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1.
基于大样本14 C测年资料的 华北平原沉积速率研究* 总被引：2，自引：1，他引：2
华北平原是我国研究程度较高的地区,历年来积累了大量的14 C测年资料。从这些资料中尽可能地提取沉积速率的信息,并进而研究华北平原沉积速率的变化及其与流域自然和人文环境变化之间的关系,是一个有重要意义的问题。利用华北平原456个地点的14 C年龄与样品埋深资料,计算出了各个样品所在层位沉积以来的平均沉积速率(RT),以此来近似反映各地点的平原沉积速率,并据此建立了RT随时间的变化关系。从古至今, RT有明显的增大趋势。以点群的上包线反映各时代的平原最大沉积速率,该指标可以反映华北平原的主体即黄河下游冲积平原的沉积速率。发现了最大平均沉积速率随时间变化过程中的4个突变点,分别为10000aB.P. , 5000aB.P. , 3000aB.P. 和1400aB.P. 。4个突变点将上包线分成5条折线,由此可以将近4万年以来的变化分成5个阶段。从古至今,5条折线的斜率增大,反映了平原沉积的加速过程; 并对4个突变点的成因进行了解释。阶段1,阶段2和阶段3沉积速率的加速是由自然原因造成的; 阶段4和阶段5沉积速率的加速则是由自然和人为原因共同造成的。从456个地点的14 C年龄与样品埋深资料中提取了距今4万年以来华北平原的平均沉积速率的信息,计算出平均沉积速率为0.9mm/a。按此求出,近4万年以来华北平原的沉积总厚度为36m。 相似文献
2.
博斯腾湖湖泊沉积物光释光年代测量* 总被引：2，自引：0，他引：2
使用光释光年代学的单片再生法测量了博斯腾湖沉积剖面中碳酸盐泥及粉砂质泥底部的浅湖相灰色粉细砂和风成沙的年龄,对剖面上部碳酸盐层中陆生植物残体进行了AMS 14 C测年。通过不同测片的等效剂量(De)值的分布状况评价了样品的晒褪程度,选择不随灵敏度校正后的自然释光信号变化的相对集中的等效剂量(De)值计算了样品的埋藏年龄。通过这些年龄结果的对比,发现石英矿物的OSL年龄和AMS 14 C年龄在地层上是一致的,表明尽管在浅湖相细砂中存在不完全晒褪,但根据相对较小而集中的De值计算得到的年龄结果是可靠的。这些年龄结果和地层资料揭示末次冰消期以来至早全新世,博斯腾湖处于无水干盆地向深水湖泊转化的浅水湖泊状态,现代深水博斯腾湖大约形成于距今8ka前后。 相似文献
3.
14C测年与示踪用于研究四万年来的全球变化 总被引：2，自引：1，他引：2
14C测年方法由于其假设前提经受过严格的检验,测年精确度极高,在全新世范围可达±50年。因此,在建立晚更新世以来的气候年表、各种地层年表、史前考古年表以及研究晚更新世以来的地壳运动、地貌及植被变化等方面起了重要作用。作为示踪剂14C与树木年轮相配合,揭示了近万年来地球磁场,太阳活动与全球气候变化的变化规律,以及它们间的相关关系。 相似文献
4.
对采自浙江西天目山地区的3株柳杉树盘,交叉定年后,测定了3株树轮δ13C的年序列,分析了3株树轮δ13C序列中所含的共同环境变化信息。用二项式拟合法去除气候因素引起的3个δ13C序列的高频变化,得到3个低频变化序列。分析了theLowDome冰芯记录的大气CO2浓度与树轮δ13C序列低频变化趋势的关系,建立了相应的转移函数,重建了天目山地区1685年以来大气CO2浓度变化。结果表明:用3株树轮δ13C序列重建的结果有较好的一致性,并与南极冰芯的记录及前人研究结果有很好的吻合。这一结果表明用同一地区不同树木个体的树轮δ13C序列的低频变化序列可以重建出基本一致的大气CO2浓度变化历史。 相似文献
5.
环渤海泥质海岸带近30年来获得的600余个放射性碳测年数据,确定了该地区晚更新世晚期以来的基本年代地层序列。但是,对14C数据的系统校正,迄未得到应有的重视,致使在应用14C数据解释地层和地质现象的年代时,存在着一定程度的混乱。文章对作者自己所采集和由国内外有关实验室测定的126个14C数据进行了系统校正,主要步骤包括分馏效应、地区性海洋贮存库效应及大气14C含量变化校正等。建议以-2.68‰PDB作为环渤海晚更新世晚期以来半咸水和开放浅海区(潮间带与潮下带上部)贝壳的地区性δ13C平均值。另外,讨论了在地区性海洋贮存库效应值获得之前的1990年代,以MARINE93与INTCAL93程序的平均校正年龄近似地视作该地区贝壳的校正值,以抵消这一类地区小型水体与大气迅速进行14CO2交换而对年龄值的影响。CALIB4.4校正结果表明,前述近似校正是可行的,其结果仍可沿用。文章经统一校正的年龄,最大限度地接近其太阳历纪年的"真实"年龄,从而有助于更加准确地重建该地区的晚更新世晚期以来的地质年代史,并可与考古纪年及其他测年方法获得的绝对年龄直接对比。 相似文献
6.
广东四会古森林地下生态系统14 C地层年代学研究* 总被引：1，自引：1，他引：0
运用AMS-14 C定年技术,研究了被埋藏水松古木的发育和死亡时间以及土壤剖面中总有机碳的14 C表观年龄和细根的14 C年龄。结果表明:该地区的水松古木开始发育和死亡的时间大致为4~3kaB.P. 。根据土壤有机碳14 C的表观年龄,该土壤剖面的14 C年代地层可以分为3层,分别为:1)表层,2634±32~3305±29aB.P. ; 2)腐殖层,3305±29~3813±31aB.P. ; 3)基底,3813±31~4544±33aB.P. 。基底、腐殖土层和表层的沉积速率分别为0.55mm/a, 4.33mm/a和0.26mm/a。 细根的14 C年龄变化范围为2290±29~3542±28aB.P. ,较同层位的土壤有机碳的年龄年轻。腐殖层土壤中有机碳含量高达33 ％ ~46 ％ ,大多数有机碳仍处于未分解状态。该地区自4~3kaB.P.以来,环境演化可能经历了由陆到沼泽再到被水淹没最后又变成陆地的过程,植被从以水松为优势种的森林群落演化成当前以常绿阔叶林为主的森林生态群落,气候和海平面变化、地质构造运动和人类活动是这种环境演化的主要驱动因子。 相似文献
7.
8.
对东北四海龙湾玛珥湖SHLF6孔纹层沉积物的137Cs放射性测量表明:137Cs比活度的最大值出现在55cm处,对应于1963年世界原子弹试爆高峰期。纹层计年表明0～6cm共有35个纹层层偶。从75cm到65cm,137Cs比活度从256±009dpm/g急剧增加到1868±017dpm/g,可能65cm对应于1954年。通过测量226Ra子核214Pb和214Bi（能量为295keV,352keV和609keV）放射的光子数获得226Ra比活度数据,然后求得过剩210Pb比活度（210Pbuns）。210Pbuns比活度随深度增加而呈指数衰减,其异常波动可能与人类活动以及沉积速率变化有关,例如55cm处210Pb比活度较高,与137Cs的峰值对应,这可能与1963年前后人工核实验的高峰有关,因为核试验不仅产生137Cs,而且可以产生208Pb和210Pb;45cm处210Pb比活度较低,而226Ra较高,可能与人类活动加剧,导致沉积速率增加有关。根据210PbunsCRS模式,SHLF6孔0～19cm的平均沉积速率为20mg/cm2·a,或约为011cm/a。210Pb测年数据与137Cs时标及纹层计年均有很好的一致性。四海龙湾玛珥湖发育的纹层为年纹层,可以建立高分辨率时间序列。 相似文献
9.
210Pb具有百年时间尺度沉积计年的重要价值。210Pbex计年假设：沉积物是封闭系统；进入水体的210Pb能有效地转移到沉积物中并不发生沉积后迁移；非过剩210Pb与其母体226Ra保持平衡。210Pbex计年可用稳定输入通量-稳定沉积物堆积速率模式、常量初始浓度模式或恒定补给速率模式。沉积物柱芯必须保持原态并以0．5～1cm间隔分截；用相应层节226Ra校正。沉积物表层混合作用及222Rn的丢失可能导致顶部210Pbex异常。季节性缺氧湖泊沉积物顶部可能存在210Pb及210Po的再迁移。210Pb与137Cs两种计年方法原理上具有根本差别。210Pb，137Cs与沉积纹理方法对比是准确计年的重要保证。 相似文献
10.
宇宙成因核素10 Be(半衰期1.5Ma)不但是古环境变化的示踪剂,而且具有确定地质年龄的能力。80个全岩样品的10 Be和化学分析数据表明,黄土高原约6Ma以来的红粘土和黄土序列中年龄校正的10 Be浓度与沉积物粒度和风化程度的化学指标具有显著的关系。根据这种关系建立的10 Be浓度与化学指标的经验回归线性模型,可以估计红粘土和黄土形成时的10 Be浓度,确定红粘土和黄土形成的10 Be放射性年龄。 相似文献
11.
黄土高原粉尘物质的搬运、沉积过程与来自中高纬度地区的季风密切相关。研究冬季风演化历史将有助于深入理解全球变化背景下,东亚地区气候变化的动力机制。通过对黄土高原的磁组构研究发现:1)各向异性度(P)与磁面理度(F)相关性较高,因此各向异性主要由磁面理引起,磁化率椭球体为压扁状;2)磁面理大致水平,K3近垂直于水平面;3)黄土平均磁面理为1.007,古土壤为1.004,古土壤层的磁面理与各向异性度均要低于其下伏的母质黄土层。成土作用在某种程度上破坏了黄土的原生磁组构;4)P,F和粉尘粒度间具有一定内在联系,一般而言冬季风越强,搬运的粉尘颗粒越粗,从而导致在沉积过程中形成较高的磁面理;5)K1方向的等面积赤平投影图和玫瑰花图解表明,末次间冰期以来该地区的主导风向为NW向冬季风。 相似文献
12.
本文介绍了国外利用AMS14C法研究极冰、海水中溶解的碳、大气中含碳,深海沉积含碳物等的最新进展和成果。这些成果表明,由于AMS14C法测定需要的样品量仅是常规测定用量的千分之一,因而为在地学领域中的应用开辟了广阔的前景。我国的AMS14C方法研究已经起步,新方法的建成和使用必将推动有关学科的进一步发展。 相似文献
13.
《Applied Geochemistry》2000,15(8):1191-1201
The impact of climatic and vegetation conditions over the past 15 Ka on the chemical composition and 14C dating of groundwater from the Franconian Albvorland aquifer system is discussed. Seven groundwaters over a flow distance of 25.5 km are investigated. Groundwater dating is made by 14C of dissolved inorganic carbon (DIC) and aqueous fulvic acid as well as 18O. 14C dating via fulvic acid gives groundwater ages consistent with climatic and vegetation records and variations in the groundwater composition. No correction for geochemical processes is required, since under these geochemical conditions fulvic acid remains stable over this time period and flow-distance. On the other hand, 14C dating via DIC requires correction of the 14C value due to perturbation by different geochemical processes. Up to a groundwater flow distance of approximately 17 km and an age of about 10 Ka, the 14C dating by DIC shows considerable dependence on the 14C-correction model applied. Beyond this groundwater age, 14C-DIC dating results in an overestimation by two to three 14C half-lives (T1/2=5730 a). This deviation may result from different groundwater recharge conditions at the end of the past glaciation and geochemical processes acting on DIC that cannot be adequately characterized. The present study has implications for humic substance mediated transport of pollutants in natural aquatic systems over long time periods. 相似文献
14.
山西平陆黄底沟入三门峡水库北侧发育了一级湖滨阶地(T3)和两级河流阶地(T2和T1)。阶地上覆黄土地层野外划分和室内磁化率测试结果与蓝田段家坡黄土地层的对比结果表明,T3上覆黄土地层最底部为古土壤层S2;T2最底部为黄土层L2中弱发育古土壤层L2-2;T1最底部为马兰黄土L1中弱发育古土壤层L1-4。根据黄土-古土壤年代序列及光释光(OSL)年龄测试结果,T3,T2和T1阶地分别于245kaB.P. ,149kaB.P.和50kaB.P. 前形成。其中,T3和T2阶地的形成时间,分别代表了山西平陆古三门湖开始消亡和最老黄河阶地形成的年代。古三门湖消亡与黄河贯通三门峡的时代是否一致,有待进一步研究。 相似文献
15.
N. Petersen N. Schembera E. Schmidbauer H. Vali 《Physics and Chemistry of Minerals》1987,14(2):118-121
On heating the paramagnetic clay mineral nontronite for ≈ 30 h at 970 °C in air, a new ferrimagnetic phase forms which was studied by magnetic techniques, microprobe analysis, x-ray diffraction and Mössbauer spectroscopy. The new phase has a Curie temperature T c ≈ 240°C and high magnetic anisotropy at room temperature with a spontaneous magnetization >12 Am2/kg. Semiquantitative microprobe analyses show Fe to be the dominating consistuent. X-ray analysis points to a lattice which may be similar to that of ?-Fe2O3 but differs from it in detail. 57Fe Mössbauer spectra, taken between 78 K and 295 °C, can be deconvoluted into three sextet subpatterns in the ferrimagnetic region which are well resolved at room temperature and exhibit a rather small line width. Above T c, a doublet is visible which is typical for Fe3+ ions. 相似文献
16.
The kinetics of non-convergent cation ordering in MgFe2O4 have been studied by measuring the Curie temperature (T
c) of synthetic samples as a function of isothermal annealing time. The starting material was a synthetic sample of near-stoichiometric
MgFe2O4, synthesised from the oxides in air and quenched from 900 °C in water. Ordering experiments were performed using small chips
of this material and annealing them at temperatures between 450 °C and 600 °C. The chips were periodically removed from the
furnace, and their Curie temperatures were determined from measurements of alternating-field magnetic susceptibility (χ) as
a function of temperature (T) to 400 °C. The Curie temperature of MgFe2O4 is very sensitive to the intracrystalline distribution of Fe3+ and Mg cations between tetrahedral and octahedral sites of the spinel crystal structure, and hence provides a very sensitive
probe of the cation ordering process. The χ-T curve for the starting material displays a single sharp magnetic transition at a temperature of 303 °C. During isothermal
annealing, the χ-T curve develops two distinct magnetic transitions; the first at a temperature corresponding to T
c for the disordered starting material and the second at a higher temperature corresponding to T
c for the equilibrium ordered phase. The size of the magnetic signal from the ordered phase increases smoothly as a function
of time, until equilibrium is approached and the shape of the χ-T curve corresponds to a single sharp magnetic transition for the homogeneous ordered phase. These observations demonstrate
that cation ordering in MgFe2O4 proceeds via a heterogeneous mechanism, involving the nucleation and growth of fine-scale domains of the ordered phase within
a matrix of disordered material. Disordering experiments were performed by taking material equilibrated at 558 °C and annealing
it at 695 °C. The mechanism of isothermal disordering is shown to involve nucleation and growth of disordered domains within
an ordered matrix, combined with continuous disordering of the ordered matrix. This mixed mechanism of disordering may provide
an explanation for the difference between the rates of ordering and disordering observed in MgFe2O4 using X-ray diffraction. The origin of the heterogeneous ordering/disordering mechanism is discussed in terms of the Ginzburg-Landau
rate law. It is argued that heterogeneous mechanisms are likely to occur in kinetic experiments performed far from equilibrium,
whereas a homogeneous mechanism may operate under slow equilibrium cooling. The implications of these observations for geospeedometry
are discussed.
Received: 12 May 1998 / Accepted: 25 June 1998 相似文献
17.
作为晚更新世与全新世地层年代测定的一种重要手段,14C测年被广泛应用于地质样品的年代测定。但对于14C数据的系统校正,迄今未得到应有的重视。文章在环渤海海岸带14C数据集(Ⅰ)的基础上,对所收集的421个由其他研究者获得的环渤海海岸带14C数据进行了系统校正。并讨论了百年、千年与万年尺度的14C数据校正效果。结果表明,直接测定值与系统校正值之间的差值常有数百年至两千年的差别。经统一校正的14C年龄,最大限度地接近样品太阳历纪年的“真实”年龄,从而有助于更加准确地重建该地区的晚更新世晚期以来的地质年代史,并可与考古纪年及其他测年方法获得的绝对年龄直接对比。 相似文献
18.
R. AUGIER P. AGARD P. MONIÉ L. JOLIVET C. ROBIN G. BOOTH-REA 《Journal of Metamorphic Geology》2005,23(5):357-381
The combination of metamorphic petrology tools and in situ laser 40Ar/39Ar dating on phengite (linking time of growth, compositions and P–T conditions) enables us to identify a detailed P–T–d–t path for the still debated tectonometamorphic evolution of the Nevado‐Filabride complex and infer new geodynamic‐scale constraints. Our data show an isothermal decompression (at 550 °C) from 20 kbar for the Bédar‐Macael unit and 14 kbar for the Calar Alto unit down to c. 3–4 kbar for both units at 2.8 mm year?1. At 22–18 Ma, this first part of the exhumation is followed by a final exhumation at 0.6 mm year?1 along a high‐temperature low‐pressure (HTLP) gradient of c. 60 °C km?1. The age of the peak of pressure is not precisely known but it is shown that it is around 30 Ma and possibly older, which is at variance with recent models suggesting a younger age for high‐pressure (HP) metamorphism. Most of the exhumation is related to late‐orogenic extension from c. 30 to 22–18 Ma. Thus the formation of the main ductile extensional shear zone, the Filabres Shear Zone (FSZ), occurred at 22–18 Ma and is clearly associated with a top‐to‐the‐west shear sense once the FSZ is well localized. The transition from ductile to brittle then occurred at c. 14 Ma. The final exhumation, accommodated by brittle deformation, occurred from c. 14 to 9 Ma and was accompanied, from 12 to 8 Ma, by the formation of nearby extensional basins. The duration of the extensional process is c. 20 Myr which argues in favour of a progressive slab retreat from c. 30 to 9 Ma. The change in the shape of the P–T path at 22–18 Ma together with strain localization along the main top‐to‐the‐west shear zone suggests that this date corresponds to a change in the direction of slab retreat from southwards to westwards. 相似文献
19.
C. Bender Koch C. A. Oxborrow S. Mørup M. B. Madsen A. J. Quinn J. M. D. Coey 《Physics and Chemistry of Minerals》1995,22(5):333-341
Magnetization curves and high-field Mössbauer spectra are used to deduce a model for the magnetic order in synthetic samples of δ-FeOOH (feroxyhyte), which takes account of the changes in magnetization when the samples are heated at 105 °C. Feroxyhyte is essentially a planar antiferromagnet with the net sublattice moments aligned parallel or antiparallel to c. Each particle acquires a net moment due to the very small number of layers along the c-direction, and the presence of surface steps causing the formation of ferrimagnetic domains with an odd number of layers. There is some spin canting which is related to the crystallinity of the sample. The decrease in magnetization following heating is mainly due to an increase in the extent of antiferromagnetic coupling between the closely packed ferrimagnetic particles, but changes in the spin canting within the bulk may also contribute. A typical, rather well crystallized specimen has magnetization σ=14 JT?1 kg?1 and Curie temperature T c=455 K. 相似文献