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1.
根据对东昆仑地区东段哈拉郭勒—哈图一带不同高度基岩的系列锆石裂变径迹年龄分析，结合磷灰石裂变径迹年龄分析和中酸性侵入岩角闪石压力计分析揭示了东昆仑东段中生代的岩石隆升剥露冷却历史．巴隆哈图一带中酸性侵入岩角闪石压力计分析结果反映晚海西—印支期以来的总体剥露幅度约8～9km，早二叠世至晚三叠世初剥蚀作用极为缓慢，大约为20～40m／Ma．不同高程样品的锆石裂变径迹年龄分析结果揭示了东昆仑地区东段在中晚侏罗世处于缓慢的岩石隆升剥露阶段，其中中侏罗世相对较快，抬升速率77～88m／Ma，晚侏罗世相对较慢，抬升速率小于37m／Ma，且呈减慢趋势，这种减慢趋势反映了早中侏罗世之交强构造抬升期后的逐渐衰退．锆石裂变径迹—磷灰石裂变径迹年龄分析结果反映了中侏罗世以来的剥蚀速率一般不超过55m／Ma，岩石的剥蚀速率与岩石的抬升速率基本为同一量级，中侏罗世—白垩纪剥蚀作用与岩石抬升作用基本处于平衡状态。  相似文献   

2.
对新疆博格达-哈尔里克山火山岩和花岗岩的15个磷灰石样品和5个锆石样品的裂变径迹年龄测定表明,磷灰石的裂变径迹年龄变化于109.3～11.9 Ma之间,锆石的裂变径迹年龄变化于81.7～56.8 Ma之间.矿物对法计算得到,该地区晚白垩世至新生代中期的视剥露速率为0.157～0.222 mm/a.热史模拟结果表明,博格达-哈尔里克山自白垩纪以来经历了多期冷却剥露,分别是早白垩世(119～105 Ma)、晚白垩世晚期(67～65 Ma)、新生代早中期(47～31 Ma)和新生代晚期(12～7 Ma).白垩纪以来的天山变形作用,与亚洲南缘多期的地体碰撞增生有关.  相似文献   

3.
滇西临沧花岗岩基冷却的热年代学分析   总被引：2，自引：3，他引：2  
为利用热年代学方法重建临沧花岗岩基的冷却历史,测定了6块花岗岩样品的锆石U-Pb年龄、黑云母Rb-Sr等时线年龄、黑云母和钾长石的~(40)Ar/~(39)Ar年龄以及锆石和磷灰石的裂变径迹数据。分析表明,自结晶以来,岩基主体经历了较复杂的热演化,在两个基本阶段即早期快速冷却阶段和晚期缓慢冷却阶段上叠加了短周期的热扰动,从中—晚三叠世到早侏罗世末,冷却速率可以达到6℃～13℃/Ma,中侏罗世冷却缓慢,晚侏罗世到早白垩世早期,岩基快速冷却,平均速率达到5℃/Ma,早白垩世晚期到喜山运动前,为缓慢冷却阶段,平均速率仅为0．5℃/Ma,喜山运动后,受印藏碰撞的影响,岩基经历了两期冷却事件,早期冷却速率为5℃～10℃/Ma,晚期即5Ma以来冷却速率明显增大,特别是近3Ma以来的冷却速率达到16℃～20℃/Ma；早白垩世侵入的岩体(如样品S57),在侵入后快速冷却,晚白垩世以后与岩基主体同步冷却；宕基东倒糜棱岩带不是形成于150Ma,而可能是早期陆陆碰撞造山时推覆冲断的产物；自晚白垩世以来,岩基地区的总剥蚀厚度可达5000m左右,其中印藏碰撞引起的剥蚀可达3500m左右。  相似文献   

4.
哈萨克斯坦阿克斗卡特大型斑岩型铜矿床产在中亚成矿域巴尔喀什成矿带阿克斗卡矿田。本文根据花岗岩类岩石的锆石U-Pb、40Ar/39Ar和裂变径迹(FT)热年代学研究,结合前人研究成果,给出了阿克斗卡斑岩铜矿床从深成岩浆活动、成矿作用、区域冷却到剥露作用的全过程。阿克斗卡矿床及附近花岗岩类锆石SHRIMPU-Pb定年结果,给出科尔达尔岩体早期英云闪长岩的结晶年龄为335.7±1.3Ma;主成矿期的含矿二长花岗斑岩结晶年龄为327.5±1.9Ma,反映了阿克斗卡矿床斑岩型铜成矿作用的年龄。花岗岩类角闪石、黑云母、钾长石40Ar/39Ar热年代学分别给出矿物冷却年龄为310.6Ma、271.5Ma和274.9Ma,进一步限定了深成斑岩型铜成矿作用的时代和区域冷却的历史。磷灰石FT测年数据揭示,受区域构造作用的影响,阿克斗卡铜矿田在晚白垩世(91～68.0Ma)发生地块的差异隆升和剥露作用。  相似文献   

5.
巴尔喀什成矿带是世界著名的中亚成矿域斑岩型铜钼成矿带, 产出许多斑岩型铜钼矿床和一些石英脉-云英岩型钨钼矿床.对巴尔喀什成矿带西部的东科翁腊德、阿克沙套、扎涅特3个典型的石英脉-云英岩型钼钨矿床的成矿时代和剥露过程进行了地质热年代学研究.锆石SHRIMP U-Pb定年给出东科翁腊德、阿克沙套、扎涅特与成矿作用有关的花岗岩类岩浆作用的时代分别为293.6±2.7 Ma、306±1 Ma和304±4 Ma, 属海西晚期构造-岩浆活动的产物.花岗岩类40Ar/39Ar测年结果给出了与成矿有关岩体的冷却年龄, 其等时线年龄分别为292±3 Ma(阿克沙套黑云母)、288.8±3.6 Ma(阿克沙套钾长石)和278±5 Ma(东科翁腊德钾长石).磷灰石裂变径迹测年给出东科翁腊德、阿克沙套、扎涅特的年龄分别为92.1±5.7 Ma、92.2±5.0 Ma和80.3±4.9 Ma, 说明这3个矿床的剥露作用主要发生在晚白垩世.花岗岩类岩石U-Pb、40Ar/39Ar和裂变径迹热年代学研究, 揭示了巴尔喀什成矿带Mo-W矿床从深成岩浆侵入活动、成矿作用、区域冷却到剥露作用的全过程.   相似文献   

6.
分别出露于东、西秦岭的曹坪和沙河湾岩体、老君山和秦岭梁岩体 ,是秦岭全面碰撞后于三叠纪末 (T3 )侵入的花岗岩体 ,其冷却历史记录了秦岭陆内造山阶段的初期隆升过程。通过对角闪石、黑云母和钾长石的40 Ar/ 3 9Ar年龄测定 ,以及对钾长石40 Ar/ 3 9Ar年龄谱进行的多重扩散域模拟计算 ,发现东、西秦岭经历了完全不同的冷却历史 :从晚三叠世末至早侏罗世 ,东、西秦岭同时由 5 0 0℃开始快速冷却 ,之后东秦岭经过一个短暂的稳定期 (约 2 0Ma)后又持续快速冷却 ,至中侏罗世末即已通过 15 0℃等温线 (约地表下 3～ 5km) ;而西秦岭在早侏罗世至晚白垩世初的近 10 0Ma中一直处于稳定平缓的状态 ,至晚白垩世中期才快速冷却至 15 0℃。这种不同的冷却历史可能反映了东、西秦岭的差异隆升过程。  相似文献   

7.
位于中央造山带西段的东昆仑造山带因多期次造山和复杂演化历史而备受关注,约束其中生代隆升剥露历史,对于理解青藏高原大规模隆升在东昆仑地区的扩展及影响颇具意义。东昆仑造山带内中生代侏罗系-白垩系地层缺失严重,体现中生代以来强烈的隆升剥露过程,也是该区热演化的研究难点。本文通过对东昆仑造山带样品的磷灰石、锆石裂变径迹分析和热演化史研究,并结合东昆仑及周缘地区现有低温热年代学研究,识别出东昆仑造山带所经历的五次隆升冷却事件,即201~193Ma（早侏罗世）、172~152Ma（中-晚侏罗世）、120~98Ma（早白垩世末-早白垩世初）、98~20Ma（晚白垩世-中新世）及20~0Ma（中新世至今）。所获5个年龄组响应东昆仑地区所经历的构造热事件,其中201~193Ma年龄组响应南部羌塘地块与昆仑地块的碰撞事件;172~152Ma年龄组为中-晚侏罗世古特提斯洋闭合后,造山后伸展的构造事件的记录;120~98Ma热事件吻合拉萨地块和羌塘地块碰撞事件;98~20Ma年龄组为东昆仑地区长期缓慢剥蚀去顶过程的印证;20~0Ma的快速隆升剥露事件则为东昆仑周缘断裂系活化相伴,多期隆升剥蚀事件均得到地层不整合及沉积记录等研究成果的证实。区内剥蚀起始时间从由南到北逐渐变老,体现东昆仑地区隆升剥蚀的不均一性。  相似文献   

8.
赵珍  陆露  吴珍汉 《地学前缘》2019,26(2):249-263
本文综合磷灰石裂变径迹年龄(113~43 Ma)、锆石裂变径迹年龄(169~103 Ma)、锆石U-Pb年龄(215~206 Ma)、黑云母K-Ar年龄(186~178 Ma),通过磷灰石热史模拟,TASC图谱分析和矿物封闭温度年龄等手段,获得了中央隆起晚三叠世至今较为完整的冷却抬升历史。中央隆起主要经历了早侏罗世、晚侏罗世-早白垩世、晚白垩世-中新世早期和中新世晚期至今四期冷却事件,与南北羌塘板块后碰撞伸展、拉萨羌塘板块碰撞、新特提斯洋板片俯冲、印度欧亚板块碰撞以及中新世南北向走滑伸展存在动力学联系,造成11.4 km、2.85 km、4.3~5 km和0.85 km的抬升量。中央隆起在侏罗纪相对两侧盆地抬升,随着两侧盆地经历了侏罗纪的沉积增厚,与两侧盆地高差减小,在早白垩世早期可能位于海平面附近,随后快速抬升至2~2.5 km,统一接受晚白垩世红层沉积,并经历长期持续的逆冲推覆构造活动,进一步抬升至5 km,随后受到中新世古大湖夷平和南北向伸展作用影响,中央隆起相对盆地发生差异抬升。  相似文献   

9.
郯庐断裂带热年代学信息及其与大别造山带折返的关系   总被引：23，自引：2，他引：21  
大别山东缘早期郯庐韧性剪切带内的 T28- 12和 T28- 13白云母的 (181.4± 0.5) Ma和 (181.6± 0.8) Ma的 40Ar/39Ar坪年龄指示了郯庐早期左旋剪切的冷却时间为 181 Ma,这些年代学数据指示了郯庐同造山期左旋走滑热事件的存在.起源于华北、华南板块陆-陆碰撞过程中的这期断裂平移活动,发生在高压-超高压带主体部分折返至中地壳后的早侏罗世,推测其活动形式表现为造山带折返过程中高压-超高压带向 SE的斜向折返中形成的转换断层.郯庐晚期韧性剪切带内糜棱岩中白云母、黑云母的 40Ar/39Ar年龄,指示了 139 Ma前(早白垩世)发生的又一次左旋走滑冷却事件.在这期断裂带左行平移的同时,大别造山带东段出现了大规模的岩浆侵入及穹状隆升.剪切带糜棱岩中斜长石 40Ar/39Ar年龄指示剪切带在晚白垩世存在一期快速冷却事件,此次快速冷却事件的时间为 97～ 92 Ma.磷灰石裂变径迹研究成果揭示了 45～ 58 Ma前郯庐断裂带的一次快速冷却事件.这两次快速冷却事件分别对应于断裂带晚白垩世、古近纪两次伸展活动,并控制发育了断裂带东侧的潜山断陷盆地.而钾长石和磷灰石所在地记录的冷却时间显示,造山带内部的抬升都相应早于东缘的郯庐断裂带,反映造山带晚白垩世-古近纪的隆升并不受该断裂带伸展控制,而应是岩石圈拆沉的结果.  相似文献   

10.
郭超  张志勇  吴林  项敦峰  王楠  肖文交 《地球科学》2022,47(9):3417-3430
天山造山带中新生代快速剥露对于了解天山构造演化过程意义重大.然而,人们对于中新生代精确的冷却时间还一直存在争议.本文报道了塔里木盆地北缘库车河剖面中生界砂岩中碎屑磷灰石裂变径迹数据和早二叠世流纹岩热史演化模拟结果. 热年代学年龄趋势显示碎屑磷灰石裂变径迹的主要年龄组分为143.0~148.9 Ma和35.7~38.1 Ma,其中较年轻的组分已经完全重置,揭示了库车坳陷的剥露信息. 热史模拟结果显示了160~140 Ma的快速冷却事件. 结合库车河剖面前人的碎屑锆石U-Pb和重矿物数据,笔者认为欧亚南缘拉萨地体的拼贴是通过刚性的塔里木将挤压应力传递至天山,导致其在晚侏罗世?早白垩世强烈隆升剥蚀,大量碎屑被搬运沉积在塔里木盆地北缘,造成库车坳陷中广泛发育的早白垩世亚格列木组砾岩及其与晚侏罗世地层之间的角度不整合. 在欧亚板块南缘多块体持续拼贴的远程效应下,天山经历始新世快速隆升变形,变形持续向南扩展,导致库车坳陷在晚始新世遭受变形和抬升.   相似文献   

11.
吴林  杨列坤  师文贝  王非 《地质科学》2010,45(3):905-916
Ar同位素体系定年矿物的封闭温度范围广,并且可以获得650℃～150℃温度段的非线性冷却历史,因此~(40)Ar/~(39)Ar热年代学成为研究地质体热演化历史过程中最有效的工具之一。但是由于矿物中Ar同位素扩散机制还有一些问题没有清楚地被认识,因此在一定程度上制约了~(40)Ar/~(39)Ar热年代学的发展。本文介绍了目前应用最广泛的两种~(40)Ar/~(39)Ar热年代学模式:多重扩散域模式和多路径扩散模式,讨论了它们的发展现状、存在的问题、可能解决的方法以及今后的发展方向。  相似文献   

12.
K–Ar and 40Ar/39Ar ages have been measured on nine mafic volcanic rocks younger than 1 myr from the Snake River Plain (Idaho), Mount Adams (Washington), and Crater Lake (Oregon). The K–Ar ages were calculated from Ar measurements made by isotope dilution and K2O measurements by flame photometry. The 40Ar/39Ar ages are incremental-heating experiments using a low-blank resistance-heated furnace. The results indicate that high-quality ages can be measured on young, mafic volcanic rocks using either the K–Ar or the 40Ar/39Ar technique. The precision of an 40Ar/39Ar plateau age generally is better than the precision of a K–Ar age because the plateau age is calculated by pooling the ages of several gas increments. The precision of a plateau age generally is better than the precision of an isotope correlation (isochron) age for the same sample. For one sample the intercept of the isochron yielded an 40Ar/36Ar value significantly different from the atmospheric value of 295.5. Recalculation of increment ages using the isochron intercept for the composition of nonradiogenic Ar in the sample resulted in much better agreement of ages for this sample. The results of this study also indicate that, given suitable material and modern equipment, precise K–Ar and 40Ar/39Ar ages can be measured on volcanic rocks as young as the latest Pleistocene, and perhaps even the Holocene.  相似文献   

13.
The mineral separate GA1550 biotite has become an international standard for K/Ar and 40Ar/39Ar dating studies, although it was prepared as an intralaboratory standard at ANU to monitor tracer depletion from a gas pipette. It is one of a small number of samples that has been calibrated against 38Ar tracers, some of which had been mixed with known amounts of atmospheric argon, so that a so-called primary calibration has been performed. By measuring GA1550 biotite against additional tracers from the same batch we have determined the radiogenic argon content of this sample as 1.342 (± 0.007) × 10? 9 mol/g, and together with the measured K content of 7.645 (± 0.050) weight percent, we derive a best estimate for the K/Ar age as 98.5 ± 0.5 Ma, where the error is derived from averaging the ages determined relative to the 38Ar tracer.  相似文献   

14.
The 40Ar/39Ar dating technique requires the activation of 39Ar via neutron irradiation. The energy produced by the reaction is transferred to the daughter atom as kinetic energy and triggers its displacement, known as the recoil effect. Significant amounts of 39Ar and 37Ar can be lost from minerals leading to spurious ages and biased age spectra. Through two experiments, we present direct measurement of the recoil-induced 39Ar and 37Ar losses on Fish Canyon sanidine and plagioclase. We use multi-grain populations with discrete sizes ranging from 210 to <5 μm. One population consists of a mixture between sanidine and plagioclase, and the other includes pure sanidine.We show that 39Ar loss (depletion factor) for sanidine is ∼3% for the smallest fraction. Age spectra of fractions smaller than ∼50 μm show slight departure from flat plateau-age spectrum usually observed for large sanidine. This departure is roughly proportional to the size of the grain but does not show typical 39Ar loss age spectra. The calculated thickness of the total depletion layer d0(sanidine) is 0.035 ± 0.012 (2σ). This is equivalent to a mean depth of the partial depletion layer (x0) of 0.070 ± 0.024 μm. The latter value is indistinguishable from previous values of ∼0.07-0.09 μm obtained by argon implantation experiments and simulation results.We show that it is possible to adequately correct ages from 39Ar ejection loss provided that the d0-value and the size range of the minerals are sufficiently constrained. As exemplified by similar calculations performed on results obtained in a similar study of GA1550 biotite [Paine J. H., Nomade S., and Renne P. R. (2006) Quantification of 39Ar recoil ejection from GA1550 biotite during neutron irradiation as a function of grain dimensions. Geochim. Cosmochim. Acta70, 1507-1517.], the d0(biotite) is 0.46 ± 0.06 μm. The significant difference between empirical results on biotite and sanidine, along with different simulation results, suggests that for biotite, crystal structures and lattice defects of the stopping medium and possibly subsequent thermal degassing (due to ∼150-200 °C temperature in the reactor or extraction line bake out) must play an important role in 39Ar loss.The second experiment suggests that 37Ar recoil can substantially affect the age via the interference corrections with results that suggest up to ∼98% of 37Ar can be ejected from the ∼5 μm grain dimension.Further investigation of silicates of various compositions and structures are required to better understand (and correct) the recoil and recoil-induced effects on both 39Ar and 37Ar and their influences on 40Ar/39Ar dating.  相似文献   

15.
In the case of volume diffusion, the closure temperature of a mineral is function of, among other factors, the characteristic diffusion dimension, which can be approximated by the grain size of the mineral analysed for grains smaller than or similar in size to the diffusion domains. The theoretical possibility of single mineral grain size thermochronology had been demonstrated empirically in earlier studies, mostly using biotite. In order to examine the potential of this method, it was tested alongside the widely used multi-mineral 40Ar/39Ar thermochronology. The sample comes from the granitic McLean pluton, in the south section of the Grenville orogeny. Seven grain size separates of biotite (ranging between 90 and 1000 μm), eight size fractions of amphibole (between 63 and 1000 μm), and three size fractions of K-feldspar (250-600 μm) were extracted and dated by the laser step-heating 40Ar/39Ar method. The total gas ages obtained behave as theoretically predicted, with increasing ages for increasing grain sizes, including for K-feldspar, but with the exception of the smallest and the largest grains for biotite and amphibole. The calculated cooling rates are ca. 0.7 °C/Ma for K-feldspar, ca. 2.5 °C/Ma for biotite, and ca. 11 °C/Ma for amphibole, corresponding very well to a monotonic cooling of the McLean pluton. A quick initial thermal re-equilibration with the cooler host-rocks is followed by a much slower cooling on a thermal path parallel to that of the Frontenac Terrain situated immediately to the southeast. The validity of the single mineral grain size thermochronology is demonstrated by comparison with the thermal evolution of the adjacent units and with the cooling history derived from a multi-mineral thermochronology, suggesting that it can be routinely used. The application of this method can be hampered by insufficiently low analytical uncertainties.  相似文献   

16.
The effects of deformation on radiogenic argon (40Ar∗) retentivity in mica are described from high pressure experiments performed on rock samples of peraluminous granite containing euhedral muscovite and biotite. Cylindrical cores, ∼15 mm in length and 6.25 mm in diameter, were drilled from granite collected from the South Armorican Massif in northwestern France, loaded into gold capsules, and weld-sealed in the presence of excess water. The samples were deformed at a pressure of 10 kb and a temperature of 600 °C over a period 29 of hours within a solid medium assembly in a Griggs-type triaxial hydraulic deformation apparatus. Overall shortening in the experiments was approximately 10%. Transmitted light and secondary and backscattered electron imaging of the deformed granite samples reveals evidence of induced defects and for significant physical grain size reduction by kinking, cracking, and grain segmentation of the micas.Infrared (IR) laser (CO2) heating of individual 1.5-2.5 mm diameter grains of muscovite and biotite separated from the undeformed granite yield well-defined 40Ar/39Ar plateau ages of 311 ± 2 Ma (2σ). Identical experiments on single grains separated from the experimentally deformed granite yield results indicating 40Ar∗ loss of 0-35% in muscovite and 2-3% 40Ar∗ loss in biotite. Intragrain in situ ultraviolet (UV) laser ablation 40Ar/39Ar ages (±4-10%, 1σ) of deformed muscovites range from 309 ± 13 to 264 ± 7 Ma, consistent with 0-16% 40Ar∗ loss relative to the undeformed muscovite. The in situ UV laser ablation 40Ar/39Ar ages of deformed biotite vary from 301 to 217 Ma, consistent with up to 32% 40Ar∗ loss. No spatial correlation is observed between in situ40Ar/39Ar age and position within individual grains. Using available argon diffusion data for muscovite the observed 40Ar∗ loss in the experimentally treated muscovite can be utilized to predict average 40Ar∗ diffusion dimensions. Maximum 40Ar/39Ar ages obtained by UV laser ablation overlap those of the undeformed muscovite, indicating argon loss of <1% and an average effective grain radius for 40Ar∗ diffusion ?700 μm. The UV laser ablation and IR laser incremental 40Ar/39Ar ages indicating 40Ar∗ loss of 16% and 35%, respectively, are consistent with an average diffusion radius ?100 μm. These results support a hypothesis of grain-scale 40Ar∗ diffusion distances in undeformed mica and a heterogeneous mechanical reduction in the intragrain effective diffusion length scale for 40Ar∗ in deformed mica. Reduction in the effective diffusion length scale in naturally deformed samples occurs most probably through production of mesoscopic and submicroscopic defects such as, e.g., stacking faults. A network of interconnected defects, continuously forming and annealing during dynamic deformation likely plays an important role in controlling both 40Ar∗ retention and intragrain distribution in deformed mica. Intragrain 40Ar/39Ar ages, when combined with estimates of diffusion kinetics and distances, may provide a means of establishing thermochronological histories from individual micas.  相似文献   

17.
Nine glauconite samples with relatively high K concentrations and which appear to be well crystallized using normal X-ray diffraction techniques have been studied using the 40Ar39Ar method. The glauconite 40Ar39Ar apparent ages exceed their KAr, RbSr and, in most cases, stratigraphic ages by substantial amounts. 40Ar39Ar release spectra sometimes yield plateaus but these apparent ages have no geological significance. The results indicate that 39Ar is lost by recoil from mineral grains during neutron irradiation, consistent with previously reported observations. The amount of 39Ar loss was measured by isotope dilution for four samples and varied from 29% to 17%. In contrast, radiogenic 40Ar is quantitatively retained during irradiation. The very fine blades which make up glauconite grains yield the mineral susceptible to large amounts of 39Ar loss and unsuitable for 40Ar39Ar dating.  相似文献   

18.
^40Ar／^39Ar测年中的冷却年龄和变形年龄   总被引：3，自引：1，他引：2  
王勇生  朱光 《地质通报》2005,24(3):285-290
^40Ar／^39Ar法年龄数据的解释与Ar同位素在矿物中的封闭温度有关。冷却年龄只能限制变质——变形事件发生的时间区间,不能真正代表地质事件的发生时间。因此,必须想办法得到变形年龄。本文从封闭温度概念出发,探讨了压力、冷却速率、有效扩散范围和几何形态、颗粒大小、动力学参数等对矿物封闭温度的影响,介绍了新近提出的“封闭窗”概念,并讨论了在什么情况下可以获得变形年龄。  相似文献   

19.
李建红  梁良  卫三元 《地球学报》2005,26(Z1):244-247
下庄铀矿田的糜棱岩按产状可以分为两种，即韧性剪切带中的糜棱岩和硅质碎裂岩带中的糜棱岩，两种糜棱岩具有不同的特征，反映糜棱岩的不同成因和环境。两个测年样确定糜棱岩年龄为140-140Ma，它与晚期花岗岩活动高峰期相近，与早期铀矿化年龄耦合。认为韧性剪切带是早期花岗岩体再度处于假塑性状态下的变形产物，岩石的韧性变形与铀的成矿在时间上和空间上密切相关，控矿因素与成矿机制与韧性剪切变形机制息息相连，这些信息有助于早期铀矿的勘查。  相似文献   

20.
《Chemical Geology》2002,182(2-4):583-603
New K/Ar ages based on 40Ar/39Ar incremental heating of <2- and 2–20-μm size fractions of the well-characterized, carbonate-bearing Heinrich layers of core V28-82 in the eastern North Atlantic are 846–1049 Ma, overlapping with conventional K/Ar ages from the same Heinrich layers on the Dreizack seamounts of 844–1074 Ma. This agreement suggests the equivalence of the methods in fine-grained terrigenous sediments. Additionally, Heinrich layer H2 yielded a 40Ar/39Ar-based K/Ar age of 970±4 from Orphan Knoll in the southern Labrador Sea, within the range found in eastern North Atlantic Heinrich layers. Thus, the K/Ar data are robust in their indication of a dominant Labrador Sea ice-rafted source to even the finest sediment fraction in the eastern North Atlantic during the massive detrital carbonate-bearing Heinrich events of the last glacial cycle (H1, H2, H4, H5). Close correspondence of the radiogenic argon concentration (40Ar*) from the de-carbonated <63-μm fractions from V28-82 with the <2- and 2–16-μm fractions from the Driezack seamounts demonstrates that this measurement is a rapid and reliable method for correlating these layers within their belt of distribution.A 40Ar/39Ar-based K/Ar age of 433±5 million years for H11 in V28-82 is within the range of published data from background sediments in the eastern North Atlantic, and is consistent with published results across this interval in the Driezack seamounts. In contrast, the 40Ar/39Ar-based K/Ar age of H11 in the western Atlantic core EW9303-JPC37 is 614±5 million years. A brick red sample from approximately the interval of H3 of core EW9303-GGC40 yielded a 40Ar/39Ar-based K/Ar age of 567±1 million years, comparable to the published range of 523–543 Ma from the 2–16-μm fractions from that interval on the Dreizack seamounts. Both JPC37 and GGC40 are located in the path of the North Atlantic Drift. The older ages from western samples of H3 and H11 may result from dilution of a Hudson Strait source or an elevated age from southeastern Laurentide sources.  相似文献   

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