中国地质学会岩矿测试技术专业委员会、国家地质实验测试中心主办

大样本量(large-n)碎屑锆石U-Pb年代学分析技术研究进展

陈玺贇, 吕开来, 王平, 黄湘通, 孔兴功. 大样本量(large-n)碎屑锆石U-Pb年代学分析技术研究进展[J]. 岩矿测试, 2022, 41(6): 920-934. doi: 10.15898/j.cnki.11-2131/td.202112260209
引用本文: 陈玺贇, 吕开来, 王平, 黄湘通, 孔兴功. 大样本量(large-n)碎屑锆石U-Pb年代学分析技术研究进展[J]. 岩矿测试, 2022, 41(6): 920-934. doi: 10.15898/j.cnki.11-2131/td.202112260209
CHEN Xiyun, LYU Kailai, WANG Ping, HUANG Xiangtong, KONG Xinggong. A Review of Research Progress on the Analytical Method of Large-n Detrital Zircon U-Pb Geochronology[J]. Rock and Mineral Analysis, 2022, 41(6): 920-934. doi: 10.15898/j.cnki.11-2131/td.202112260209
Citation: CHEN Xiyun, LYU Kailai, WANG Ping, HUANG Xiangtong, KONG Xinggong. A Review of Research Progress on the Analytical Method of Large-n Detrital Zircon U-Pb Geochronology[J]. Rock and Mineral Analysis, 2022, 41(6): 920-934. doi: 10.15898/j.cnki.11-2131/td.202112260209

大样本量(large-n)碎屑锆石U-Pb年代学分析技术研究进展

  • 基金项目:
    国家自然科学基金项目(41572154);江苏省自然科学基金项目(BK20211270)
详细信息
    作者简介: 陈玺贇,硕士研究生,从事碎屑锆石U-Pb年代学物源示踪方法学研究。E-mail:xiyunchen1999@outlook.com
    通讯作者: 王平,博士,副教授,硕士生导师,主要从事沉积学、构造地貌学研究。E-mail:tigerwp@njnu.edu.cn
  • 中图分类号: O657.63

A Review of Research Progress on the Analytical Method of Large-n Detrital Zircon U-Pb Geochronology

More Information
  • 碎屑锆石U-Pb年代学是识别沉积物来源和确定地层最大沉积年龄的重要工具。利用激光剥蚀电感耦合等离子体质谱(LA-ICP-MS)进行物源分析的碎屑锆石测试数量为60~120颗,在这个范围内,年龄组分通常不能从样本中识别出来。近年来,为提高物源分析的可靠性,LA-ICP-MS测试要求有更多数量的锆石颗粒(n≥300),甚至大于1000颗的大样本量(large-n)试验。大样本量碎屑锆石U-Pb年代学的出现对数据测试方法、处理和评估都提出了挑战。本文通过对国内外大样本量文献进行梳理,总结了大样本量碎屑锆石U-Pb年代学在测试方法、数据处理以及数据评估方面的进展。首先,单颗粒测试需要对U、Pb同位素信号进行快速获取,这可以通过改进气溶胶传输效率实现,“峰值”信号模式代替“平顶”信号接收也可实现快速测试。其次,大样本量产生的数据,需要高效的数据处理协议和强大的软件(如Iolite)进行处理,以减少实验室间比较的误差;针对U-Pb数据处理流程,介绍了同位素分馏校正以及不确定度传播等方面的方法优化;此外,还引入了累积计数法和线性回归校正法两种处理方法专门处理“峰形”信号。在数据评估方面,新的U-Pb和Pb-Pb年龄不谐和度计算方法的提出,如采用Aitchison谐和距离,使数据过滤更加合理。基于上述新进展,对仪器和处理软件的选取进行了讨论,并对未来大样本量碎屑锆石U-Pb年代学分析的自动化、规范化提出了展望。基于已有研究,未来大样本量碎屑锆石U-Pb年代学的发展具有广阔前景,在物源示踪及确定地层年代等研究中将发挥更大的作用。

  • 加载中
  • 图 1  气溶胶快速引入系统(Aerosol Rapid Introduction System,ARIS)与激光和ICP-MS连接示意图:激光端与PEEK管相接,并通过ARIS转接器将气溶胶传输至ICP-MS(据文献[25])

    Figure 1. 

    图 2  单颗粒分析时间分别为30s(a)、12s(b)、6s(c)和3s(d)条件下的信号特征。信号强度以对数坐标呈现,不同颜色的线条分别表示不同同位素的信号强度(据文献[26])

    Figure 2. 

    图 3  线性拟合(a、b、c)和指数函数拟合(d)的激光诱导元素分馏校正方法(据文献[37])

    Figure 3. 

    图 4  (a) 采用LRC法计算206Pb/238U的比值;(b)206Pb和238U的“峰形”信号图(据文献[31])

    Figure 4. 

    图 5  (a) Wetherill谐和图示意图,误差椭圆三个方向分别表示三组比值的误差;(b)T-W谐和图示意图

    Figure 5. 

    图 6  两个不谐和度对数比值距离的定义:da表示数据点到谐和线的垂直Aitchison距离;dc表示数据点与计算的谐和年龄(tc)之间的Aitchison距离(据文献[60])

    Figure 6. 

    表 1  不谐和度计算方法及特点

    Table 1.  Different definitions of discordance and their characteristics

    参数 计算方法 表示公式 特点
    dr[61] 相对年龄差异 dr=1- t68/ t76 滤除年轻的年龄组分
    dt[57] 绝对年龄差异 dt =t76- t68 滤除年老的年龄组分
    dp[55] U-Pb比值 dp=Prob(sS~χ22) 影响准确度和精度
    dsk[62] 地幔演化模型 $d_{\mathrm{sk}}=1-\left[\frac{{ }^{238} \mathrm{U}}{{ }^{206} \mathrm{~Pb}}\right] /\left[\frac{{ }^{238} \mathrm{U}}{{ }^{206} \mathrm{~Pb}}\right]^*$ 滤除年老组分
    da[60] Aitchison距离 $d_{\mathrm{a}}=\mathrm{d} x\left(t_{68}\right) \sin \left[\arctan \frac{\mathrm{d} y\left(t_{76}\right)}{\mathrm{d} x\left(t_{68}\right)}\right]$ 滤除1000~2000Ma的锆石颗粒
    dc[60] Aitchison谐和距离 $d_{\mathrm{c}}=\operatorname{sgn}\left(t_{76}-t_{68}\right) \sqrt{\mathrm{d} x\left(t_{\mathrm{c}}\right)^2+\mathrm{d} y\left(t_{\mathrm{e}}\right)^2}$ 最合理
    DMS[63] 年龄差异绝对值的较小值 $D_{\mathrm{MS}}=\left\{\left|t_{68}-t_{75}\right|, \left|t_{76}-t_{75}\right|\right\}$ 滤除较老的年龄组分
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出版历程
收稿日期:  2021-12-26
修回日期:  2022-07-14
录用日期:  2022-08-18
刊出日期:  2022-11-28

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