末次冰盛期山东半岛高分辨率气候环境变化

于溪川, 青芷仪, 周厚云. 末次冰盛期山东半岛高分辨率气候环境变化[J]. 海洋地质与第四纪地质, 2023, 43(6): 103-111. doi: 10.16562/j.cnki.0256-1492.2023010101
引用本文: 于溪川, 青芷仪, 周厚云. 末次冰盛期山东半岛高分辨率气候环境变化[J]. 海洋地质与第四纪地质, 2023, 43(6): 103-111. doi: 10.16562/j.cnki.0256-1492.2023010101
YU Xichuan, QING Zhiyi, ZHOU Houyun. High resolution climatic and environmental changes in Shandong Peninsula during the last glacial maximum[J]. Marine Geology & Quaternary Geology, 2023, 43(6): 103-111. doi: 10.16562/j.cnki.0256-1492.2023010101
Citation: YU Xichuan, QING Zhiyi, ZHOU Houyun. High resolution climatic and environmental changes in Shandong Peninsula during the last glacial maximum[J]. Marine Geology & Quaternary Geology, 2023, 43(6): 103-111. doi: 10.16562/j.cnki.0256-1492.2023010101

末次冰盛期山东半岛高分辨率气候环境变化

  • 基金项目: 国家自然科学基金“川东北石笋铀含量及同位素组成的控制机制与古降水指示意义” (41473093),“14—15世纪东南亚严重干旱在华南陆地地区的表现与意义”(41271212)
详细信息
    作者简介: 于溪川(1996—),女,硕士研究生,从事全球变化研究,E-mail:yuxichuann@163.com
    通讯作者: 周厚云(1967—),男,教授,从事全球变化研究,E-mail:hyzhou@gig.ac.cn
  • 中图分类号: P532;P736

High resolution climatic and environmental changes in Shandong Peninsula during the last glacial maximum

More Information
  • 末次冰盛期是末次冰期以来地球表面最寒冷的时期。通过对山东半岛地下画廊溶洞石笋DXHL3进行高精度230Th定年和高分辨率氧-碳稳定同位素分析,重建了该地区23.2~18.8 ka时期高分辨率夏季风气候环境变化历史。结果发现,山东半岛末次冰盛期夏季风气候存在显著的千年尺度波动;REDFIT分析表明,氧、碳同位素值均存在显著的2.2 ka周期。末次冰盛期山东半岛总体处于冷干状态,具体又可细分为4个阶段,即冷干(23.2~22 ka)-相对暖湿(22~21 ka)-冷干(21~19 ka)-相对暖湿(19~18.8 ka)。石笋DXHL3的δ18O变化趋势总体上与亚洲季风区内其他石笋记录相似,也与西太平洋暖池婆罗洲的石笋记录类似。这反映了末次冰盛期西太平洋暖池气候环境变化可能对山东半岛的夏季风气候变化产生了重要影响,推测西太平洋暖池表层海水温度变化引起的大气环流和黑潮的变化,是将气候环境变化信号从低纬地区传递到中高纬地区的纽带。

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  • 图 1  地下画廊溶洞区域概览

    Figure 1. 

    图 2  石笋DXHL3与年龄模式

    Figure 2. 

    图 3  石笋DXHL3的δ18O和δ13C记录及与极地冰芯、婆罗洲北部石笋及中国季风区内其他石笋δ18O 记录对比

    Figure 3. 

    图 4  石笋DXHL3的氧(a)和碳(b)同位素REDFITF分析结果

    Figure 4. 

    表 1  石笋DXHL3的U-230Th年代数据

    Table 1.  U-230Th dating results of stalagmite DXHL3

    样品号深度/mm238U/10−9232Th/10−12实测 δ234U[230Th/238U]活度比[230Th/232Th]/10−6未校正年龄/aBP校正年龄/aBPδ234Ui
    DXHL-13.524467±212220±83015.5±4.5
    0.67890±0.00072123563±44819774±3319774±333188.8±4.7
    DXHL-37.022657±28635±223147.5±5.5
    0.73498±0.00097432661±1483320794±4220794±423338.0±5.8
    DXHL-410.019816±2656±73189.6±6.4
    0.77094±0.001064531392±55019121654±4821654±483390.9±6.8
    DXHL-526.518180±25165±163120.4±6.8
    0.77806±0.001141413001±13823822270±5322270±533323.2±7.2
    DXHL-631.029792±43128±213118.2±8.0
    0.78114±0.001243004717± 49974422379±6122379±613321.8±8.6
    DXHL-759.027930±33323±153115.6±6.5
    0.78600±0.000991120882±5027922545±4922545±493320.6±6.9
    DXHL-864.224744±32621±233051.2±6.2
    0.77506±0.00111509515±1874022591±5122591±513252.4±6.6
    DXHL-990.023807±2366±203054.3±4.6
    0.77846±0.001164609934±136185522680±4622680±463256.5±5.0
    DXHL-10111.035390±39293±183186.8±5.5
    0.80779±0.001361609388±9793622793±5322793±533398.8±5.9
    DXHL-2132.831713±3250±93113.7±5.10.80362±0.000918416357±155067723106±4223106±423323.8±5.4
    注: λ230=9.1599×10−6 a−1λ234=2.8263×10−6 a−1λ238=1.55125×10−10 a−1 。δ234U=([234U/238U]活度比−1)×1000;234U初始值是根据230Th年龄获得的,即δ234U初始值=δ234U测量值×eλ234×t。校正230Th年龄假设初始的230Th/232Th摩尔比为(4±2)×10−6
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收稿日期:  2023-01-01
修回日期:  2023-03-27
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