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1.
选择伊朗中部、南部及西北部地区的近２０条晚元古代－早古生代完整地层剖面，系统采集Ｓｏｌｔａｎｉｅｈ组、Ｂａｒｕｔ组、Ｚａｉｇｕｎ组、Ｌａｌｕｎ组及Ｍｉｌａ组古地磁样品９６０件．经测试和对比获得结论：Ｓｏｌｔａｎｉｅｈ组记录的地磁极性带为反向，Ｂａｒｕｔ组－Ｌａｌｕｎ组为正向，Ｍｉｌａ组又为反向．此成果完全可与国际地质科学联合会（ＩＵＯＳ）１９８９年建立的全球地层极性柱中相应时代的极性带对比．计算得出５个地层组的古地磁南极位置．古地磁研究表明，晚元古代－早古生代伊朗全境均属稳定地块，处于赤道南侧约１６°的低纬度区．此期间似无大幅度转动和纬度变化．  相似文献   

2.
Upper　Jaramillo极性转换期间地球磁场变化特征   总被引：6，自引：2，他引：6       下载免费PDF全文
利用陕西渭南剖面黄土层位Ｌ１０的剩余磁性获得了ＵｐｐｅｒＪａｒａｍｉｌｌｏ极性转换期间地球磁场的记录。与地球磁场方向相联系的极性转换持续时间约３２００ａ。极性转换过程虚地磁极（ＶＧＰ）主要位于美洲大陆及其边缘，根据Ｒｏｃｈｅｔｔｅ模型。由极性转换前后地球磁场处于稳定极性状态时的平均方向模拟出的地磁极移曲线与实测曲线不同。这说明所得结果并不是由极性转换前后地球磁场平均效应引起的，应该是地球磁场变化的实际记录。本文收集了１９８９年之前中朝陆块自晚石炭世至第三纪期间的古地磁极数据。应用分类过滤方法选出可靠的古地磁极，建立了中朝陆块新的视极移曲线。通过中朝陆块与扬子陆块视极移曲线的比较，对前人提出的两个陆块会聚的几种模式进行了检验。本文提出的旋转模式，对研究两陆块的会聚过程是较合理的新观点。  相似文献   

3.
Ｇｕｏ－ＭｉｎＺＨＡＮＧ（张国民）ＧｏｔＢａｃｈｅｌｏｒａｎｄＭａｓｔｅｒＤｅｇｒｅｅｓｉｎＧｅｏｐｈｙｓｉｃａｌＤｅｐａｒｔｍｅｎｔ，ｔｈｅＳｃｉｅｎｃｅａｎｄＴｅｃｈｎｏｌｏｇｙＵｎｉｖｅｒｓｉｔｙ．ｏｆＣｈｉｎａｉｎ１９６５ａｎｄ１９６８ｒｅｓ...  相似文献   

4.
附录Ｍ数字宽频带地震仪台站ＳｔａｔｉｏｎＬｏｃａｔｉｏｎＣｏｄｅＬａｔｉｔｕｄｅＬｏｎｇｌｔｕｄｅＰｒｏｇｒａｍＮｏｒｔｈＡｍｅｒｉｃａ：ＡｄａｋＩｓｌａｎｄＡｌａｓｋａ．Ｕ．Ｓ．Ａ．ＡＤＫ５１．８８Ｎ．１７６．６８Ｗ．ＩＲＩＳ（ＧＳＮ）ＵＳＮＳＮＢ...  相似文献   

5.
ＡＮＡＬＹＳＩＳＯＮＴＨＥＤＥＢＲＩＳＦＬＯＷＳＵＲＧＥＳ￥ＷａｎｇＧｕａｎｇｑｉａｎ（Ｐｒｏｆｅｓｓｏｒ，Ｄｅｐｔ．ｏｆＨｙｄｒａｕｌｉｃＥｎｇｉｎｅｅｒｉｎｇ，ＴｓｉｎｇｈｕａＵｎｉｖｅｒｓｉｔｙ）Ａｂｓｔｒａｃｔ：Ｂａｓｅｄｏｎｔｈｅｆｕｎｄａ...  相似文献   

6.
ＭＯＤＥＬＩＮＧＯＦＲＩＶＥＲＭＯＲＰＨＯＬＯＧＩＣＣＨＡＮＧＥＳＣｈａｒｌｅｓＣ．Ｓ．ＳＯＮＧ；ＹｉｆａｎＺＨＥＮＧ；ａｎｄＣｈｉｈＴｅｄＹＡＮＧ（Ｐｒｏｆｅｓｓｏｒ，Ｓｔ．ＡｎｔｈｏｎｙＦａｌｌｓＨｙｄｒａｕｌｉｃＬａｂｏｒａｔｏｒｙ，Ｄｅｐａｒ...  相似文献   

7.
甘肃灵台黄土剖面记录地球磁场长期变化的可靠性探析   总被引：11，自引：4，他引：7  
对甘肃灵台黄土／古土壤序列黄土层Ｌ１以及古土壤层ＳＯ和Ｓ１进行的较为详细的古地磁和岩石磁学研究表明：该剖面黄土剩余磁性在锁定过程中受到的平滑作用不大,因此能够记录百年尺度的地球磁场长期变化;而古土壤剩余磁性则受到强烈的平滑作用,不能记录百年尺度的地球磁场长期变化．在此基础上,对黄土层Ｌ１记录的地球磁场长期变化特征进行了分析,进一步证实了Ｍｏｎｏ Ｌａｋｅ和Ｌａｓｃｈａｍｐ漂移是两个独立的事件。  相似文献   

8.
ＳＯＭＥＡＰＰＲＯＡＣＨＥＳＦＯＲＳＴＵＤＹＩＮＧＴＨＥＩＮＴＥＮＳＩＴＹＯＦＳＭＡＬＬＲＩＶＥＲＡＧＧＲＡＤＡＴＩＯＮＶ．Ｎ．Ｇｏｌｏｓｏｖ（ＬａｂｏｒａｔｏｒｙｏｆＳｏｉｌａｎｄＦｌｕｖｉａｌＰｒｏｃｅｓｓｅｓ，ＦａｃｕｌｔｙｏｆＧｅｏｇｒａｐｈ...  相似文献   

9.
（赵根模，姚兰予，马淑芹）Ｔｈｅｓｔｒｅｓｓｆｉｅｌｄｖａｒｉａｔｉｏｎｃａｕｓｅｄｂｙｆａｕｌｔｉｎｇａｎｄｔｈｅｐｒｅｄｉｃｔｉｏｎｆｏｒｓｅｉｓｍｉｃｒｉｓｋ￥Ｇｅｎ－ＭｏＺＨＡＯ；Ｌａｎ－ＹｕＹＡＯａｎｄＳｈｕ－ＱｉｎＭＡ（Ｓｅｉｓｍｏｌｏｇ...  相似文献   

10.
极性转换期间地球磁场形态学研究   总被引：3，自引：1，他引：2  
本文对采自中国黄土高原西峰（35.7°N,107.6°E）和段家坡（34.2°N,109.2°E）两个剖面中黄土层L8和古土壤层S8的1281块定向古地磁样品做了详细的岩石磁学和古地磁学研究.证实了Matuyama-Brunhes（M-B）极性转换带位于L8的中下部.提出了下列观点:1.M-B极性转换过程与地球磁场方向变化相联系的持续时间为3600-4500a,而与地球磁场强度变化相联系的持续时间则为8000-9000a,即强度变化存在“超前和滞后” 效应;2.M-B转换场的形态是由三次快速倒转和一次不成功的倒转构成,或者说,转换场具有快速变换极性的振荡特征;3.M-B转换过程中地球磁场并不是以轴对称的非偶极子场为主,而是偶极子场至少与非偶极子场相当;4.中国黄土-古土壤沉积物所含磁性矿物的主要成分是磁铁矿,它是研究极性转换期间地球磁场详细结构的良好物质.  相似文献   

11.
The results of a palaeomagnetic investigation of a 27 m thick loess/palaeosol sequence in Viatovo (NE Bulgaria) are presented in this paper. The sequence consists of topsoil S0, seven loess horizons (L1–L7) and six interbedded palaeosols (S1–S6) overlying a red clay (terra rossa) complex. Magnetic viscosity experiments, IRM acquisition, AMS analysis and NRM stepwise alternating and thermal demagnetisation experiments of pilot samples were implemented for precise determination of the characteristic remanence and construction of a reliable magnetostratigraphical scheme. Analysis of IRM acquisition curves using the expectation – maximization algorithm of Heslop et al. [Heslop, D., Dekkers, M., Kruiver, P., van Oorschot, H., 2002. Analysis of isothermal remanent magnetization acquisition curves using the expectation – maximization algorithm. Geophys. J. Int., 148, 58–64] suggests that the best fitting is obtained by three coercivity components. Component 1 corresponds to SD maghemite/magnetite, while component 2 is probably related to the presence of oxidised detrital magnetites. The third component shows varying coercivities depending on the degree of pedogenic alteration of the samples and probably reflects the presence of detrital magnetite grains oxidised at different degree.

The relevance of the Viatovo section as a key representative sequence for the loess cover in the Danube basin is confirmed by the presence of geomagnetic polarity changes in the lower part of the sequence. The youngest one recorded in the seventh loess unit L7 can be identified as corresponding to the Matuyama/Brunhes palaeomagnetic polarity transition. Two normal magnetozones were found in the red clay complex, probably corresponding to the Jaramillo and Olduvai subchronozones of the Matuyama chron.  相似文献   


12.
New contributions to Chinese Plio-Pleistocene magnetostratigraphy   总被引：14，自引：0，他引：14  
A new collection of over 500 orientated hand-samples (of which 180 are red clays) from a 195 m loess/red clay section near Xian (109° 12′ E, 34° 12′ N), China, has been dated by magnetic stratigraphy. Biostratigraphic and previous magnetostratigraphic investigations gave a maximum age for the Chinese loess of 2.4 Ma, implying that the underlying Red Clay Formation is Pliocene in age. The present study yields a clearly defined magnetic polarity stratigraphy in good agreement with a polarity time scale developed by earlier workers. An interpretation of this magnetostratigraphy suggests a basal age for the loess series in this region of 2.5 Ma, and a minimum age for the base of the Red Clay Formation, which is also the base of the section, of 5.0 Ma.  相似文献   

13.
The Berriasian-Valanginian stage boundary near the town of Cehegin in the eastern Subbetic Cordillera of Spain is documented by a detailed ammonite zonation in pelagic limestones. Two magnetostratigraphic sections spanning the uppermost ammonite subzone of the Berriasian and the lower two zones of the Valanginian yielded identical magnetic polarity patterns. Remanent magnetization is predominantly carried by magnetite, and characteristic directions were obtained by thermal demagnetization. The mean characteristic directions from both sites have an inclination of 48°; however, the site declinations are divergent (030° and 074°) due to the tectonic disturbance of the region. The Cehegin polarity pattern can be correlated by means of ammonite and calpionellid zonation to the magnetostratigraphies of the Berriasian stratotype and several Italian sections, thereby enabling a unique correlation to the M-sequence magnetic polarity time scale. The Berriasian-Valanginian stage boundary is in the middle of normal-polarity chron M15n.  相似文献   

14.
Petromagnetic and magnetostratigraphic characteristics are obtained for the Tetritskaro section. The boundary layer at the Mesozoic/Cenozoic (K/T) boundary is fixed primarily by an abrupt rise in the paramagnetic magnetization (total Fe concentration) and, to a lesser degree, by an increase in the concentration of such magnetic minerals as goethite, hemoilmenite, and magnetite. The along-section distribution of titanomagnetite of volcanic origin and metallic iron of cosmic origin does not correlate with the K/T boundary and lithologic properties of the sediments.The boundary of the Mesozoic and Cenozoic geological eras lies within the reversed polarity chron C29r and is marked by an abrupt rise in the geomagnetic field paleointensity and an instability of paleomagnetic directions, rather than by a polarity change. The accumulation time of the boundary clay layer is about 1.5–2 kyr, while abrupt changes in the paleointensity and direction of the geomagnetic field encompass 30–40 kyr. Such long occurrence intervals of the events in question cannot be related to a short-term impact phenomenon.  相似文献   

15.
Gauss-Matuyama极性转换期间地球磁场方向和强度变化特征   总被引：13，自引：2，他引：11  
粒度分析和风化强度研究表明 ,黄土高原渭南阳郭剖面黄土层L33沉积期间成壤化作用相对较弱 .在此基础上 ,为研究极性转换期间地球磁场变化特征 ,本文对黄土层L33进行了详细的岩石磁学和古地磁学研究 ,其结果表明黄土层L33的主要载磁矿物为磁铁矿和磁赤铁矿 ,并以沉积剩磁为主 ;由逐步热退磁确定的特征剩磁 （ChRM ）揭示了G M（Gauss Matuyama）极性转换过程的持续时间为 9 43± 0 64ka;在G M极性转换之前 ,地球磁场曾发生过持续时间为 2 2± 0 1 3ka的短极性漂移事件 ;相对强度研究表明 ,G M极性转换期间地球磁场强度减弱 .  相似文献   

16.
Summary A magnetostratigraphic subdivision of the Danian and Upper Maastrichtian at Limhamn, souternmost Sweden, based upon 63 samples from drill cores (only up and down is known), is proposed. The boundary between the Maastrichtian and the Danian — situated in chron 29R — was determined by means of nanofossils. It is marked by a hardground surface indicating a hiatus with an estimated duration of 100 ka. The presence of chron 28R at the top of the Limhamn rock sequence and chron 30R in the Maastrichtian is indicated by single samples with reversed polarity. Net sedimentation rates have been calculated on the basis of the proposed magnetochronozones. the highest net sedimentation rate is found in the Danian part of chron 29R.  相似文献   

17.
Continous marine sedimentation characterizes many Late Permian to Early Triassic sections on the Yangtze terrane in South China. The Permo-Triassic (P/Tr) boundary section at Shangsi (Sichuan Province) consists of limestones intercalated with clays and mudstones which belong to the Wuchiapingian and Changxingian (Upper Permian) and the Griesbachian and Dienerian (Lower Triassic) stages. The P/Tr boundary is formed by a clay horizon with an unusually high iridium concentration. The intensity of natural remanent magnetization is very low with a mean of 0.15 mA m−1. About 40% of the samples contain secondary or unstable magnetization components only, whereas the remaining samples carry a characteristic remanent magnetization thought to reflect the polarity of the geomagnetic field during deposition with sufficient accuracy. Normal and reversed polarity of the characteristic magnetization constitute a pattern of at least six polarity zones, the P/Tr boundary being situated very close to the transition from a reversed to a normal polarity zone. The Shangsi polarity sequence represents part of the Illawarra interval of mixed polarity, the exact beginning of which has still to be determined.  相似文献   

18.
对山西襄汾丁村文化遗址群内大柴剖面进行的磁性地层学研究表明,松山与布容的极性界线（M/B）出现在距剖面顶部45 m处;磁化率对比结果显示,此位置正好与S8上部对应.由这种极性和磁化率的对应结果可推断,下、中更新统（Q1/Q2）的地层分界也应在距剖面顶部45 m处的S8上部,而不是传统上认为的Q1/Q2的地层分界,在距剖面顶部80 m处.这种以古地磁学为基础的新的划分方案,对丁村遗址群的对比以及丁村遗址年代的最终确定都有重要的指示意义.根据其沉积环境和地层特征推断,采样部位下部的磁化率低值带应为水成黄土.而岩石磁学研究结果显示,磁铁矿、赤铁矿和热不稳定性磁赤铁矿是大柴剖面沉积物中主要的磁性矿物;磁铁矿和赤铁矿同为高温稳定性磁性载体.  相似文献   

19.
Paleomagnetic records of the Gauss-Matuyama reversal were obtained from two loess sections at Baoji on the Chinese Loess Plateau. Stepwise thermal demagnetization shows two obvious magnetization components. A low-temperature component isolated between 100 and 200–250°C is close to the present geomagnetic field direction, and a high-temperature component isolated above 200–250°C reveals clearly normal, reversed, and transitional polarities. Magnetostratigraphic results of both sections indicated that the Gauss-Matuyama reversal consists of a high-frequency polarity fluctuation zone, but the characteristic remanent magnetization directions during the reversal are clearly inconsistent. Rock magnetic experiments demonstrated that for all the specimens with normal, reversed, and transitional polarities magnetite and hematite are the main magnetic carriers. Anisotropy of magnetic susceptibility indicates that the studied loess sediments have a primary sedimentary fabric. Based on virtual geomagnetic pole latitudes, the Gauss-Matuyama reversal records in the two sections are accompanied by 14 short-lived geomagnetic episodes (15 rapid polarity swings) and 12 short-lived geomagnetic episodes (13 rapid polarity swings), respectively. Our new records, together with previous ones from lacustrine, marine, and aeolian deposits, suggest that high-frequency polarity swings coexist with the Gauss-Matuyama reversal, and that the Gauss-Matuyama reversal may have taken more than 11 kyr to complete. However, we need more detailed analyses of sections across polarity swings during reversals as well as more high-resolution reversal records to understand geomagnetic behavior and inconsistent characteristic remanent magnetization directions during polarity reversals.  相似文献   

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