 | 516 | 0.72 | 0.0495 | 0.0025 | 0.1206 | 0.0058 | 0.0178 | 0.0003 | 172.31 | 118.50 | 115.62 | 5.23 | 113.68 | 1.71 |
| QQ02-14 | 250 | 530 | 0.47 | 0.0467 | 0.0028 | 0.1106 | 0.0064 | 0.0173 | 0.0003 | 35.28 | 140.73 | 106.50 | 5.88 | 110.62 | 1.59 |
| QQ02-15 | 233 | 506 | 0.46 | 0.0480 | 0.0026 | 0.1189 | 0.0060 | 0.0181 | 0.0003 | 98.24 | 122.20 | 114.06 | 5.41 | 115.87 | 1.65 |
| QQ02-16 | 151 | 310 | 0.49 | 0.0480 | 0.0035 | 0.1139 | 0.0067 | 0.0173 | 0.0003 | 101.94 | 159.24 | 109.52 | 6.12 | 110.31 | 1.65 |
| QQ02-17 | 153 | 363 | 0.42 | 0.0491 | 0.0030 | 0.1244 | 0.0074 | 0.0181 | 0.0003 | 153.79 | 56.48 | 119.04 | 6.72 | 115.67 | 1.63 |
| QQ02-18 | 167 | 455 | 0.37 | 0.0515 | 0.0030 | 0.1258 | 0.0069 | 0.0177 | 0.0002 | 264.88 | 135.17 | 120.35 | 6.23 | 113.39 | 1.53 |
| QQ02-19 | 168 | 297 | 0.57 | 0.0532 | 0.0041 | 0.1220 | 0.0078 | 0.0171 | 0.0004 | 338.95 | 175.90 | 116.92 | 7.06 | 109.09 | 2.33 |
| QQ02-20 | 208 | 294 | 0.71 | 0.0467 | 0.0032 | 0.1158 | 0.0073 | 0.0178 | 0.0003 | 35.28 | 155.54 | 111.29 | 6.61 | 114.03 | 1.87 |
| QQ02-21 | 146 | 367 | 0.40 | 0.0505 | 0.0034 | 0.1206 | 0.0075 | 0.0175 | 0.0003 | 216.74 | 155.54 | 115.62 | 6.82 | 111.66 | 1.73 |
| QQ02-22 | 225 | 289 | 0.78 | 0.0466 | 0.0032 | 0.1098 | 0.0073 | 0.0171 | 0.0003 | 27.88 | 155.54 | 105.82 | 6.72 | 109.31 | 1.81 |
| QQ02-23 | 268 | 419 | 0.64 | 0.0525 | 0.0040 | 0.1311 | 0.0074 | 0.0179 | 0.0003 | 305.62 | 176.83 | 125.11 | 6.63 | 114.43 | 1.85 |
| QQ02-25 | 192 | 395 | 0.49 | 0.0539 | 0.0032 | 0.1332 | 0.0075 | 0.0180 | 0.0003 | 364.87 | 130.54 | 127.01 | 6.73 | 114.97 | 1.65 |
| QQ02-26 | 189 | 368 | 0.51 | 0.0473 | 0.0032 | 0.1120 | 0.0072 | 0.0173 | 0.0003 | 64.91 | 151.83 | 107.76 | 6.54 | 110.54 | 1.78 |
| QQ02-27 | 281 | 574 | 0.49 | 0.0500 | 0.0030 | 0.1238 | 0.0073 | 0.0180 | 0.0002 | 194.53 | 136.09 | 118.54 | 6.61 | 114.89 | 1.43 |
| QQ02-28 | 517 | 606 | 0.85 | 0.0472 | 0.0027 | 0.1149 | 0.0066 | 0.0177 | 0.0002 | 61.21 | 129.62 | 110.42 | 5.98 | 113.30 | 1.58 |
| QQ02-29 | 127 | 287 | 0.44 | 0.0481 | 0.0035 | 0.1133 | 0.0077 | 0.0173 | 0.0003 | 105.65 | 166.64 | 109.01 | 6.98 | 110.62 | 2.11 |
| QQ02-30 | 152 | 351 | 0.43 | 0.0476 | 0.0036 | 0.1115 | 0.0081 | 0.0171 | 0.0003 | 79.72 | 170.35 | 107.34 | 7.41 | 109.16 | 1.78 |
| ZZ02-01 | 108 | 154 | 0.70 | 0.0546 | 0.0050 | 0.1361 | 0.0105 | 0.0186 | 0.0003 | 394.50 | 205.53 | 129.56 | 9.35 | 118.98 | 2.08 |
| ZZ02-02 | 418 | 846 | 0.49 | 0.0522 | 0.0025 | 0.1402 | 0.0065 | 0.0195 | 0.0002 | 300.06 | 104.62 | 133.21 | 5.80 | 124.45 | 1.34 |
| ZZ02-03 | 429 | 888 | 0.48 | 0.0528 | 0.0021 | 0.1357 | 0.0052 | 0.0186 | 0.0002 | 320.43 | 88.88 | 129.23 | 4.62 | 118.52 | 1.22 |
| ZZ02-04 | 123 | 216 | 0.57 | 0.0527 | 0.0031 | 0.1433 | 0.0083 | 0.0198 | 0.0003 | 316.73 | 139.80 | 135.99 | 7.34 | 126.17 | 2.19 |
| ZZ02-05 | 209 | 336 | 0.62 | 0.0484 | 0.0030 | 0.1257 | 0.0069 | 0.0189 | 0.0003 | 120.46 | 140.72 | 120.19 | 6.20 | 120.55 | 1.72 |
| ZZ02-07 | 206 | 373 | 0.55 | 0.0511 | 0.0027 | 0.1405 | 0.0075 | 0.0198 | 0.0002 | 242.66 | 122.21 | 133.51 | 6.65 | 126.43 | 1.57 |
| ZZ02-08 | 204 | 207 | 0.99 | 0.0499 | 0.0042 | 0.1330 | 0.0102 | 0.0198 | 0.0004 | 187.12 | 188.86 | 126.75 | 9.13 | 126.56 | 2.28 |
| ZZ02-09 | 135 | 185 | 0.73 | 0.0507 | 0.0036 | 0.1308 | 0.0079 | 0.0191 | 0.0004 | 233.40 | 164.79 | 124.80 | 7.07 | 121.82 | 2.24 |
| ZZ02-13 | 136 | 247 | 0.55 | 0.0497 | 0.0033 | 0.1266 | 0.0073 | 0.0188 | 0.0003 | 188.97 | 153.68 | 121.08 | 6.61 | 120.23 | 1.79 |
| ZZ02-14 | 535 | 1090 | 0.49 | 0.0474 | 0.0051 | 0.1208 | 0.0131 | 0.0186 | 0.0002 | 77.87 | 231.45 | 115.76 | 11.85 | 118.49 | 1.15 |
| ZZ02-15 | 426 | 933 | 0.46 | 0.0513 | 0.0024 | 0.1406 | 0.0057 | 0.0199 | 0.0002 | 253.77 | 112.02 | 133.57 | 5.03 | 126.74 | 1.36 |
| ZZ02-16 | 512 | 786 | 0.65 | 0.0480 | 0.0020 | 0.1244 | 0.0051 | 0.0189 | 0.0002 | 98.24 | 96.29 | 119.01 | 4.58 | 120.42 | 1.25 |
| ZZ02-17 | 263 | 673 | 0.39 | 0.0520 | 0.0033 | 0.1354 | 0.0061 | 0.0189 | 0.0002 | 287.10 | 116.65 | 128.94 | 5.44 | 120.84 | 1.57 |
| ZZ02-18 | 110 | 163 | 0.68 | 0.0535 | 0.0044 | 0.1321 | 0.0088 | 0.0188 | 0.0004 | 350.06 | 187.01 | 126.02 | 7.93 | 119.89 | 2.37 |
| ZZ02-19 | 148 | 283 | 0.52 | 0.0505 | 0.0033 | 0.1384 | 0.0085 | 0.0197 | 0.0003 | 220.44 | 151.83 | 131.64 | 7.59 | 125.86 | 1.66 |
| ZZ02-20 | 189 | 311 | 0.61 | 0.0492 | 0.0031 | 0.1288 | 0.0079 | 0.0190 | 0.0003 | 166.75 | 146.28 | 123.00 | 7.12 | 121.13 | 1.71 |
| ZZ02-21 | 179 | 218 | 0.82 | 0.0479 | 0.0037 | 0.1213 | 0.0079 | 0.0184 | 0.0003 | 94.54 | 238.86 | 116.27 | 7.13 | 117.85 | 1.91 |
| ZZ02-22 | 176 | 278 | 0.63 | 0.0504 | 0.0032 | 0.1307 | 0.0070 | 0.0192 | 0.0003 | 213.04 | 144.43 | 124.77 | 6.30 | 122.89 | 1.86 |
| ZZ02-23 | 237 | 416 | 0.57 | 0.0534 | 0.0034 | 0.1380 | 0.0071 | 0.0189 | 0.0003 | 342.65 | 142.57 | 131.23 | 6.37 | 120.42 | 2.06 |
| ZZ02-24 | 504 | 1001 | 0.50 | 0.0535 | 0.0017 | 0.1384 | 0.0043 | 0.0188 | 0.0002 | 350.06 | 78.70 | 131.62 | 3.88 | 119.78 | 1.13 |
| ZZ02-26 | 201 | 223 | 0.90 | 0.0527 | 0.0045 | 0.1375 | 0.0096 | 0.0189 | 0.0003 | 316.73 | 196.27 | 130.79 | 8.61 | 120.86 | 2.19 |
| ZZ02-27 | 183 | 604 | 0.30 | 0.0497 | 0.0024 | 0.1271 | 0.0051 | 0.0187 | 0.0002 | 188.97 | 119.43 | 121.52 | 4.58 | 119.21 | 1.54 |
| ZZ02-28 | 125 | 184 | 0.68 | 0.0480 | 0.0036 | 0.1197 | 0.0071 | 0.0186 | 0.0004 | 101.94 | 231.45 | 114.78 | 6.40 | 118.78 | 2.25 |
| ZZ02-29 | 255 | 261 | 0.98 | 0.0509 | 0.0036 | 0.1258 | 0.0070 | 0.0184 | 0.0003 | 235.25 | 164.79 | 120.28 | 6.31 | 117.50 | 2.01 |
| ZZ02-30 | 248 | 720 | 0.34 | 0.0526 | 0.0020 | 0.1372 | 0.0047 | 0.0189 | 0.0002 | 309.32 | 88.88 | 130.57 | 4.24 | 120.59 | 1.30 |
| ZZ07-01 | 74.8 | 156 | 0.48 | 0.0519 | 0.0046 | 0.1521 | 0.0121 | 0.0222 | 0.0005 | 283.40 | 203.68 | 143.79 | 10.62 | 141.40 | 2.91 |
| ZZ07-02 | 165 | 272 | 0.61 | 0.0463 | 0.0032 | 0.1384 | 0.0090 | 0.0215 | 0.0003 | 13.06 | 159.25 | 131.61 | 8.05 | 137.29 | 2.06 |
| ZZ07-03 | 99.4 | 234 | 0.43 | 0.0461 | 0.0035 | 0.1399 | 0.0102 | 0.0219 | 0.0004 | 400.05 | 224.04 | 132.97 | 9.08 | 139.37 | 2.24 |
| ZZ07-04 | 137 | 232 | 0.59 | 0.0463 | 0.0032 | 0.1390 | 0.0092 | 0.0217 | 0.0004 | 13.06 | 159.25 | 132.12 | 8.21 | 138.51 | 2.30 |
| ZZ07-05 | 219 | 355 | 0.62 | 0.0524 | 0.0039 | 0.1530 | 0.0104 | 0.0214 | 0.0003 | 301.91 | 168.50 | 144.54 | 9.18 | 136.21 | 1.76 |
| ZZ07-05 | 219 | 355 | 0.62 | 0.0524 | 0.0039 | 0.1530 | 0.0104 | 0.0214 | 0.0003 | 301.91 | 168.50 | 144.54 | 9.18 | 136.21 | 1.76 |
| ZZ07-06 | 118 | 201 | 0.59 | 0.0526 | 0.0045 | 0.1486 | 0.0102 | 0.0214 | 0.0004 | 322.28 | 196.27 | 140.72 | 9.06 | 136.44 | 2.42 |
| ZZ07-07 | 178 | 361 | 0.49 | 0.0478 | 0.0025 | 0.1445 | 0.0077 | 0.0218 | 0.0003 | 87.13 | 118.50 | 137.07 | 6.80 | 138.94 | 1.88 |
| ZZ07-08 | 50.5 | 93.8 | 0.54 | 0.0480 | 0.0058 | 0.1314 | 0.0119 | 0.0211 | 0.0005 | 98.24 | 262.93 | 125.33 | 10.65 | 134.59 | 2.91 |
| ZZ07-10 | 118 | 324 | 0.36 | 0.0464 | 0.0031 | 0.1351 | 0.0081 | 0.0214 | 0.0003 | 20.47 | 155.54 | 128.69 | 7.23 | 136.61 | 1.97 |
| ZZ07-11 | 145 | 201 | 0.72 | 0.0491 | 0.0037 | 0.1481 | 0.0097 | 0.0225 | 0.0005 | 150.09 | 170.35 | 140.23 | 8.60 | 143.69 | 3.15 |
| ZZ07-12 | 318 | 609 | 0.52 | 0.0464 | 0.0022 | 0.1424 | 0.0062 | 0.0225 | 0.0003 | 16.77 | 111.10 | 135.20 | 5.55 | 143.25 | 1.81 |
| ZZ07-13 | 166 | 419 | 0.40 | 0.0526 | 0.0027 | 0.1576 | 0.0078 | 0.0217 | 0.0003 | 309.32 | 114.80 | 148.62 | 6.86 | 138.26 | 1.82 |
| ZZ07-14 | 113 | 244 | 0.46 | 0.0480 | 0.0038 | 0.1414 | 0.0098 | 0.0217 | 0.0004 | 98.24 | 177.75 | 134.27 | 8.70 | 138.61 | 2.37 |
| ZZ07-15 | 182 | 323 | 0.56 | 0.0525 | 0.0033 | 0.1542 | 0.0091 | 0.0216 | 0.0003 | 309.32 | 144.43 | 145.62 | 8.05 | 137.93 | 2.17 |
| ZZ07-16 | 242 | 367 | 0.66 | 0.0511 | 0.0031 | 0.1514 | 0.0085 | 0.0217 | 0.0003 | 242.66 | 138.87 | 143.15 | 7.53 | 138.34 | 2.06 |
| ZZ07-17 | 88.5 | 209 | 0.42 | 0.0534 | 0.0051 | 0.1563 | 0.0125 | 0.0220 | 0.0004 | 346.35 | 212.01 | 147.42 | 11.01 | 140.11 | 2.70 |
| ZZ07-18 | 90.7 | 178 | 0.51 | 0.0505 | 0.0039 | 0.1481 | 0.0100 | 0.0217 | 0.0004 | 216.74 | 176.83 | 140.24 | 8.83 | 138.40 | 2.84 |
| ZZ07-19 | 446 | 865 | 0.52 | 0.0481 | 0.0024 | 0.1469 | 0.0071 | 0.0220 | 0.0003 | 105.65 | 111.10 | 139.14 | 6.30 | 140.17 | 1.69 |
| ZZ07-20 | 228 | 325 | 0.70 | 0.0542 | 0.0038 | 0.1543 | 0.0103 | 0.0210 | 0.0004 | 388.94 | 159.24 | 145.74 | 9.05 | 134.03 | 2.38 |
| ZZ07-21 | 82.3 | 179 | 0.46 | 0.0500 | 0.0037 | 0.1538 | 0.0104 | 0.0224 | 0.0004 | 194.53 | 176.83 | 145.25 | 9.17 | 143.03 | 2.43 |
| ZZ07-22 | 76.1 | 159 | 0.48 | 0.0510 | 0.0042 | 0.1441 | 0.0101 | 0.0212 | 0.0004 | 242.66 | 197.20 | 136.72 | 8.95 | 135.37 | 2.72 |
| ZZ07-23 | 133 | 269 | 0.49 | 0.0510 | 0.0038 | 0.1453 | 0.0101 | 0.0208 | 0.0003 | 238.96 | 204.61 | 137.76 | 8.93 | 132.85 | 2.02 |
| ZZ07-24 | 99.6 | 224 | 0.45 | 0.0546 | 0.0038 | 0.1565 | 0.0086 | 0.0213 | 0.0004 | 398.20 | 155.54 | 147.66 | 7.59 | 136.01 | 2.61 |
| ZZ07-26 | 245 | 428 | 0.57 | 0.0528 | 0.0031 | 0.1599 | 0.0093 | 0.0221 | 0.0003 | 320.43 | 130.54 | 150.58 | 8.17 | 140.97 | 2.15 |
| ZZ07-27 | 78.9 | 175 | 0.45 | 0.0492 | 0.0045 | 0.1419 | 0.0111 | 0.0211 | 0.0004 | 166.75 | 199.97 | 134.72 | 9.91 | 134.88 | 2.39 |
| ZZ07-28 | 209 | 623 | 0.34 | 0.0470 | 0.0021 | 0.1448 | 0.0065 | 0.0223 | 0.0003 | 50.10 | 99.99 | 137.31 | 5.76 | 141.91 | 2.00 |
| ZZ07-29 | 65.8 | 149 | 0.44 | 0.0478 | 0.0044 | 0.1384 | 0.0106 | 0.0217 | 0.0005 | 100.09 | 199.97 | 131.64 | 9.42 | 138.37 | 2.95 |
| ZZ07-30 | 90.9 | 168 | 0.54 | 0.0535 | 0.0043 | 0.1626 | 0.0118 | 0.0223 | 0.0004 | 350.06 | 178.68 | 152.95 | 10.30 | 142.34 | 2.78 |
| ZZ11-01 | 144 | 94.5 | 1.53 | 0.0469 | 0.0065 | 0.0919 | 0.0101 | 0.0150 | 0.0004 | 55.65 | 294.41 | 89.24 | 9.38 | 95.68 | 2.50 |
| ZZ11-02 | 837 | 1124 | 0.75 | 0.0482 | 0.0020 | 0.1014 | 0.0043 | 0.0151 | 0.0002 | 109.35 | 98.14 | 98.03 | 3.93 | 96.73 | 1.22 |
| ZZ11-03 | 105 | 104 | 1.01 | 0.0540 | 0.0074 | 0.1019 | 0.0094 | 0.0147 | 0.0005 | 372.28 | 311.07 | 98.48 | 8.69 | 93.92 | 2.95 |
| ZZ11-04 | 268 | 352 | 0.76 | 0.0499 | 0.0032 | 0.1007 | 0.0058 | 0.0145 | 0.0002 | 190.82 | 148.13 | 97.39 | 5.40 | 92.83 | 1.45 |
| ZZ11-05 | 343 | 407 | 0.84 | 0.0507 | 0.0030 | 0.1017 | 0.0058 | 0.0144 | 0.0002 | 227.85 | 141.65 | 98.31 | 5.33 | 92.46 | 1.18 |
| ZZ11-06 | 480 | 532 | 0.90 | 0.0493 | 0.0029 | 0.0998 | 0.0054 | 0.0146 | 0.0002 | 166.75 | 143.50 | 96.59 | 4.98 | 93.53 | 1.27 |
| ZZ11-07 | 58.7 | 61.0 | 0.96 | 0.0546 | 0.0083 | 0.0993 | 0.0110 | 0.0146 | 0.0005 | 394.50 | 344.40 | 96.11 | 10.16 | 93.41 | 3.25 |
| ZZ11-08 | 178 | 228 | 0.78 | 0.0518 | 0.0045 | 0.1025 | 0.0072 | 0.0146 | 0.0003 | 275.99 | 201.83 | 99.10 | 6.59 | 93.55 | 1.71 |
| ZZ11-10 | 187 | 290 | 0.65 | 0.0471 | 0.0041 | 0.0954 | 0.0074 | 0.0150 | 0.0003 | 53.80 | 196.27 | 92.49 | 6.86 | 95.78 | 1.63 |
| ZZ11-11 | 169 | 266 | 0.63 | 0.0499 | 0.0043 | 0.1003 | 0.0075 | 0.0149 | 0.0003 | 190.82 | 198.12 | 97.03 | 6.95 | 95.51 | 1.95 |
| ZZ11-12 | 281 | 308 | 0.91 | 0.0529 | 0.0031 | 0.1099 | 0.0063 | 0.0150 | 0.0003 | 324.13 | 135.17 | 105.86 | 5.74 | 95.81 | 1.75 |
| ZZ11-13 | 187 | 222 | 0.84 | 0.0501 | 0.0044 | 0.1034 | 0.0084 | 0.0152 | 0.0003 | 198.23 | 192.56 | 99.95 | 7.69 | 97.31 | 1.97 |
| ZZ11-14 | 406 | 378 | 1.07 | 0.0501 | 0.0038 | 0.1021 | 0.0069 | 0.0149 | 0.0002 | 198.23 | 175.91 | 98.68 | 6.33 | 95.39 | 1.45 |
| ZZ11-18 | 436 | 422 | 1.03 | 0.0483 | 0.0028 | 0.1003 | 0.0055 | 0.0152 | 0.0002 | 122.31 | 133.31 | 97.09 | 5.11 | 97.01 | 1.51 |
| ZZ11-19 | 306 | 368 | 0.83 | 0.0517 | 0.0033 | 0.1018 | 0.0056 | 0.0145 | 0.0002 | 272.29 | 146.28 | 98.48 | 5.13 | 92.67 | 1.35 |
| ZZ11-20 | 211 | 199 | 1.06 | 0.0490 | 0.0043 | 0.0976 | 0.0061 | 0.0149 | 0.0003 | 146.38 | 192.57 | 94.60 | 5.68 | 95.46 | 1.87 |
| ZZ11-21 | 180 | 179 | 1.01 | 0.0542 | 0.0051 | 0.1038 | 0.0074 | 0.0145 | 0.0003 | 375.98 | 212.94 | 100.25 | 6.82 | 92.92 | 1.90 |
| ZZ11-22 | 204 | 277 | 0.74 | 0.0522 | 0.0040 | 0.1051 | 0.0070 | 0.0150 | 0.0003 | 294.51 | 169.42 | 101.50 | 6.45 | 95.88 | 1.75 |
| ZZ11-23 | 212 | 308 | 0.69 | 0.0482 | 0.0033 | 0.0988 | 0.0061 | 0.0150 | 0.0002 | 109.35 | 151.83 | 95.62 | 5.60 | 96.23 | 1.56 |
| ZZ11-24 | 152 | 140 | 1.09 | 0.0563 | 0.0065 | 0.1051 | 0.0091 | 0.0145 | 0.0003 | 464.86 | 259.22 | 101.50 | 8.39 | 92.76 | 2.20 |
| ZZ11-26 | 179 | 187 | 0.96 | 0.0463 | 0.0040 | 0.0918 | 0.0062 | 0.0147 | 0.0003 | 13.06 | 196.27 | 89.20 | 5.79 | 94.08 | 1.90 |
| ZZ11-27 | 149 | 239 | 0.62 | 0.0503 | 0.0035 | 0.1054 | 0.0065 | 0.0152 | 0.0003 | 209.33 | 161.09 | 101.71 | 5.95 | 97.12 | 1.77 |
| ZZ11-28 | 152 | 218 | 0.70 | 0.0504 | 0.0043 | 0.0966 | 0.0068 | 0.0145 | 0.0003 | 213.04 | 0.92 | 93.66 | 6.31 | 92.71 | 1.61 |
| ZZ11-29 | 253 | 374 | 0.68 | 0.0510 | 0.0038 | 0.1020 | 0.0067 | 0.0148 | 0.0003 | 238.96 | 204.61 | 98.66 | 6.17 | 94.69 | 1.82 |
| ZZ11-30 | 222 | 333 | 0.67 | 0.0492 | 0.0041 | 0.0978 | 0.0069 | 0.0149 | 0.0002 | 166.75 | 172.20 | 94.71 | 6.35 | 95.25 | 1.50 |
| HZ05-01 | 128 | 186 | 0.69 | 0.0475 | 0.0041 | 0.1323 | 0.0104 | 0.0204 | 0.0004 | 76.02 | 257.37 | 126.12 | 9.29 | 130.46 | 2.45 |
| HZ05-02 | 114 | 146 | 0.78 | 0.0522 | 0.0048 | 0.1477 | 0.0112 | 0.0205 | 0.0004 | 294.51 | 213.86 | 139.85 | 9.89 | 130.66 | 2.82 |
| HZ05-03 | 534 | 913 | 0.59 | 0.0526 | 0.0019 | 0.1558 | 0.0056 | 0.0214 | 0.0002 | 322.28 | 80.55 | 147.01 | 4.90 | 136.72 | 1.56 |
| HZ05-04 | 227 | 548 | 0.41 | 0.0540 | 0.0032 | 0.1574 | 0.0075 | 0.0211 | 0.0003 | 368.57 | 133.32 | 148.40 | 6.56 | 134.69 | 1.75 |
| HZ05-05 | 159 | 306 | 0.52 | 0.0505 | 0.0036 | 0.1474 | 0.0096 | 0.0213 | 0.0003 | 220.44 | 160.17 | 139.61 | 8.46 | 135.68 | 2.06 |
| HZ05-06 | 205 | 246 | 0.83 | 0.0536 | 0.0045 | 0.1513 | 0.0108 | 0.0209 | 0.0004 | 366.72 | 216.64 | 143.06 | 9.49 | 133.53 | 2.53 |
| HZ05-07 | 159 | 347 | 0.46 | 0.0493 | 0.0033 | 0.1435 | 0.0087 | 0.0214 | 0.0004 | 164.90 | 157.38 | 136.17 | 7.71 | 136.80 | 2.28 |
| HZ05-08 | 107 | 260 | 0.41 | 0.0514 | 0.0047 | 0.1519 | 0.0114 | 0.0220 | 0.0004 | 257.47 | 209.24 | 143.57 | 10.08 | 140.06 | 2.69 |
| HZ05-09 | 65.9 | 88.3 | 0.75 | 0.0501 | 0.0068 | 0.1340 | 0.0110 | 0.0219 | 0.0006 | 198.23 | 288.85 | 127.69 | 9.82 | 139.58 | 3.94 |
| HZ05-10 | 152 | 243 | 0.62 | 0.0493 | 0.0038 | 0.1392 | 0.0097 | 0.0208 | 0.0004 | 161.20 | 183.31 | 132.35 | 8.63 | 132.47 | 2.62 |
| HZ05-11 | 328 | 732 | 0.45 | 0.0505 | 0.0024 | 0.1448 | 0.0067 | 0.0208 | 0.0003 | 216.74 | 111.10 | 137.29 | 5.93 | 132.80 | 1.65 |
| HZ05-12 | 125 | 217 | 0.58 | 0.0461 | 0.0036 | 0.1267 | 0.0092 | 0.0204 | 0.0004 | 400.05 | 211.08 | 121.12 | 8.28 | 130.49 | 2.48 |
| HZ05-13 | 228 | 582 | 0.39 | 0.0484 | 0.0024 | 0.1384 | 0.0066 | 0.0207 | 0.0003 | 120.46 | 86.10 | 131.61 | 5.89 | 132.15 | 1.59 |
| HZ05-14 | 108 | 243 | 0.45 | 0.0526 | 0.0035 | 0.1510 | 0.0092 | 0.0209 | 0.0004 | 322.28 | 151.83 | 142.79 | 8.16 | 133.36 | 2.32 |
| HZ05-15 | 158 | 202 | 0.78 | 0.0483 | 0.0043 | 0.1348 | 0.0100 | 0.0209 | 0.0005 | 122.31 | 199.97 | 128.42 | 8.96 | 133.37 | 2.85 |
| HZ05-16 | 195 | 390 | 0.50 | 0.0486 | 0.0029 | 0.1408 | 0.0085 | 0.0208 | 0.0003 | 127.87 | 137.02 | 133.75 | 7.55 | 132.97 | 1.90 |
| HZ05-17 | 245 | 594 | 0.41 | 0.0512 | 0.0032 | 0.1535 | 0.0086 | 0.0221 | 0.0003 | 250.07 | 144.43 | 144.96 | 7.56 | 140.60 | 1.95 |
| HZ05-18 | 157 | 259 | 0.61 | 0.0538 | 0.0042 | 0.1498 | 0.0113 | 0.0204 | 0.0004 | 364.87 | 177.76 | 141.74 | 9.94 | 130.37 | 2.43 |
| HZ05-19 | 114 | 303 | 0.38 | 0.0530 | 0.0036 | 0.1461 | 0.0090 | 0.0204 | 0.0003 | 327.84 | 153.68 | 138.49 | 7.99 | 130.10 | 2.06 |
| HZ05-20 | 102 | 167 | 0.61 | 0.0553 | 0.0053 | 0.1483 | 0.0107 | 0.0205 | 0.0005 | 433.38 | 219.41 | 140.44 | 9.45 | 130.83 | 2.90 |
| HZ05-21 | 448 | 570 | 0.79 | 0.0495 | 0.0026 | 0.1512 | 0.0077 | 0.0222 | 0.0003 | 172.31 | 115.73 | 142.94 | 6.79 | 141.37 | 1.85 |
| HZ05-22 | 140 | 260 | 0.54 | 0.0486 | 0.0030 | 0.1483 | 0.0083 | 0.0220 | 0.0004 | 127.87 | 137.02 | 140.41 | 7.31 | 140.18 | 2.42 |
| HZ05-23 | 154 | 308 | 0.50 | 0.0512 | 0.0032 | 0.1506 | 0.0081 | 0.0219 | 0.0004 | 250.07 | 142.58 | 142.43 | 7.16 | 139.94 | 2.48 |
| HZ05-24 | 139 | 282 | 0.49 | 0.0517 | 0.0035 | 0.1483 | 0.0089 | 0.0214 | 0.0003 | 272.29 | 149.06 | 140.37 | 7.89 | 136.21 | 2.08 |
| HZ05-25 | 56.2 | 90.4 | 0.62 | 0.0534 | 0.0057 | 0.1544 | 0.0133 | 0.0212 | 0.0005 | 342.65 | 244.42 | 145.80 | 11.66 | 135.52 | 3.46 |
| HZ05-26 | 174 | 176 | 0.99 | 0.0552 | 0.0040 | 0.1582 | 0.0092 | 0.0214 | 0.0004 | 420.42 | 160.17 | 149.16 | 8.04 | 136.71 | 2.54 |
| HZ05-27 | 105 | 201 | 0.53 | 0.0513 | 0.0035 | 0.1544 | 0.0091 | 0.0218 | 0.0004 | 253.77 | 183.31 | 145.77 | 7.99 | 138.92 | 2.36 |
| HZ05-28 | 127 | 214 | 0.60 | 0.0512 | 0.0037 | 0.1446 | 0.0092 | 0.0209 | 0.0004 | 255.62 | 164.79 | 137.15 | 8.20 | 133.20 | 2.43 |
| HZ05-29 | 129 | 386 | 0.33 | 0.0520 | 0.0032 | 0.1525 | 0.0092 | 0.0214 | 0.0003 | 283.40 | 110.17 | 144.12 | 8.13 | 136.59 | 1.93 |
| HZ05-30 | 97.9 | 184 | 0.53 | 0.0490 | 0.0038 | 0.1425 | 0.0088 | 0.0214 | 0.0004 | 150.09 | 174.05 | 135.27 | 7.82 | 136.71 | 2.40 |
Zircon U-Pb data of granites in the study area.
A total of 26 valid data were obtained from GA02. These zircon grains have moderate and variable concentrations of Th (102–200 ppm) and U (125–318 ppm), corresponding Th/U ratios of 0.8–1.14, showing the characteristic of magmatic zircon (Hoskin and Black, 2000;
There is no obvious pattern of age distribution of such samples in the region. In general, the age of all samples in the study area shows that they are formed in Cretaceous age, indicating that Yanshanian tectonic thermal events are the dominant thermal events in the area. According to the U-Pb dating results, at least three acidic magmatic events occurred during Cretaceous: early stage of Early Cretaceous (about 138–135.1 Ma), late stage of Early Cretaceous (110–121 Ma) and the early stage of Late Cretaceous (about 93–96 Ma).
Geochemistry
20 fresh granite samples are obtained for major and trace element analyses. The results are listed in Table 2. The samples have very low loss on ignition (∼0.85 wt%), indicating little or no modification by weathering. Rock geochemical test results show that the rock mass geochemical composition analyses are as follows: SiO2 content ranged from 65.86 to 83.83% with an average of 73.64%; TiO2 content ranged from 0.08 to 0.55% with an average of 0.23%; Al2O3 content ranged from 7.38 to 15.8% with an average of 13.53%; MgO content ranged from 0.12 to 1.73% with an average of 0.48%; and (K2O + Na2O) content ranged from 4.76 to 8.87% with an average of 7.66%, belonging to high-K calc-alkaline series. The granites are characterized by weakly peraluminous (A/CNK = 1.03). At the diagram of SiO2 (Na2O + K2O) (Figure 7), sample dots fell within the granite region. The aluminum saturation index (A/CNK) ranges from 0.88 to 1.33 and ranges mainly from 1.0 to 1.1 on the diagram of A/NK–A/CNK (Figure 7).
TABLE 2
| Sample | GA02 | GA05 | GM01 | GM02 | QQ02 | ZZ01 | ZZ02 | ZZ03 | ZZ04 | ZZ07 | ZZ09 | ZZ11 | ZZ12 | ZZ13 | ZZ14 | ZZ15 | ZZ17 | HZ05 | HZ06 | HZ18 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| SiO2 | 66.74 | 65.86 | 73.18 | 74.69 | 75.27 | 68.43 | 69.24 | 69.89 | 69.62 | 73.05 | 83.83 | 73.59 | 77.34 | 75.35 | 76.67 | 75.66 | 76.34 | 75.50 | 75.03 | 77.56 |
| TiO2 | 0.51 | 0.55 | 0.26 | 0.24 | 0.14 | 0.39 | 0.35 | 0.31 | 0.35 | 0.13 | 0.08 | 0.31 | 0.08 | 0.12 | 0.11 | 0.13 | 0.17 | 0.11 | 0.11 | 0.09 |
| Al2O3 | 15.16 | 15.25 | 14.68 | 13.65 | 13.41 | 15.80 | 15.21 | 14.49 | 14.65 | 13.70 | 7.38 | 13.71 | 12.83 | 13.28 | 12.45 | 13.58 | 12.71 | 12.93 | 13.37 | 12.60 |
| Fe2O3T | 4.26 | 4.80 | 1.60 | 1.63 | 1.54 | 3.06 | 2.62 | 2.61 | 2.72 | 1.66 | 0.47 | 2.05 | 0.58 | 0.81 | 0.79 | 0.95 | 1.05 | 1.57 | 1.36 | 0.67 |
| FeOT | 3.83 | 4.32 | 1.44 | 1.47 | 1.39 | 2.75 | 2.36 | 2.34 | 2.45 | 1.50 | 0.43 | 1.84 | 0.52 | 0.73 | 0.71 | 0.85 | 0.95 | 1.42 | 1.22 | 0.60 |
| MnO | 0.11 | 0.11 | 0.07 | 0.06 | 0.04 | 0.05 | 0.07 | 0.09 | 0.08 | 0.04 | 0.03 | 0.09 | 0.07 | 0.05 | 0.04 | 0.09 | 0.04 | 0.04 | 0.03 | 0.03 |
| MgO | 1.52 | 1.73 | 0.44 | 0.37 | 0.22 | 0.92 | 0.77 | 0.79 | 0.85 | 0.15 | 0.21 | 0.51 | 0.06 | 0.15 | 0.15 | 0.17 | 0.20 | 0.14 | 0.19 | 0.12 |
| CaO | 3.84 | 3.92 | 1.53 | 1.07 | 1.17 | 3.35 | 2.86 | 2.06 | 2.66 | 1.08 | 1.75 | 0.88 | 0.28 | 0.70 | 0.66 | 0.89 | 0.79 | 0.76 | 0.79 | 0.13 |
| Na2O | 3.48 | 3.46 | 3.96 | 3.69 | 4.17 | 3.49 | 3.21 | 3.20 | 3.19 | 3.20 | 2.52 | 3.57 | 4.52 | 3.29 | 3.20 | 3.99 | 3.53 | 3.74 | 3.75 | 2.09 |
| K2O | 3.05 | 3.21 | 4.17 | 4.29 | 3.73 | 3.62 | 3.76 | 4.57 | 4.07 | 5.28 | 2.25 | 4.47 | 4.35 | 4.78 | 4.53 | 4.19 | 4.60 | 4.71 | 5.13 | 5.28 |
| P2O5 | 0.16 | 0.18 | 0.05 | 0.05 | 0.04 | 0.14 | 0.10 | 0.10 | 0.11 | 0.03 | 0.02 | 0.08 | 0.01 | 0.03 | 0.02 | 0.03 | 0.03 | 0.03 | 0.02 | 0.01 |
| LOI | 1.01 | 0.65 | 0.38 | 0.41 | 0.43 | 0.54 | 1.35 | 1.42 | 1.41 | 1.38 | 1.66 | 1.01 | 0.28 | 1.48 | 1.00 | 0.44 | 0.14 | 0.45 | 0.43 | 1.10 |
| SUM | 99.83 | 99.72 | 100.31 | 100.15 | 100.17 | 99.80 | 99.53 | 99.51 | 99.70 | 99.70 | 100.18 | 100.26 | 100.39 | 100.02 | 99.62 | 100.11 | 99.61 | 99.97 | 100.20 | 99.68 |
| Li | 7.48 | 14.16 | 22.27 | 14.90 | 12.87 | 5.82 | 7.87 | 6.14 | 8.05 | 7.67 | 3.06 | 12.72 | 29.82 | 6.51 | 6.66 | 32.62 | 10.45 | 31.40 | 27.34 | 11.30 |
| Be | 1.90 | 1.70 | 2.48 | 2.95 | 2.07 | 2.27 | 2.36 | 2.41 | 2.46 | 3.92 | 0.87 | 3.81 | 5.38 | 2.94 | 2.13 | 1.96 | 4.70 | 6.43 | 4.17 | 4.27 |
| Sc | 8.44 | 10.11 | 4.55 | 4.18 | 5.24 | 4.27 | 5.20 | 4.99 | 7.47 | 2.50 | 0.80 | 4.57 | 1.58 | 2.69 | 2.48 | 3.32 | 1.71 | 5.21 | 5.34 | 2.50 |
| V | 68.35 | 75.21 | 15.12 | 13.15 | 6.29 | 42.70 | 26.92 | 21.09 | 33.17 | 5.87 | 4.73 | 24.17 | 2.00 | 4.21 | 6.10 | 6.10 | 8.91 | 5.19 | 4.20 | 1.53 |
| Cr | 1.50 | 1.61 | 1.06 | 0.92 | 0.42 | 1.51 | 0.87 | 0.96 | 1.00 | 0.49 | 0.89 | 0.98 | 0.33 | 0.38 | 0.34 | 0.32 | 0.88 | 0.91 | 0.83 | 0.26 |
| Co | 6.84 | 8.07 | 1.26 | 1.31 | 0.90 | 4.98 | 3.77 | 3.31 | 3.41 | 1.03 | 0.77 | 2.13 | 0.07 | 0.54 | 0.39 | 0.53 | 0.68 | 0.56 | 0.41 | 0.10 |
| Ni | 2.07 | 2.15 | 1.12 | 1.01 | 0.89 | 2.41 | 1.27 | 1.28 | 1.28 | 0.82 | 1.05 | 1.43 | 0.58 | 0.74 | 0.63 | 0.59 | 1.17 | 0.71 | 0.87 | 0.55 |
| Cu | 3.06 | 3.45 | 1.33 | 1.81 | 0.40 | 2.91 | 58.72 | 16.73 | 60.52 | 0.45 | 0.64 | 1.24 | 0.32 | 0.46 | 0.36 | 0.45 | 0.98 | 0.34 | 0.44 | 0.71 |
| Zn | 52.38 | 47.76 | 36.14 | 40.53 | 35.11 | 76.11 | 48.94 | 49.04 | 33.91 | 25.69 | 6.19 | 50.24 | 39.48 | 21.08 | 17.89 | 26.62 | 14.54 | 17.29 | 22.26 | 36.71 |
| Ga | 15.30 | 15.76 | 16.70 | 16.03 | 15.85 | 18.90 | 15.10 | 12.72 | 15.65 | 17.38 | 7.16 | 17.65 | 19.23 | 27.27 | 25.91 | 15.10 | 15.77 | 17.97 | 17.56 | 16.93 |
| Rb | 90.99 | 112.01 | 170.09 | 155.20 | 133.37 | 133.14 | 116.49 | 144.05 | 131.38 | 174.51 | 62.06 | 210.19 | 267.52 | 191.46 | 179.68 | 189.25 | 233.26 | 262.13 | 263.46 | 324.54 |
| Sr | 431.06 | 415.98 | 212.04 | 209.11 | 156.40 | 527.36 | 392.22 | 303.69 | 383.07 | 150.88 | 76.96 | 154.73 | 5.22 | 1378.40 | 934.19 | 132.30 | 75.50 | 55.80 | 62.44 | 30.99 |
| Y | 15.98 | 21.59 | 27.60 | 29.06 | 29.35 | 13.29 | 21.35 | 24.63 | 31.65 | 36.83 | 18.59 | 30.76 | 29.91 | 19.15 | 20.32 | 25.91 | 27.96 | 49.38 | 26.70 | 37.10 |
| Zr | 169.31 | 183.67 | 189.84 | 174.22 | 144.86 | 162.57 | 183.96 | 168.97 | 186.27 | 125.39 | 74.57 | 186.87 | 79.85 | 82.43 | 66.27 | 86.58 | 129.71 | 140.49 | 120.91 | 83.32 |
| Nb | 9.12 | 9.97 | 15.77 | 16.33 | 13.59 | 9.25 | 12.02 | 11.56 | 15.66 | 11.47 | 5.77 | 22.01 | 37.09 | 15.50 | 13.71 | 21.89 | 23.34 | 26.17 | 17.96 | 25.55 |
| Sn | 1.08 | 1.36 | 2.07 | 2.20 | 2.02 | 1.19 | 1.73 | 1.78 | 2.72 | 2.53 | 1.03 | 2.89 | 2.98 | 1.95 | 1.82 | 2.58 | 1.36 | 2.93 | 2.82 | 1.56 |
| Cs | 2.87 | 2.57 | 5.56 | 3.72 | 2.04 | 5.10 | 2.29 | 2.28 | 2.15 | 1.24 | 0.52 | 3.42 | 6.92 | 15.89 | 11.50 | 3.65 | 2.93 | 7.34 | 6.28 | 4.07 |
| Ba | 987.77 | 975.04 | 1207.11 | 1068.56 | 838.01 | 844.17 | 558.96 | 678.02 | 580.46 | 647.35 | 375.27 | 418.07 | 16.66 | 1479.56 | 1122.94 | 694.20 | 203.27 | 140.57 | 167.22 | 97.67 |
| La | 34.94 | 42.64 | 55.29 | 52.86 | 30.36 | 34.59 | 36.67 | 39.59 | 45.19 | 49.08 | 19.65 | 47.87 | 21.88 | 24.55 | 22.60 | 29.54 | 39.57 | 42.38 | 25.79 | 115.84 |
| Ce | 63.02 | 77.08 | 105.87 | 101.44 | 58.86 | 65.44 | 69.14 | 75.19 | 87.19 | 98.22 | 40.22 | 89.59 | 44.37 | 48.88 | 46.18 | 58.76 | 72.62 | 87.62 | 52.83 | 57.85 |
| Pr | 6.52 | 8.02 | 11.58 | 10.92 | 6.80 | 7.24 | 7.44 | 8.00 | 9.53 | 10.92 | 4.43 | 9.69 | 4.55 | 5.30 | 4.92 | 6.34 | 7.47 | 10.11 | 6.21 | 20.79 |
| Nd | 23.18 | 28.76 | 41.92 | 39.51 | 25.69 | 26.41 | 26.03 | 28.10 | 33.39 | 38.05 | 15.85 | 32.19 | 13.42 | 18.01 | 16.49 | 21.34 | 23.20 | 36.99 | 22.86 | 60.89 |
| Sm | 4.07 | 5.19 | 7.10 | 7.01 | 5.11 | 4.76 | 4.84 | 5.45 | 6.81 | 7.32 | 3.15 | 6.08 | 3.05 | 3.75 | 3.53 | 4.54 | 4.33 | 8.85 | 5.47 | 10.89 |
| Eu | 1.11 | 1.09 | 1.26 | 1.19 | 0.87 | 1.05 | 1.11 | 1.21 | 1.07 | 0.74 | 0.37 | 0.81 | 0.15 | 0.48 | 0.47 | 0.53 | 0.36 | 0.38 | 0.30 | 1.01 |
| Gd | 3.55 | 4.24 | 5.45 | 5.52 | 4.66 | 3.39 | 3.73 | 4.24 | 5.21 | 5.65 | 2.52 | 4.87 | 2.64 | 2.82 | 2.71 | 3.59 | 3.27 | 7.38 | 4.43 | 8.18 |
| Tb | 0.53 | 0.59 | 0.80 | 0.80 | 0.74 | 0.47 | 0.57 | 0.68 | 0.86 | 0.97 | 0.46 | 0.81 | 0.57 | 0.52 | 0.51 | 0.66 | 0.60 | 1.33 | 0.75 | 1.08 |
| Dy | 2.99 | 3.52 | 4.60 | 4.78 | 4.48 | 2.54 | 3.59 | 4.12 | 5.13 | 5.75 | 2.93 | 4.86 | 4.01 | 3.14 | 3.19 | 4.08 | 3.75 | 8.19 | 4.57 | 6.00 |
| Ho | 0.61 | 0.71 | 0.92 | 0.95 | 0.94 | 0.47 | 0.66 | 0.81 | 1.01 | 1.20 | 0.62 | 0.98 | 0.89 | 0.61 | 0.64 | 0.82 | 0.83 | 1.63 | 0.88 | 1.14 |
| Er | 1.78 | 2.10 | 2.82 | 2.86 | 2.85 | 1.33 | 2.16 | 2.41 | 3.03 | 3.52 | 1.82 | 2.94 | 2.97 | 1.86 | 1.87 | 2.44 | 2.67 | 4.74 | 2.43 | 3.44 |
| Tm | 0.27 | 0.32 | 0.39 | 0.43 | 0.45 | 0.17 | 0.32 | 0.38 | 0.46 | 0.54 | 0.29 | 0.44 | 0.47 | 0.30 | 0.30 | 0.38 | 0.45 | 0.71 | 0.37 | 0.54 |
| Yb | 1.88 | 2.27 | 2.70 | 2.78 | 3.15 | 1.23 | 2.18 | 2.49 | 3.19 | 3.70 | 2.00 | 3.22 | 3.39 | 2.04 | 2.08 | 2.73 | 3.37 | 4.89 | 2.45 | 3.81 |
| Lu | 0.30 | 0.34 | 0.40 | 0.42 | 0.47 | 0.17 | 0.32 | 0.38 | 0.47 | 0.57 | 0.36 | 0.47 | 0.51 | 0.32 | 0.32 | 0.43 | 0.53 | 0.75 | 0.38 | 0.60 |
| Hf | 4.39 | 4.56 | 5.42 | 5.11 | 4.47 | 4.44 | 4.89 | 4.52 | 5.03 | 4.33 | 2.36 | 5.71 | 4.05 | 2.96 | 2.38 | 3.26 | 4.40 | 5.14 | 4.04 | 3.72 |
| Ta | 0.66 | 0.70 | 1.08 | 1.08 | 1.00 | 0.65 | 0.82 | 0.85 | 1.22 | 1.58 | 0.46 | 1.51 | 2.07 | 1.39 | 1.21 | 2.22 | 1.93 | 2.25 | 1.45 | 1.53 |
| Tl | 0.52 | 0.73 | 1.05 | 0.87 | 0.62 | 0.61 | 0.83 | 1.30 | 0.96 | 0.99 | 0.39 | 1.44 | 1.46 | 1.37 | 1.35 | 1.08 | 1.17 | 1.46 | 1.41 | 2.48 |
| Pb | 22.31 | 17.76 | 34.83 | 33.99 | 16.54 | 23.25 | 25.30 | 19.93 | 16.29 | 21.95 | 3.88 | 32.90 | 36.59 | 26.41 | 26.40 | 26.24 | 28.24 | 19.91 | 21.00 | 14.85 |
| Th | 17.38 | 19.36 | 23.75 | 24.02 | 13.98 | 20.82 | 12.79 | 14.31 | 21.04 | 20.57 | 9.22 | 27.36 | 29.67 | 15.78 | 14.46 | 17.44 | 32.61 | 27.06 | 16.77 | 26.36 |
| U | 3.04 | 3.31 | 3.63 | 4.96 | 2.71 | 4.29 | 3.01 | 2.89 | 3.63 | 4.48 | 1.56 | 4.82 | 8.33 | 3.48 | 3.27 | 7.70 | 4.30 | 7.11 | 4.61 | 3.17 |
Analytical data of major (%) and trace element(ppm) of granites in the study area.
FIGURE 7

TAS (A) and A/CNK (B) diagrams of magmatic rocks.
On the primitive mantle normalized trace element spider diagram (Figure 8), Large ionic Lithophile Elements (LILE) such as K and Rb, Th, and U are enriched, and there is a strong loss of Ba, Sr, and High Field Strong Elements (HFSE) such as Nb, Ti, Ta, and P, which are similar to the geochemical characteristics of rocks in the subduction zone (
FIGURE 8

Chondrite Normalized REE distribution patterns (A), (C), (E) and primitive mantle normalized trace element spider diagram (B), (D), (F) of granitic rocks.
Discussion
Genetic Mechanism of Yanshannian Granite
Large-scale Yanshanian granites constitute the main part of southeastern China, and were formed related to the subduction of the Pacific plate, large-scale basaltic magma invasion, crust-mantle mixing, and extensive melting of crustal rocks (
According to the results of this paper, at least three acidic magmatic events occurred during Cretaceous: early stage of Early Cretaceous (about 138–135.1 Ma), late stage of Early Cretaceous (about 112–121 Ma) and the early stage of Late Cretaceous (about 93–96 Ma).
The age of the granite sample (ZZ07) in Zhangzhou area and the granite sample (HZ05) in the south of Huangshadong geothermal field in Huizhou are 138.4 ± 1.1 Ma and 135.1 ± 1.3 Ma, indicating that the granite body is the product of magmatic activity in the early stage of early Cretaceous. At the diagram of SiO2/(Na2O + K2O) (Figure 7A), sample dots fell within the granite region. The granites are characterized by weakly peraluminous (A/CNK = 1.02–1.08) (Figure 7B). The aluminum saturation index (A/CNK) ranges from 1.14 to 1.33. On the SiO2 − FeOT/(FeOT + MgO) and SiO2 − Al2O3 diagram (Figures 9A,B), most samples are plotted in the POG (post-Orogenic Grabite) zone (
FIGURE 9

SiO2-FeOT/(FeOT + MgO), (A) SiO2 − Al2O3, (B) Y − Nb, (C) and (Yb +Nb) − Rb, (D) diagrams of granites.
Discussion on the Burial Depth of Deep Granite
Seismic Profiles in Huangshadong Area of Guangdong Province
The two seismic profiles in Huangshadong area of Guangdong Province (Figures 10A,B) (
FIGURE 10

Profiles of seismic inversion, (A), (B) and its geological interpretation in Huangshadong area (
According to the profiles of seismic inversion (Figure 10), the buried depth of Tg (interface between sedimentary strata and granites) is generally located between 1,000–1,900 ms (corresponding depth of 1,400–2,200 m), and the seismic phase characteristics of Tg interface are significantly different from each other. The granite core sample from Well Huire one is similar to Yanshanian granite, indicating that seismic facies unit may correspond to the intrusive body in Yanshanian period, emplaced from the deep crust upward into shallow rock bed. 2050–2,900 ms (corresponding to the depth of 3,600–4,800 m) for the bedrock under the bottom of the interface (Td), reflection of geological units in phase axis continuity better, different from the adjacent granite rock mass. It may be older sedimentary rocks or metamorphic rocks with certain stratification.
Apparent Resistivity Inversion Profiles in North Hainan Province
In the area outside the east of Fushan Depression of Hainan Province, wide field electromagnetic detection has been conducted (Figure 11) (
FIGURE 11

Profiles of apparent resistivity inversion based on wide field electromagnetic method and corresponding geological interpretation in North Hainan Province (
The Significance of Granite to the Geothermal Energy
The heat source of geothermal energy mainly include heat transfer in the mantle, local anomalous heat transfers in the crust (magma chamber), and radioactive heat generation from granitic rocks. Surface heat flow, as a direct reflection of deep heat, usually accounts for 40–60% of the heat flow from the mantle. The heat flow caused by radioactive heat generation in the crust is slightly less than that from the mantle, accounting for about 40% and up to 50% in some areas (
Former research suggested that the heat generated by radioactive element decay in rocks is one of the main sources of Earth heat (
Previous studies have analyzed the overall heat generation rate of radioactive elements in the study area shown as low heat generation rate of strata and high heat generation rate of granitic rocks (
This is mainly attributed to Yanshanian granites formed from remelting of pre-Cambian rocks in this region (
The Significance of Granite to Deep Geothermal in Southeast China
Large-scale granite events occurred in the coastal area of southeast China during Mesozoic, especially Yanshannian (
Based on produced heat rate of typical magmatic rocks in Guangdong, Jiangxi and southeast of Fujian, previous scholars indicated that the radioactive heat production rate of most granitic rocks is greater than the average heat production rate of the Earth’s crust, signifying that the Yanshanian granite radioactive heat production have great contribution to regional heat (
Based on seismic inversion in the area, it is clear that in this area and the surrounding granite areas, based on P wave inversion of deep seismic profiles, shows 5–10 km depth of granite. A reasonable speculation in the area is that Yashaninan granites have great potential for the geothermal reservoirs. Moreover, the Moho surface in the whole southeast region is relatively shallow and the temperature of the Moho surface is relatively high (
Conclusion
1) The age of granite reservoirs are mainly 94.7–138.4 Ma, mainly late Yanshanian period. The geochemical characteristics of rocks show they are formed in the subduction zone signature, indicating they are formed related to the extensional environment formed by retractable subduction of the ancient Pacific plate.
2) Deep Yanshanian granites promote mantle heat transfer to the surface and increase the proportion of mantle heat flow in the heat flow value. Yanshanian granite has high content of Th, U, and K, and its radioactive decay heat generation provides heat source for the high-temperature geothermal in the study area. The combined action of the two forms the high-temperature geothermal energy in the study area.
3) The deep granite in the study area has huge potential for geothermal resources. The geothermal genesis model in the study area has reference significance for the understanding of geothermal in the southeast region or the calculation of geothermal reserves.
Statements
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
JL is responsible for experimental design, HZ and YZ are responsible for providing overall ideas, JF is responsible for data analysis, YZ and MW is responsible for instrument operation.
Funding
This study was financially supported by National Key Research and Development Project (No. 2019YFC0604903), National Natural Science Foundation of China (Grant No. U20B6001) and consultation research project of Chinese Academy of Engineering (No. 2019-XZ-35-04 and No. 2021-XZ-16-01).
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
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
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Summary
Keywords
southeast coastal areas, granite geothermal reservoir, geothermal resources, geochemistry, geochrohology
Citation
Zheng H, Luo J, Zhang Y, Feng J, Zeng Y and Wang M (2021) Geological Characteristics and Distribution of Granite Geothermal Reservoir in Southeast Coastal Areas in China. Front. Earth Sci. 9:683696. doi: 10.3389/feart.2021.683696
Received
22 March 2021
Accepted
30 July 2021
Published
13 August 2021
Volume
9 - 2021
Edited by
Shu Jiang, The University of Utah, United States
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Copyright
© 2021 Zheng, Luo, Zhang, Feng, Zeng and Wang.
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: Jun Luo, luojun.syky@sinopec.com
This article was submitted to Economic Geology, a section of the journal Frontiers in Earth Science
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