基于剩磁各向异性方法对华北下三叠统红层磁倾角浅化效应的研究

薛艺, 黄宝春, 赵千, 韩露, 李能韬. 2021. 基于剩磁各向异性方法对华北下三叠统红层磁倾角浅化效应的研究. 地球物理学报, 64(3): 916-924, doi: 10.6038/cjg2021O0112
引用本文: 薛艺, 黄宝春, 赵千, 韩露, 李能韬. 2021. 基于剩磁各向异性方法对华北下三叠统红层磁倾角浅化效应的研究. 地球物理学报, 64(3): 916-924, doi: 10.6038/cjg2021O0112
XUE Yi, HUANG BaoChun, ZHAO Qian, HAN Lu, LI NengTao. 2021. Reconnaissance on inclination shallowing effect of Lower Triassic red beds from North China Block by the anisotropy of remanence. Chinese Journal of Geophysics (in Chinese), 64(3): 916-924, doi: 10.6038/cjg2021O0112
Citation: XUE Yi, HUANG BaoChun, ZHAO Qian, HAN Lu, LI NengTao. 2021. Reconnaissance on inclination shallowing effect of Lower Triassic red beds from North China Block by the anisotropy of remanence. Chinese Journal of Geophysics (in Chinese), 64(3): 916-924, doi: 10.6038/cjg2021O0112

基于剩磁各向异性方法对华北下三叠统红层磁倾角浅化效应的研究

  • 基金项目:

    国家自然科学基金项目(41774074)资助

详细信息
    作者简介:

    薛艺, 女, 硕士研究生, 构造地质学专业, 构造磁学方向.E-mail: yixue@pku.edu.cn

    通讯作者: 黄宝春, 男, 教授, 主要从事古地磁学及其应用的教学和研究.E-mail: bchuang@pku.edu.cn
  • 中图分类号: P541;P318

Reconnaissance on inclination shallowing effect of Lower Triassic red beds from North China Block by the anisotropy of remanence

More Information
  • 本文报道利用岩石剩磁组构对华北下三叠统红层进行磁倾角浅化效应的进一步识别与校正研究结果.首先,采用45°等温剩磁各向异性方法,即通过沿与样品原始水平面(即层面)呈45°夹角方向施加磁化场获得等温剩磁,并进行逐步热退磁,获得平行于层面和垂直于层面的等温剩磁分量随外加磁场和热退磁温度的变化趋势,计算获得浅化因子f=0.70.其次,应用高场等温剩磁各向异性方法,结合峰值为100 mT的交变退磁和120℃热退磁处理,分离获得碎屑赤铁矿对剩磁各向异性的贡献;由直接测量获得的单颗粒碎屑赤铁矿的各向异性度(a=1.35),计算获得f=0.59.该结果与前人对刘家沟组红层进行E/I法磁倾角浅化校正的结果(f=0.60)具有很好的一致性;表明华北下三叠统刘家沟组红层磁倾角浅化效应显著,其浅化因子为f=0.59;高场等温剩磁各向异性方法是红层磁倾角浅化校正的最有效方法.同时,如果有足够的独立样品数,且特征剩磁来自于单一剖面或有证据表明多条采样剖面之间未发生显著的相对运动,E/I法对红层磁倾角浅化因子的估计也是可信的.

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  • 图 1 

    山西安泽地区区域地质简图(修改自周庭红等,2018),其中,1安泽剖面,2沁水剖面,3长子剖面

    Figure 1. 

    Simplified regional geological map of the Anze area showing paleomagnetic sampling areas after Zhou et al. (2018). 1 Anze Section, 2 Qinshui Section, 3 Changzi Section

    图 2 

    剩磁各向异性测量的九个方向(改自Bilardello, 2016)

    Figure 2. 

    The 9-position orientation scheme of Girdler (1961) to measure anisotropy of remanence (modified from Bilardello, 2016)

    图 3 

    (a) 刘家沟组红层代表性样品沿与岩层层面呈45°方向逐步递增外加磁场过程中,IRMX(平行于地层层面)和IRMZ(垂直于地层层面)对比图;(b) 外加磁场强度10~800 mT过程中IRMZ/IRMX对比图;(c) 热退磁过程中IRMZ/IRMX对比图

    Figure 3. 

    (a) Plots of IRMX (parallel to bedding) and IRMZ (perpendicular to bedding) acquisitions produced by applying magnetic fields at 45° to bedding as function of increasing field. (b) The IRMZ/IRMX as a function of pulse magnetic field up to 800 mT; and (c) the IRMZ/IRMX as a function of thermal demagnetization up to 680 ℃. The slope (IRMZ/IRMX) of the least-squares-fit for data points between 300 and 800 mT and between 600 and 680 ℃ is used to estimate the magnetic anisotropy of hematite, respectively

    图 4 

    双向等温剩磁获得曲线

    Figure 4. 

    Double IRM acquisition curve

    图 5 

    hf-AIR法测量的磁组构

    Figure 5. 

    Hf-AIR measured fabric

    表 1 

    刘家沟组红层样品45°AIR数据表

    Table 1. 

    The shallowing factor of 45°AIR for the Liujiagou Formation

    采点 IRMZ/IRMX
    (300~800 mT获得)
    IRMZ/IRMX
    (600~680 ℃获得)
    Site1 0.6339 0.7467
    Site2 0.8221 0.8224
    Site3 0.6048 0.6354
    Site4 0.6151 0.6905
    Site5 0.6510 0.6980
    Site6 0.6162 0.6838
    f 0.6572 0.7128
    σ 0.0752 0.0588
    注:f为浅化因子,σ为标准差.
    下载: 导出CSV

    表 2 

    沁水盆地刘家沟组红层高场等温剩磁各向异性张量的特征值和特征向量数据表

    Table 2. 

    Hf-AIR eigenvalues and eigenvectors of the unleached samples from the Liujiagou Formation, Qinshui Basin

    Sample Kmin Dec Inc Kint Dec Inc Kmax Dec Inc %RMS L F
    1-3 0.32088175 347.96 86.97 0.33222669 238.92 0.99 0.34689155 148.88 2.87 0.03 1.0441 1.0354
    1-4 0.31622094 114.82 8.98 0.32214069 281.44 80.78 0.36163837 24.49 2.10 0.03 1.1226 1.0187
    1-5 0.30762869 53.02 82.04 0.34308791 150.48 1.04 0.34928340 240.63 7.89 0.04 1.0181 1.1153
    1-9 0.31086367 205.33 81.66 0.33687297 328.92 4.64 0.35226333 59.48 6.91 0.03 1.0457 1.0837
    1-10 0.31664458 90.41 85.62 0.33711034 296.74 3.93 0.34624508 206.60 1.94 0.03 1.0271 1.0646
    2-3 0.32431120 112.56 64.70 0.33376652 252.09 19.78 0.34192231 347.67 15.13 0.03 1.0244 1.0292
    2-5 0.32132798 167.45 67.60 0.33396357 41.36 13.65 0.34470844 306.99 17.42 0.03 1.0322 1.0393
    2-8 0.32315037 155.35 67.89 0.33547482 307.01 19.68 0.34137478 40.51 9.69 0.03 1.0176 1.0381
    2-10 0.32135636 170.58 69.55 0.33256698 274.48 5.12 0.34607667 6.33 19.75 0.03 1.0406 1.0349
    3-5 0.32028690 274.76 80.58 0.33538401 67.54 8.39 0.34432909 158.17 4.25 0.05 1.0267 1.0471
    3-9 0.31979981 155.11 85.83 0.33708069 353.51 3.96 0.34311950 263.42 1.31 0.05 1.0179 1.0540
    5-1 0.31155932 280.96 71.07 0.32122377 71.53 16.63 0.36721691 164.17 8.78 0.06 1.1432 1.0310
    5-9 0.31376299 94.14 74.33 0.33704117 239.38 12.98 0.34919584 331.39 8.63 0.06 1.0361 1.0742
    8-1 0.31760779 45.17 58.88 0.33538893 238.61 30.42 0.34700331 145.11 5.95 0.09 1.0346 1.0560
    8-3 0.31655568 44.18 77.75 0.33679661 197.18 10.95 0.34664771 288.23 5.43 0.08 1.0292 1.0639
    8-4 0.31213912 50.02 59.54 0.33991507 252.04 28.6 0.34794581 156.74 9.61 0.08 1.0236 1.0890
    8-6 0.30675119 46.83 63.30 0.34302604 168.38 14.74 0.35022280 264.40 21.74 0.08 1.0210 1.1183
    8-7 0.30744728 60.26 59.65 0.34344280 256.91 29.29 0.34910992 162.81 7.25 0.09 1.0165 1.1171
    注:KminKintKmax分别是最小、中间、最大特征值;Dec、Inc分别是它们的偏角和倾角;% RMS是测量数据与二阶张量之间的均方根误差;LF分别是磁线理和磁面理.
    下载: 导出CSV

    表 3 

    E/I法与剩磁各向异性法磁倾角校正数据表

    Table 3. 

    Comparison of E/I and remanence anisotropy correction methods

    Method f IChRM Icorr
    E/I 0.60 30.9° 44.0°
    45°AIR 0.70 30.9° 40.5°
    hf-AIR 0.59 30.9° 45.4°
    注:f为浅化因子,IChRM为特征剩磁磁倾角,Icorr为校正后的磁倾角.
    下载: 导出CSV
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收稿日期:  2020-03-30
修回日期:  2020-05-08
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