4.2 Article

Crystallographic orientation mapping of lizardite serpentinite by Raman spectroscopy

Journal

EUROPEAN JOURNAL OF MINERALOGY
Volume 34, Issue 3, Pages 285-300

Publisher

COPERNICUS GESELLSCHAFT MBH
DOI: 10.5194/ejm-34-285-2022

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Funding

  1. Marsden Fund Council [UOO1829]
  2. DoddWalls Centre for Photonic and Quantum Technologies
  3. New Zealand Ministry for Business and Innovation Endeavour funding grant [C11X2001]
  4. New Zealand Ministry of Business, Innovation & Employment (MBIE) [C11X2001] Funding Source: New Zealand Ministry of Business, Innovation & Employment (MBIE)

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The study found that the serpentine mineral lizardite has strong Raman anisotropy in the OH-stretching region, and the wavenumber shifts depend on the orientation of the excitation laser relative to the crystallographic axes. By studying well-characterised lizardite samples, the relationship between crystallographic orientation and Raman wavenumber was quantified, providing a simple and cost-effective technique for measuring and quantifying lizardite-bearing serpentinite fault rocks. This technique is particularly useful when EBSD alone is insufficient.
The serpentine mineral lizardite displays strong Raman anisotropy in the OH-stretching region, resulting in significant wavenumber shifts (up to ca. 14.5 cm(-1)) that depend on the orientation of the impinging excitation laser relative to the crystallographic axes. We quantified the relationship between crystallographic orientation and Raman wavenumber using well-characterised samples of Monte Fico lizardite by applying Raman spectroscopy and electron backscatter diffraction (EBSD) mapping on thin sections of polycrystalline samples and grain mounts of selected single crystals, as well as by a spindle stage Raman study of an oriented cylinder drilled from a single crystal. We demonstrate that the main band in the OH-stretching region undergoes a systematic shift that depends on the inclination of the c-axis of the lizardite crystal. The data are used to derive an empirical relationship between the position of this main band and the c-axis inclination of a measured lizardite crystal: y = 14.5cos(4) (0.013x + 0.02) + (3670 +/- 1), where y is the inclination of the c-axis with respect to the normal vector (in degrees), and x is the main band position (wavenumber in cm(-1)) in the OH-stretching region. This new method provides a simple and cost-effective technique for measuring and quantifying the crystallographic orientation of lizardite-bearing serpentinite fault rocks, which can be difficult to achieve using EBSD alone. In addition to the samples used to determine the above empirical relationship, we demonstrate the applicability of the technique by mapping the orientations of lizardite in a more complex sample of deformed serpentinite from Elba Island, Italy.

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