使用显微拉曼光谱法识别具有不同成分和结晶取向的主要蛇纹石锑岗石、蜥蜴石和温石棉

IF 2 4区 地球科学 Q3 GEOSCIENCES, MULTIDISCIPLINARY
Xi Liu , Yunlu Ma , Wei Yan , Mingyue He , Lamei Li , Xinhao Sui , Bijie Peng
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引用次数: 0

摘要

蛇纹石是地质学上的重要矿物,其中的三个主要品种是蚁石(Atg)、蜥蜴石(Lz)和温石棉(Ctl)。使用显微拉曼光谱快速准确地识别它们需要考虑不同晶体学取向和不同化学成分的影响。我们从现有文献中收集了从相同或完全相同的 Atg、Lz 和 Ctl 样品中获得的所有拉曼光谱数据和成分数据,首次对成分影响进行了批判性研究,发现 Al2O3 和 Cr2O3 含量等成分参数对拉曼特征有显著影响。考虑到成分差异和晶体取向差异的影响,我们对 Atg、Lz 和 Ctl 提出了两种识别方案:第一种方案使用 1200-1000 cm-1 处微弱但有特征的拉曼峰,第二种方案使用 688、378 和 229 cm-1 处强烈且一致观察到的拉曼峰。在第一种鉴别方案中,1200-1000 cm-1 处没有拉曼峰表明存在 Lz;1045、1070 或 1106 cm-1 处的单峰分别表明存在 Atg、Lz 或 Ctl;1040 和 1070 cm-1 处的两个拉曼峰表明存在 Lz;偶尔在 ∼1040 cm-1 处观察到的一个单峰可能意味着 Atg 或 Lz 的存在,可通过峰位比 R ∼1045/688 来确定(Atg 的 R ∼1045/688 > ∼1.521,而 Lz 达到 R∼1045/688 < ∼1.521)。在第二种鉴别方案中,利用拉曼峰在∼688 和 ∼378 cm-1 处的精确波长,可以很容易地将 Atg 与 Lz 和 Ctl 区分开来;利用拉曼峰在∼378 和 ∼229 cm-1 处的精确波长,可以进一步将 Lz 和 Ctl 区分开来。在大多数情况下,这两种鉴别方法都不需要晶体取向或成分信息,可以方便地用于鉴别 Atg、Lz 和 Ctl 的蛇纹石。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Identify key serpentines antigorite, lizardite and chrysotile with various compositions and crystallographic orientations using micro-Raman spectroscopy

Serpentines are geologically important minerals, and antigorite (Atg), lizardite (Lz) and chrysotile (Ctl) are the three key varieties. Their quick and accurate identification with micro-Raman spectroscopy requires to consider the effects of different crystallographic orientations and different chemical compositions. By collecting from existing literatures all Raman spectroscopic data and compositional data acquired from the same or identical Atg, Lz and Ctl samples, we critically examined the compositional effects for the first time, and found that some compositional parameters like the Al2O3 and Cr2O3 contents have significant impacts on the Raman features. Taking into account the effects of both compositional difference and crystallographic orientation difference, we propose two identification schemes for Atg, Lz and Ctl: the first one uses those weak but characteristic Raman peaks at 1200–1000 cm−1, and the second one uses those intense and unanimously-observed Raman peaks at ∼688, 378 and 229 cm−1. As for the first identification scheme, no peak at 1200–1000 cm−1 suggests the presence of Lz; a single peak at ∼1045, at ∼1070, or at ∼1106 cm−1 indicates the presence of Atg, Lz, or Ctl, respectively; two Raman peaks at ∼1040 and 1070 cm−1 implies the presence of Lz; the occasionally observed one single peak at ∼1040 cm−1 may imply the presence of either Atg or Lz, which can be sought out by resorting to the peak position ratio R∼1045/688 (Atg having R∼1045/688 > ∼1.521 whereas Lz attaining R∼1045/688 < ∼1.521). As for the second identification scheme, Atg can be readily separated from Lz and Ctl by using the exact wavenumbers of the Raman peaks at ∼688 and ∼378 cm−1, and Lz and Ctl can be further discriminated by using the exact wavenumbers of the Raman peaks at ∼378 and ∼229 cm−1. Under most circumstances, both identification schemes do not require the information of crystallographic orientation or composition, and can be conveniently applied to identify the serpentines of Atg, Lz and Ctl.

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来源期刊
Solid Earth Sciences
Solid Earth Sciences GEOSCIENCES, MULTIDISCIPLINARY-
CiteScore
3.60
自引率
5.00%
发文量
20
审稿时长
103 days
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