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碳酸锌矿物菱锌矿的红外和红外发射光谱。

Infrared and infrared emission spectroscopy of the zinc carbonate mineral smithsonite.

作者信息

Frost Ray L, Martens Wayde N, Wain Daria L, Hales Matt C

机构信息

Inorganic Materials Research Program, School of Physical and Chemical Sciences, Queensland University of Technology, GPO Box 2434, Brisbane, Queensland 4001, Australia.

出版信息

Spectrochim Acta A Mol Biomol Spectrosc. 2008 Oct;70(5):1120-6. doi: 10.1016/j.saa.2007.10.027. Epub 2007 Oct 30.

Abstract

Infrared emission and infrared spectroscopy has been used to study a series of selected natural smithsonites from different origins. An intense broad infrared band at 1440 cm(-1) is assigned to the nu3 CO3(2-) antisymmetric stretching vibration. An additional band is resolved at 1335 cm(-1). An intense sharp Raman band at 1092 cm(-1) is assigned to the CO3(2-) symmetric stretching vibration. Infrared emission spectra show a broad antisymmetric band at 1442 cm(-1) shifting to lower wavenumbers with thermal treatment. A band observed at 870 cm(-1) with a band of lesser intensity at 842 cm(-1) shifts to higher wavenumbers upon thermal treatment and is observed at 865 cm(-1) at 400 degrees C and is assigned to the CO3(2-)nu2 mode. No nu2 bending modes are observed in the Raman spectra for smithsonite. The band at 746 cm(-1) shifts to 743 cm(-1) at 400 degrees C and is attributed to the CO3(2-)nu4 in phase bending modes. Two infrared bands at 744 and around 729 cm(-1) are assigned to the nu4 in phase bending mode. Multiple bands may be attributed to the structural distortion ZnO6 octahedron. This structural distortion is brought about by the substitution of Zn by some other cation. A number of bands at 2499, 2597, 2858, 2954 and 2991 cm(-1) in both the IE and infrared spectra are attributed to combination bands.

摘要

红外发射和红外光谱已被用于研究一系列来自不同产地的精选菱锌矿。在1440 cm⁻¹处的一个强烈宽红外带被归因于ν3 CO₃²⁻反对称伸缩振动。在1335 cm⁻¹处分辨出一个附加带。在1092 cm⁻¹处的一个强烈尖锐拉曼带被归因于CO₃²⁻对称伸缩振动。红外发射光谱显示在1442 cm⁻¹处有一个宽反对称带,随着热处理向较低波数移动。在870 cm⁻¹处观察到的一个带以及在842 cm⁻¹处强度较小的一个带在热处理后向较高波数移动,在400℃时在865 cm⁻¹处被观察到,并被归因于CO₃²⁻ν2模式。在菱锌矿的拉曼光谱中未观察到ν2弯曲模式。在746 cm⁻¹处的带在400℃时移至743 cm⁻¹,并归因于CO₃²⁻ν4同相弯曲模式。在744 cm⁻¹和729 cm⁻¹左右的两个红外带被归因于ν4同相弯曲模式。多个带可能归因于结构畸变的ZnO6八面体。这种结构畸变是由一些其他阳离子取代Zn引起的。在红外发射光谱和红外光谱中,在2499、2597、2858、2954和2991 cm⁻¹处的一些带归因于组合带。

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