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1.
万京林  李齐 《地震地质》1997,19(1):88-90
对采自红河断裂带元阳—嘎洒段的4个片麻岩和糜棱岩样品中的磷灰石进行裂变径迹(FT)测年,得到5.61~10.64Ma的年龄范围。结果表明,RRFZ段磷灰石FT年龄有从东南向西北变新的趋势。结合已有的钾长石多重扩散域(MDD)模式结果,得到该段150℃至110℃温度范围的冷却过程(冷却速度为3.4~9.45℃/Ma)。FT结果反映的特征与南海盆地得到的15Ma时断裂带所受力的转换的结果是一致的  相似文献   
2.
Twenty-four new zircon and apatite fission track ages from the Getic and Danubian nappes in the South Carpathians are discussed in the light of a compilation of published fission track data. A total of 101 fission track ages indicates that the Getic nappes are generally characterized by Cretaceous zircon and apatite fission track ages, indicating cooling to near-surface temperatures of these units immediately following Late Cretaceous orogeny.The age distribution of the Danubian nappes, presently outcropping in the Danubian window below the Getic nappes, depends on the position with respect to the Cerna-Jiu fault. Eocene and Oligocene zircon and apatite central ages from the part of the Danubian core complex situated southeast of this fault monitor mid-Tertiary tectonic exhumation in the footwall of the Getic detachment, while zircon fission track data from northwest of this fault indicate that slow cooling started during the Latest Cretaceous. The change from extension (Getic detachment) to strike-slip dominated tectonics along the curved Cerna-Jiu fault allowed for further exhumation on the concave side of this strike-slip fault, while exhumation ceased on the convex side. The available fission track data consistently indicate that the change to fast cooling associated with tectonic denudation by core complex formation did not occur before Late Eocene times, i.e. long after the cessation of Late Cretaceous thrusting.Core complex formation in the Danubian window is related to a larger-scale scenario that is characterized by the NNW-directed translation, followed by a 90° clockwise rotation of the Tisza-Dacia “block” due to roll-back of the Carpathian embayment. This led to a complex pattern of strain partitioning within the Tisza-Dacia “block” adjacent to the western tip of the rigid Moesian platform. Our results suggest that the invasion of these southernmost parts of Tisza-Dacia started before the Late Eocene, i.e. significantly before the onset of Miocene-age rollback and associated extension in the Pannonian basin.  相似文献   
3.
The Cretaceous to Palaeogene Alpine exhumation of previously buried Variscan basements is recorded in the southern portion of the Western Carpathians in the Gemeric and Veporic units. The Meso-Cenozoic collisional processes resulted in basement exhumation of the Tatric Unit from Palaeogene to Neogene times. According to zircon and apatite fission track data, the Gemeric Unit, an uppermost thick-skinned thrust sheet, cooled from depth levels of ∼10 up to 2.5 km (temperature interval of ∼250–60 °C) about 88–64 Ma ago, after the collapse of overlying Meliata-Turňa-Silica Mesozoic accretionary prism. The middle and lower thick-skinned thrust sheets, Veporic and Tatric units, cooled from the depths of ∼10 up to 2.5 km ∼110–40 Ma ago. The process was controlled by unroofing of footwall from beneath the Gemeric Unit. About 50–20 Ma ago, the internal zone of Tatric Unit gradually exhumed to depth of <2 km and some parts of the unit appeared at the surface level. However, the external zone of Tatric Unit was buried beneath the Eocene to Lower Miocene sedimentary successions and exhumed to the subsurface level at ∼21–8 Ma ago, as a result of oblique collision of the Western Carpathians with the European Platform.  相似文献   
4.
矿床保存变化研究的热年代学技术方法   总被引:1,自引:0,他引:1  
袁万明 《岩石学报》2016,32(8):2571-2578
成矿后矿床的保存与变化是矿床地质研究的重要组成部分,但研究程度不高,至今仍属于薄弱环节。矿床的保存与其隆升剥露密切相关,深入细致研究恢复矿区矿床的隆升和剥露历史,是揭示矿床保存变化的一种重要途径。本文重点论述研究矿床保存变化的技术方法,通过综合应用裂变径迹、(U-Th)/He、~(40)Ar-~(39)Ar年代学以及La-ICP-MS、锆石U-Pb定年等多种技术手段,研究成矿期次、构造活动期次以及二者间的联系,定量计算不同矿区、不同矿体、不同部位、不同时间的冷却隆升速率、隆升幅度、剥蚀速率和剥蚀量,探讨矿床保存深度与剥蚀量间的关系,总结不同时代、不同矿区矿床保存-变化过程,建立新的矿床地质-保存环境模型,完善矿床预测的综合示踪标志,最终预测不同矿区、不同地段隐伏矿床可能的产出深度,给出矿床可能已经被剥蚀殆尽的区段或地段,为深部找矿和区域成矿潜力评价提供依据。本文可为地质工作者的相关应用提供借鉴和手段。  相似文献   
5.
李理  钟大赉 《岩石学报》2018,34(2):483-494
对采自渤海湾盆地东南部济阳坳陷的碎屑岩进行测年研究,目的是通过碎屑锆石裂变径迹年龄揭示源区及其抬升剥露史和构造热事件,为华北克拉通构造演化特别是元古宙构造演化提供新的热年代学约束。14件上白垩统-上新统砂岩/粉砂岩岩心样品测年结果显示,锆石裂变径迹年龄分布在308±35Ma~145±19Ma之间,且所有单颗粒锆石径迹年龄均大于其沉积年龄,表明这些锆石为碎屑锆石。除1件样品外,其余13件样品的单颗粒年龄的,可以用来识别源区及其构造抬升。未通过χ2检验的锆石二项式最佳拟合峰值年龄集中分为9组:P1(1187Ma)、P2(720~548Ma)、P3(526Ma)、P4(330~319Ma)、P5(296~274Ma)、P6(213~201Ma)、P7(195~177Ma、162Ma)、P8(134~102Ma)和P9(94Ma),加上通过χ2检验的三叠纪(230Ma),指示源区中元古代-晚白垩世经历的9期构造抬升/岩浆活动。它们分别是发生在中元古代的芹峪运动、新元古代的构造抬升(约720~575Ma)、~548Ma的蓟县运动;古生代~526Ma早寒武世末构造运动、海西期构造抬升;晚三叠世印支期挤压构造抬升、早-中侏罗世印支期弱挤压抬升、早白垩世燕山期强烈岩浆活动及晚白垩世燕山晚期的抬升。华北克拉通北缘、克拉通内部古陆和盆地内部是渤海湾盆地上白垩统-上新统的主要物源区,古生代以来剥露速率逐渐增大,古生代、三叠纪、早-中侏罗世和白垩纪分别为0.020~0.033mm/y,0.033~0.042mm/y,0.034~0.049mm/y和0.041~0.097mm/y,反映源区白垩纪构造/岩浆活动最强烈。锆石裂变径迹年龄记录的中元古代-晚白垩世构造运动对探讨华北克拉通的构造演化特别是元古宙的演化提供了年代学证据,综合分析推断华北克拉通可能参与了Rodinia超大陆的形成与裂解。  相似文献   
6.
460矿床是火山岩型铀矿床。玻璃包裹体中裂变径迹研究表明:成矿岩体次流纹斑岩的原始铀含量为13.0ppm;裂变径迹测年龄法在强烈蚀变地区可以作为一种测年龄的有效辅助手段。  相似文献   
7.
位于藏东-滇西高原构造急剧转折地段的独龙江地区,其花岗岩体内系统垂向取样的9个花岗闪长岩样品的磷灰石裂变径迹年龄数据在4~6.8Ma之间.裂变径迹分析显示样品应处于剥露的部分退火带,其表观年龄主体表现为冷却年龄,部分具混合年龄特征.热史分析揭示出岩体至少记录了自晚中新世以来的3个显著冷却阶段.早期的时限可推至约13~8Ma,中、晚期的时限分别在约5.5Ma和2.8Ma,基本可以与区域上的不整合相对应.依据冷却史推导的各阶段剥蚀速率分别为0.10~0.12mm/a,0.26~0.3mm/a和0.85~1.02mm/a,可以与藏东-滇西高原周缘及邻区的盆地沉积记录相对应.研究结果为探讨藏东-滇西高原晚中新世以来的构造抬升-伸展变形提供了定量的参照时限.  相似文献   
8.
库鲁克塔格隆起位于塔里木盆地北缘,广泛出露前寒武基底岩石。辛格尔村附近出露的太古宙杂岩,包括灰色片麻岩、角闪岩、片岩、混合岩和大理岩。新元古代地层出露在库鲁克塔格隆起西部的兴地、西山口、辛格尔和杀马山附近,不整合在古元古代和中元古代的片麻岩、角闪岩和片岩之上,并被早古生代的地层不整合。因此,该地区是了解塔里木盆地前寒武基底热演化史的理想地区。本研究的目的是为了探索:①塔里木基底岩石最初于何时剥露于地表?②塔里木基底剥露以后是否经历过再次埋藏和剥露?③塔里木基底岩石构造热演化过程对大陆边缘不同构造事件的响应。为了获取塔里木北缘剥露史和冷却过程信息,我们开展了裂变经迹的研究。含磷灰石的样品采自库鲁克塔格隆起的兴地断裂两侧。样品池年龄介于146.0±13.4和67.6±6.7Ma 之间,平均经迹长度介于.11.79±0.14和13.89±0.27μm之间。根据样品年龄和样品所处的构造位置,样品可以分为3组。A 组样品包括 F2、F3、F4、F5和 F8,裂变经迹表观年龄约100~110Ma,通常位于未遭断层变形的地区。B 组样品包括 F7、F9和 F10,裂变经迹表观年龄小于80Ma,构造上位于断层上盘并靠近断层。C 组样品 F11具有最大的裂变经迹表观年龄146.0±13.4Ma。热模拟表明,库鲁克塔格地区的隆升剥露作用可以划分为四期,分别是早侏罗世晚期(180Ma)、晚侏罗世—早白垩世(144~118Ma)、晚白垩世早期(94~82Ma)和新生代晚期(约10Ma)。裂变经迹记录的库鲁克塔格多阶段隆升作用,是对亚洲南缘多期地体碰撞增生的响应。  相似文献   
9.
Recent data on He diffusion challenge the temperature sensitivity of apatite (U–Th)/He thermochronology: the damage induced by recoil of U and Th decay series during emission of α particles (α-recoil damage) has been proposed to modify He-diffusion properties through time. However, we propose that annealing of these irradiation defects may be an important phenomenon and may be significant in case of slowly-cooled or reheated basement rocks. To test this hypothesis, we developed a quantitative model including an explicit treatment of α-recoil damage, annealing, and their effect on He-diffusion kinetics, and calibrate it against literature data. Our model is based on two hypotheses: (1) helium is in equilibrium between an apatite crystal and its defects and (2) alpha-recoil damage annealing can be described analogously to fission-track annealing. This model has been embedded into a Monte Carlo simulation of helium production/ejection/diffusion and applied to data from the French Massif Central; a complex slowly-cooled terrain with burial reheating, where the thermal history has been constrained by previous fission-track (FT) data including FT length distributions. (U–Th)/He ages are close to the FT ages from the same samples and are generally reproducible among replicates, but some samples present He-age dispersion that is not correlated with crystal size. Our model reproduces the Massif Central data very well except for three samples where He ages are older than corresponding FT ages. We show that annealing of irradiation damage has an important impact on retentivity of helium and that the He content, [He] is only a rough approximation of the damage level. In particular our results show that independence of He ages on crystal sizes, in case of reheated samples, is a clear indication of the higher He retentivity induced by α-recoil defects and that an explicit treatment of defect annealing is required for a correct interpretation of (U–Th)/He ages in such a case. More generally a correlation with the crystal size can bring information on the thermal path only if the age of defects, well represented by the fission-track age, is available, due to the dependence of the partial retention zone on damages. Conversely, in case of rapid cooling or for samples having low U and Th contents, damage effects can be ignored without significant effects on He ages.  相似文献   
10.
Fission-track (FT) thermochronologic analysis was performed on zircon separates from rocks in and around the Nojima fault, which was activated during the 1995 Kobe earthquake. Samples were collected from the University Group 500 m (UG-500) borehole and nearby outcrops. FT lengths in zircons from localities > 25 m away from the fault plane as well as one 0.1 m away from the fault in the footwall are characterized by concordant mean values of  10–11 μm and unimodal distributions with negative skewness, which showed no signs of appreciable reduction in FT length. In contrast, those adjacent (< 3 m) to the fault at depths on the hanging wall side showed significantly reduced mean track lengths of  6–8 μm and distributions having a peak around 6–7 μm with rather positive skewness. The former pattern is interpreted to reflect cooling through the zircon partial annealing zone (ZPAZ), without later, partial thermal overprints. The latter indicates substantial track shortening due probably to secondary heating by a thermal event(s) that locally perturbed the geothermal structure. Modeled zircon FT length and age data of partially annealed samples from the UG-500 borehole revealed a cooling episode in the ZPAZ that started at  4 Ma within  3 m from the fault plane, whereas those from the Geological Survey of Japan 750 m borehole record cooling started at  31–38 Ma within  25 m from the fault. On the basis of one-dimensional heat conduction modeling as well as the consistency between the degree of FT annealing and the degree of deformation/alteration of borehole rocks, these cooling ages in both boreholes are interpreted as consequences of ancient thermal overprints by heat transfer or dispersion via fluids in the fault zone. Together with the zircon FT data of a pseudotachylyte layer recently analyzed, it is suggested that the present Nojima fault system was reactivated in the Middle Quaternary from an ancient fault initiated at  56 Ma at mid-crustal depths. Also shown is a temporal/spatial variation in terms of the thermal anomalies recorded in the fault rocks, implying heterogeneity of hot fluid flows in the fault zone.  相似文献   
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