Abstract

Ten natural cordierite single crystals with XFe in the range 0.044–0.76 and 0.12 to 1.97 wt% CO2 were investigated with Raman microspectroscopy using three different wavelengths. Improved calibration diagrams for CO2 determinations in single crystals and thin sections for the 488, 515 and 633 nm laser excitation wavelengths show significantly lower standard deviations for CO2 determinations (±0.04 to 0.07 wt%) compared to an earlier study done solely at 633 nm. The diagrams are based on the linear relationship between CO2 in wt.% and the ratios of the Raman peak of CO2 to two Si-O-stretching vibrations. The consideration of orientation dependencies and the improvement of background corrections and spectra fitting procedures also contributed to the significantly higher precision. Because Fe-incorporation in cordierite leads to structural changes that result in Raman peak shifts and peak broadening, including peaks considered in this investigation, a correction was introduced for precise CO2 determination on Fe-bearing samples. This improved CO2 determination method was then applied on a 2D spatial scale to two cordierite grains in a thin section of a granulite-facies metapelite from Kösseldorf in the Sauwald area (southern Bohemian Massif, Upper Austria), which yielded CO2 contents of 0.27–0.31 ±0.07 wt%.

1. Introduction

Cordierite is a common mineral in medium- to high-grade metamorphic aluminous rocks and used as an important geothermobarometer, especially in rocks of the granulite facies where it is in equilibrium with other Fe-Mg-silicates (Lonker, 1981; Bhattacharya, 1986; Kalt et al., 1999; Kalt, 2000). Since cordierite has the ability to incorporate fluid molecules like H2O and CO2, it can also be used as a monitor of fluid composition during metamorphism (Carrington & Harley, 1996; Knop & Mirwald, 2000; Harley et al., 2002). The simultaneous incorporation of different fluid molecules allows an estimation of the amount of H2O and CO2 in the coexisting fluids or melts and hence calculation of their activities. This information can then be used for improved phase-diagram calculations. Different pressure (P) – temperature (T) conditions lead to significant variations in the partitioning of H2O and CO2 into cordierite (Harley, 1994; Stevens et al., 1995; Carrington & Harley, 1996; Harley & Carrington, 2001; Thompson et al., 2001; Harley et al., 2002). The dominant channel occupant in natural samples is H2O but, especially in granulite-facies rocks, CO2 and N2 may also become important volatile components (Armbruster, 1985). For instance Rigby et al. (2008) analysed 34 samples from the Etive thermal aureole, Scotland, using Fourier-transform infrared spectroscopy (FTIR) and the measured volatile contents were then used to calculate peak metamorphic H2O and CO2 activities.

Cordierite has also received considerable attention as an electronic packaging material, one of the key technologies to meet a variety of microelectronic applications, because of its low dielectric constant and thermal expansion coefficient (Tummala, 1991; Shannon et al., 1992). In order to obtain more accurate results on dielectric constants and the dielectric loss of cordierite, the contributions of channel H2O and CO2 must be taken into account (Shannon et al., 1992). The thermal expansion coefficient, dielectric constant and Young’s modulus of cordierite ceramics may also vary due to the substitution of part of the oxygen atoms by nitrogen (Unuma et al., 1993). As it will be seen in the next section, CO2 determination using micro-Raman spectroscopy has been done for quite a while (e.g., Kolesov & Geiger, 2000). After a review of the previous investigations, this paper presents new data for the improved CO2 determination.

2. Overview of Raman-based CO2 determination in cordierite

Confocal Raman micro-spectroscopy offers a good tool for quick and destruction-free determination of CO2 in cordierite (Kolesov & Geiger, 2000). The in situ method can be applied to single crystals and to grains within thin sections. This method is based on linear relationships between the CO2 content in wt% and the Raman intensity ratio of the CO2-stretching mode against two Si–O streching modes of the cordierite structure in a certain orientation (Kolesov & Geiger, 2000; Kaindl et al., 2006). The incorporation and orientation of CO2 molecules in the structural channels of cordierite were investigated using various methods including DTA and dehydration studies (Sugiura, 1959), X-ray and neutron diffraction (e.g., Cohen et al., 1977; Armbruster, 1985), IR spectroscopy (Farrell & Newnham, 1967; Goldman et al., 1977; Le Breton, 1989; Vry et al., 1990; Kalt, 2000), proton NMR spectroscopy (Carson et al., 1982), quasi-elastic neutron scattering (Winkler et al., 1994b), and quantum mechanical calculations (Winkler et al., 1994a). Most of the rod-shaped CO2-molecules within the channels are aligned perpendicular to the crystallographic c-axis (Farrell & Newnham, 1967); only a small part is aligned parallel to the c-axis (Farmer, 1974; Armbruster, 1985). Infrared spectroscopic studies confirm the position of the CO2-molecule parallel to the a-axis (Armbruster & Bloss, 1982; Armbruster & Bürgi, 1982; Aines & Rossman, 1984; Khomenko & Langer, 2005). According to the Raman- and IR-spectroscopic examinations of Kolesov & Geiger (2000) at least 90% of the CO2-molecules are aligned parallel to the a-axis, less than 10% parallel to b. The position parallel to the a-axis is energetically favoured, because the diameter of the channels is bigger in direction of the a-axis than in direction of the b-axis (Hochella et al., 1979).

To gain the maximum intensity of the Raman-active, symmetric 2ν2 vibrational mode of CO2 at 1383 cm −1, the Raman spectra have to be recorded in aa-geometry (abbreviated Porto notation, where the first symbol gives the polarization direction of the incident light and the second one the polarization direction of the scattered light, Damen et al., 1966; Nasdala et al., 2004). The vector component of the electric field of the incident laser beam must be parallel to the grains a-axis. Both the polarisation plane of the incident laser beam and the scattered Raman light are polarised parallel to a. Two symmetric stretching modes of the cordierite structure at 972 and 1182 cm−1 show similar angular dependency and maximum intensity in the aa-oriented Raman spectra. To avoid uncertainties in the measurement of absolute Raman mode intensities, the intensities of the CO2 stretching mode can be normalized to the lattice vibration modes. The two ratios obtained are approximately constant in the angular range between ±30° and may, therefore, be used for this analytical measurement (Kolesov & Geiger, 2000; Kaindl et al., 2006).

Kolesov & Geiger (2000) investigated ten cordierite samples with varying chemical compositions using polarized single-crystal Raman spectroscopy at room temperature and 5 K and polarized infrared spectroscopy at room temperature. They found a linear trend between the CO2-content in wt% and the intensity ratios of the Raman active CO2-stretching mode and the Si-O-stretching modes using the 514 and 488 nm lines of an Ar-laser for excitation. The CO2 contents of seven samples were determined previously by bulk measurements (Vry et al., 1990).

Kaindl et al. (2006) presented a method for in situ determination of CO2 content of natural cordierites in thin section using the 633 nm wavelength. Their investigation of nine synthetic and natural cordierite samples with different chemical compositions and CO2-contents led to an improvement of the calibration curve although, for samples with XCO2 <0.1, the calibration curve was slightly shifted away from the origin. The results agree with those of Kolesov & Geiger (2000) and show a smaller scattering. The Raman measurements were performed on oriented cordierite single crystals. Linear least squares regression of the data showed correlation coefficients R2 of 0.912 and 0.883 for equations intersecting the origin of the diagram. The estimated error of about ±0.11 wt% is very similar to the error of the CO2 determination by SIMS analysis (Harley et al., 2002).

A preliminary investigation was undertaken to expand applicability of the method to three different laser excitation wavelengths (Haefeker et al., 2006). Ten natural cordierite single crystals with different chemical compositions were used for the Raman measurements. Bulk CO2 contents, determined by coloumetric titration, varied from 0.12 to 1.97 wt% CO2.

This work presents new data for the improved CO2 determinations of cordierite in thin sections at three different laser excitation wavelengths (488, 515 and 633 nm). Sources of errors like orientation dependency, background correction and spectra fitting procedures have been thoroughly investigated, which leads to an increase in the precision of measurement and analysis. The influence of peak shifts and peak broadening due to Fe incorporation based on the investigation by Haefeker et al. (2012) has been corrected. In addition, 2D images of the spatial CO2 and Fe distribution within natural cordierites, generated by Raman mapping techniques, are presented.

3. Experimental setup and data evaluation

The natural single crystals of cordierite used in this study were collected by Charles A. Geiger, University Kiel, DFG project Nr. Ge 659/6-1. Their CO2 content was measured after thermal extraction by Bertoldi et al. (2004) using CO2 coulometric titration. Sample designations, localities, rock types, mineral parageneses, pressure-temperature conditions and chemistry are given in the appendix of Bertoldi et al. (2004). The CO2 content of the samples varies between 0.12 and 1.97 wt%, the molar ratio XFe = [Fe/(Fe + Mg + Mn + Zn)] is between 0.044 and 0.76. A description of the used synthetic cordierite samples can be found in Haefeker et al. (2012). The Raman spectra were recorded on a Labram HR-800 confocal Raman-spectrometer by HORIBA using a 100× objective with a numerical aperture of 0.9. The emission lines of a 17 mW He-Ne-laser at 633 nm and a 30 mW Ar-ion laser at 515 nm and 488 nm were used. The spectra were recorded in the range from 900 to 1400 cm−1. The confocal pinhole aperture was 1000 μm and the width of the entrance slit was 100 μm. Light was dispersed by a static grating with 1800 lines/mm. The scattered Raman light was detected by an open-electrode charge-coupled device with 1024 × 256 pixels, each with a size of 43 μm. The spectral resolution, determined by measuring the Rayleigh line was 0.9 to 2 cm−1. The system was calibrated with the 520 cm−1 line of a Si-wafer. Background and Raman peaks were fitted using the built-in spectrometer software LabSpec with the line-segments baseline correction and convoluted Gauss-Lorentz functions (pseudo-Voigt profile). The replacement of the Ar-ion laser with a 30 mW Nd-YAG laser made it necessary to switch to the 532 nm emission line to record recent Raman profiles and maps.

In order to achieve highest intensities of 2ν2(CO2) the a-axis of the crystals were oriented parallel to the electric field vector component of the incident laser. To facilitate orientation the untreated single crystals were fixed on a pin on a goniometer head. The details of the orientation procedure can be found in Kaindl et al. (2006). The selection of suitable cordierite grains in thin sections is also described there. The Raman spectra of a natural cordierite single crystal with a CO2 content of 1.74 wt.% in the spectral range 900–1400 cm−1 are shown in Fig. 1. In aa scattering geometry, the two components of the Fermi doublet of structurally bonded CO2 at 1383 and 1270 cm−1 [2ν2, ν1(CO2)] can clearly be distinguished (Kolesov & Geiger, 2000). The intensity ratio of the two components in the measured samples ranged between 2.56 and 3.03. In cordierites with very low CO2 contents ν1(CO2) intensity was very low. For this study we assumed constant intensity ratios and therefore only 2ν2(CO2) was taken into account for the determinations.

The two intense bands at 973 and 1183 and the weak band at 1009 cm−1 can be assigned to symmetric stretching vibrations of the SiO4 tetrahedra [ν1, ν3, ν2(SiO4)] (Kolesov & Geiger, 2000). Detailed band assignments based on quantum-mechanical calculations for both cordierite Fe- and Mg-end-members can be found in Kaindl et al. (2011). The band at 973 cm−11) is related to the stretching of the ring tetrahedra T21 and the T16 tetrahedron, which connects two M-sites. The peak at 1183 cm−13) is related to the T21 and T23 tetrahedra, which stretch in counter-tact. The peak at 1009 cm−12) is caused by the T21 and T23 tetrahedral vibration. A low intensity peak can be found at 950 cm−1, which is related with the T21 and the T16 site. In cc scattering geometry, the intensity of 2ν2(CO2) strongly decreases and the intensities of ν1(CO2) and ν3(SiO4) almost disappear. In order to reduce the analytical errors and to yield highest intensities of 2ν2(CO2), every grain was rotated into aa geometry before measurement. For example, the 2ν2(CO2) intensity of the polarized single-crystal Raman spectra of sample 129875, which contains 1.74 wt% CO2, was approximately 86% higher when measured in aa compared to cc scattering geometry (Fig. 1). Figure 1 also illustrates the spectroscopic approach to find the appropriate orientation: ν1(SiO4) can be detected in every scattering geometry [bb not displayed, cf. Figure 1 in Kolesov & Geiger (2000)] whereas the intensity of ν3(SiO4) trends to a maximum in aa. Subsequently, in perfect aa geometry the intensity ratio I ν1(SiO4)/I ν3(SiO4) must trend to a minimum. In contrast to the method presented in Kaindl et al. (2006), the minimum intensity ratio I ν1(SiO4)/I ν3(SiO4) in aa may lie in the range 0.68–0.9, since it also depends on the Fe-Mg ratio of the cordierite. Considering (1) the experimental setup (static grating, small wavenumber region) and (2) the presented equations based on intensity ratios only, a calibration of the instrument response function (e.g., Ray & McCreery, 1997) was not undertaken.

4. Results and discussion

4.1. Peak overlap and peak broadening as a result of Fe-incorporation

The incorporation of Fe2+ (up to XFe~0.8 in natural crystals) leads to multiple changes in the structure of cordierite (e.g., Wallace & Wenk, 1980; Armbruster, 1985; Boberski & Schreyer, 1990; Malcherek et al., 2001; Geiger & Grams, 2003). As a result most Raman peaks shift towards lower wavenumbers with increasing XFe. Exceptions are the low-intensity bands around 330, 909 and 950 cm−1 (Kaindl et al., 2011; Haefeker et al., 2012). In Fe-rich samples opposite peak shift directions lead to a peak overlap in the 970 cm−1 region. For precise determination of I ν1(SiO4) the band at 970 cm −1 has to be deconvoluted into two individual peaks. The deconvolution for samples with XFe = 0, 0.49 and 1 is given in Fig. 2a. In Mg-cordierite ν1(SiO4) can be found at 974 cm −1 and it shifts to 966 cm−1 in the Fe-end-member. A low-intensity peak in Mg-Cordierite at 952 cm−1 shows the opposite shift direction and can be found at 958 cm−1 in samples with XFe = 1. Figure 2b shows the Raman shift as a function of XFe for natural and synthetic cordierite samples. In addition the intensity (integrated peak area) of the peak 952/962 cm−1 increases as a function of XFe. In samples with no or low Fe contents the ratio I974/I952 is ~1/12, in the sample with XFe = 1 the ratio increases to ~1/4. As another result of increasing Fe contents a peak at 1157 cm−1 gains in intensity. This peak has to be considered for precise determinations of I ν3(SiO4) at 1180 cm −1.

The incorporation of Fe causes peak broadening of all peaks related to lattice vibrations. Geiger & Grams (2003) described this effect for the IR-spectra of natural cordierite. The CO2 peak at 1383 cm −1 is not affected by the Fe-Mg exchange. To quantify the effect of peak broadening of ν1(SiO4) at 974 cm −1, six synthetic cordierite samples with similar orientations and XFe = 0–1 were investigated. The full width at half maximum of the peaks increases as a function of XFe. To determine the intensity increase, six theoretical Gauss-Lorentz functions (pseudo-Voigt profile) with equal function parameters except FWHM were modelled (Fig. 3a). FWHM were taken from the experimentally derived values. This procedure showed that I ν1(SiO4) of cordierite with XFe = 1 is ~2.8 times higher than I ν1(SiO4) of cordierite with XFe = 0. Based upon this model, correction factors for I ν1(SiO4) at six different XFe were calculated (Fig. 3b). Linear interpolation can be applied for compositions between two data points. These correction factors were also applied to I ν3(SiO4). The XFe value can be estimated by the shifts of selected Raman peaks (Haefeker et al., 2012) or, when available, chemical data from electron microprobe analysis can be used.

4.2. The influence of background correction and peak fitting

For the precise determination of the integrated peak areas (I 2ν2(CO2), I ν1(SiO4) and I ν3(SiO4)) the recorded spectra have to be corrected for their background. When an automatic software-based baseline determination and correction function is used, a revision is recommended to manually correct or subtract misplaced background points, especially when the signal-to-noise ratio of the spectra is low. In some cases additional background points are needed for proper background definition. Erroneously or over-corrected spectra can result in a reduction or increase of the integrated peak area and thus wrong intensity ratios. In addition, wrong background correction can cause peak distortions, influencing both peak-fit quality and intensities.

In Fe-rich samples two peaks between 950 and 970 cm−1 overlap. In samples with XFe > 0.5 the de-convolution of the band into two single peaks is error-prone and can lead to erroneous I ν1(SiO4) peak intensities. Therefore, as starting parameters for the fit functions the position 956 should be fixed and for 965 cm−1 a FWHM of 15 cm−1 should be given and variability restricted to ±5 cm−1. Examples of peak fitting and related sources of errors are given e.g. in Bradley (2007) and Knorr (2011).

4.3. Calibration diagrams

The intensity ratios I1 = 2ν2(CO2)/I ν1(SiO4) and I2 = 2ν2(CO2)/I ν3(SiO4) for three different laser excitation wavelengths are shown in Fig. 4–6. Least square regressions yielded very good linear correlations between both intensity ratios and CO2 contents (wt%) as indicated by high correlation coefficients (R2 > 0.98). One sample shows larger deviations (sample TA-1), which is most likely due to smaller CO2 contents than the bulk composition determined by Bertoldi et al. (2004). The standard errors of prediction of CO2 concentrations by using the regression equations range between ±0.04 to 0.07 wt%, which is a significant reduction compared to the error of ±0.11 wt% given by Kaindl et al. (2006). The correlation coefficients R2 for all equations are between 0.986 and 0.995, the standard errors of prediction for the CO2 concentrations were calculated with the equation:

 

σc1,c2=1n-2[(c1,2¯-c1,2)2-[(I1,2¯-I1,2)(c1,2¯-c1,2)]2(I1,2¯-I1,2)2]

where n is the number of observations, c1,2¯ the mean CO2 concentration determined by intensity ratios I1,2, and I1,2¯ the mean intensity ratios.

The regression equations may be used for the determination of the CO2 content of unknown cordierite samples.

  1. 488 nm

    • c1(wt%) ± 0.048 = 1.6874 · I1

    • c2 (wt%) ± 0.04 = 2.3071 · I2

  2. 514 nm

    • c1(wt%) ± 0.047 = 1.6875 · I1

    • c2 (wt%) ± 0.072 = 2.2748 · I2

  3. 633 nm

    • c1(wt%) ± 0.043 = 1.5579 · I1

    • c2(wt%) ± 0.054 = 2.4374 · I2

4.4. Application to natural cordierites in thin sections

A granulite-facies metapelite from Kösseldorf in the Sauwald area (southern Bohemian Massif, Upper Austria), containing the assemblage garnet + spinel + cordierite + sillimanite + biotite + plagioclase + K-feldspar + quartz (Tropper et al., 2006), was used for the measurements. Within an uncovered, polished thin section two cordierite porphyroblasts in suitable aa-scattering geometry were found and selected for the CO2 determinations. The XFe determinations were done with the calibration diagrams presented by Haefeker et al. (2012). Along a line profile across a grain, 27 measurement points over a distance of 60 μm were recorded and the CO2 contents calculated by inserting into Equation (2b) and a correction factor of 1.4 for XFe ~ 0.5 (Fig. 3b and 7a, b). The CO2 distribution is homogeneous with CO2 contents in the range of 0.27–0.31 (±0.07) wt%. The Raman signal of point 2 on the grain boundary was very weak, resulting in a higher error of the CO2 content determination. The points 1 and 27 belong to the neighbouring grains (plagioclase, quartz); therefore the CO2 content was set to zero.

A hyperspectral Raman image (112 × 263 μm, 50 × 50 data points) of a second porphyroblast also shows the 2D homogeneous distribution of CO2 and constant XFe within the grain (Fig. 8a–c). Figure 8b displays XFe in grey-scales, Fig. 8c displays the CO2 contents in grey-scales, calculated by Equation (2b) and a correction factor of 1.4 for XFe ~ 0.5. Deviations from a homogeneous CO2 content of 0.28 ± 0.07 wt% throughout the grain are caused by errors in automatic background correction and determination of the integrated peak areas as well as inclusions (black and white spots in Fig. 8c).

5. Conclusions

The presented correlation diagrams allow fast and non-destructive determinations of CO2 at standard errors of prediction from ±0.04 to 0.07 wt%. A linear correlation between CO2 contents in wt% and the intensity ratios of the CO2 mode at 1383 cm−1 and the two lattice vibration modes at 972 cm−1 and 1185 cm−1 was found. The diagrams in Kaindl et al. (2006) did not take into account peak broadening in Fe-bearing samples (Haefeker et al., 2012), which could lead to erroneous results for samples with low CO2 contents. Hence a correction for the influence of Fe-incorporation on selected Raman peaks was introduced. Additionally the influence of two peaks at 955 and 1157 cm−1 in Fe-rich samples have been considered. It could be confirmed by our investigations that most of the CO2 in the channel cavities is preferentially aligned parallel to the a-axis.

Acknowledgements

We thank Martina Tribus for her help with the electron microprobe analysis, Jürgen Konzett for his help with the experiments and Daniel Többens for his help with X-ray powder analysis. Financial support of the Austrian Science Fund (FWF): [P22013-N21 to R.K.] is gratefully acknowledged.

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