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古巴莫阿-巴拉科阿蛇绿岩地块中铬铁矿的光谱特征分析。

Spectroscopic characterization of chromite from the Moa-Baracoa Ophiolitic Massif, Cuba.

作者信息

Reddy B Jagannadha, Frost Ray L

机构信息

Inorganic Materials Research Program, Queensland University of Technology, 2 George Street, Brisbane, GPO Box 2434, Queensland 4001, Australia.

出版信息

Spectrochim Acta A Mol Biomol Spectrosc. 2005 Jun;61(8):1721-8. doi: 10.1016/j.saa.2004.07.002.

Abstract

The Cuban chromites with a spinel structure, FeCr2O4 have been studied using optical absorption and EPR spectroscopy. The spectral features in the electronic spectra are used to map the octahedral and tetrahedral co-ordinated cations. Bands due Cr3+ and Fe3+ ions could be distinguished from UV-vis spectrum. Chromite spectrum shows two spin allowed bands at 17,390 and 23,810 cm(-1) due to Cr3+ in octahedral field and they are assigned to 4A2g(F) --> 4T2g(F) and 4A2g(F) --> 4T1g(F) transitions. This is in conformity with the broad resonance of Cr3+ observed from EPR spectrum at g = 1.903 and a weak signal at g = 3.861 confirms Fe3+ impurity in the mineral. Bands of Fe3+ ion in the optical spectrum at 13,700, 18,870 and 28,570 cm(-1) are attributed to 6A1g(S) --> 4T1g(G), 6A1g(S) --> 4T2g(G) and 6A1g(S) --> 4T2g(P) transitions, respectively. Near-IR reflectance spectroscopy has been used effectively to show intense absorption bands caused by electronic spin allowed d-d transitions of Fe2+ in tetrahedral symmetry, in the region 5000-4000 cm(-1). The high frequency region (7500-6500 cm(-1)) is attributed to the overtones of hydroxyl stretching modes. Correlation between Raman spectral features and mineral chemistry are used to interpret the Raman data. The Raman spectrum of chromite shows three bands in the CrO stretching region at 730, 560 and 445 cm(-1). The most intense peak at 730 cm(-1) is identified as symmetric stretching vibrational mode, A1g(nu1) and the other two minor peaks at 560 and 445 cm(-1) are assigned to F2g(nu4) and E(g)(nu2) modes, respectively. Cation substitution in chromite results various changes both in Raman and IR spectra. In the low-wavenumber region of Raman spectrum a significant band at 250 cm(-1) with a component at 218 cm(-1) is attributed F2g(nu3) mode. The minor peaks at 195, 175, 160 cm(-1) might be due to E(g) and F2g symmetries. Broadening of the peak of A1g mode and shifting of the peak to higher wavenumber observed as a result of increasing the proportion of Al3+O6. The presence of water in the mineral shows bands in the IR spectrum at 3550, 3425, 3295, 1630 and 1455 cm(-1). The vibrational spectrum of chromite gives raise to four frequencies at 985, 770, 710 and 650 cm(-1). The first two frequencies nu1 and nu2 are related to the lattice vibrations of octahedral groups. Due to the influence of tetrahedral bivalent cation, vibrational interactions occur between nu3 and nu4 and hence the low frequency bands, nu3 and nu4 correspond to complex vibrations involving both octahedral and tetrahedral cations simultaneously. Cr3+ in Cuban natural chromites has highest CFSE (20,868 cm(-1)) when compared to other oxide minerals.

摘要

利用光吸收和电子顺磁共振光谱对具有尖晶石结构的古巴铬铁矿FeCr₂O₄进行了研究。电子光谱中的光谱特征用于绘制八面体和四面体配位阳离子的分布图。在紫外-可见光谱中可以区分出由Cr³⁺和Fe³⁺离子引起的谱带。铬铁矿光谱在17390和23810 cm⁻¹处显示出两个自旋允许带,这是由于八面体场中的Cr³⁺引起的,它们分别对应于⁴A₂g(F)→⁴T₂g(F)和⁴A₂g(F)→⁴T₁g(F)跃迁。这与从电子顺磁共振光谱在g = 1.903处观察到的Cr³⁺的宽共振以及在g = 3.861处的弱信号相一致,证实了矿物中存在Fe³⁺杂质。光谱中Fe³⁺离子在13700、18870和28570 cm⁻¹处的谱带分别归因于⁶A₁g(S)→⁴T₁g(G)、⁶A₁g(S)→⁴T₂g(G)和⁶A₁g(S)→⁴T₂g(P)跃迁。近红外反射光谱已被有效地用于显示在5000 - 4000 cm⁻¹区域内由四面体对称中Fe²⁺的电子自旋允许d-d跃迁引起的强吸收带。高频区域(7500 - 6500 cm⁻¹)归因于羟基伸缩振动模式的泛音。利用拉曼光谱特征与矿物化学之间的相关性来解释拉曼数据。铬铁矿的拉曼光谱在CrO伸缩区域的730、560和445 cm⁻¹处显示出三个谱带。730 cm⁻¹处最强的峰被确定为对称伸缩振动模式A₁g(ν₁),另外两个在560和445 cm⁻¹处的小峰分别归因于F₂g(ν₄)和E(g)(ν₂)模式。铬铁矿中的阳离子取代导致拉曼光谱和红外光谱都发生各种变化。在拉曼光谱的低波数区域,一个在250 cm⁻¹处有一个218 cm⁻¹分量的显著谱带归因于F₂g(ν₃)模式。195、175、160 cm⁻¹处的小峰可能归因于E(g)和F₂g对称性。随着Al³⁺O₆比例的增加,观察到A₁g模式的峰变宽并向更高波数移动。矿物中存在水在红外光谱中显示出在3550、3425、3295、1630和1455 cm⁻¹处的谱带。铬铁矿的振动光谱产生了985、770、710和650 cm⁻¹处的四个频率。前两个频率ν₁和ν₂与八面体基团的晶格振动有关。由于四面体二价阳离子的影响,在ν₃和ν₄之间发生振动相互作用,因此低频带ν₃和ν₄对应于同时涉及八面体和四面体阳离子的复杂振动。与其他氧化物矿物相比,古巴天然铬铁矿中的Cr³⁺具有最高的晶体场稳定能(20868 cm⁻¹)。

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