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Journal of Petrology Volume 42 Number 4 Pages 847-851 2001
© Oxford University Press 2001
Comment on Mexican Peridotite Xenoliths and Tectonic Terranes: Correlations among Vent Location, Texture, Temperature, Pressure, and Oxygen Fugacity by J. F. Luhr & J. J. Aranda-Gomez (1997)
MINERALOGISCHES INSTITUT DER UNIVERSITÄT, INF 236, D-69120 HEIDELBERG, GERMANY
Received August 1, 1999; Revised typescript accepted June 26, 2000
| ABSTRACT |
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This comment addresses the interpretation of oxygen fugacity data for spinel peridotite xenoliths from five Mexican volcanic fields presented by Luhr & Aranda-Gomez (Journal of Petrology, 38, 10751112, 1997). The postulated eastwest increase of the
FMQ (relative oxygen fugacity, where FMQ is fayalitemagnetitequartz) values is inherent to the method and therefore of questionable geological significance. Increases in
FMQ do not necessarily mirror oxidation processes in the mantle controlled by subduction-related fluids. KEY WORDS: mantle metasomatism; Mexico; peridotite xenoliths; relative oxygen fugacity
| INTRODUCTION |
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Luhr & Aranda-Gomez (1997)
FMQ values of all xenoliths from the five volcanic fields, the authors described a systematic increase from east to west, which they interpreted as a consequence of subduction-related oxidation of the Mexican lithospheric mantle, perhaps a result of eastward descent of the Farallon Plate beneath the Mesozoic and Tertiary. In this discussion I show that the eastwest increase of
FMQ values is inherent to the method, and therefore of questionable geological significance. Variations in
FMQ among xenoliths do not necessarily mirror oxidation or reduction processes in the mantle, and subduction-related fluids need not increase
FMQ. The paper of Luhr & Aranda-Gomez (1997)
SOME REMINDERS ABOUT FMQ
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The olivineorthopyroxenespinel oxygen barometer that Luhr & Aranda-Gomez (1997)
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Oxygen fugacity can be calculated using the equation
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H°T,FFsM and
S°T,FFsM are the enthalpy and entropy differences of the FFsM reaction at P° = 1 bar and temperature T, and
VT,FFsM refers to the volume difference of the solids at this temperature. In practice, several equations, based on theoretical models and on experimental results, are substituted. Two of these, the versions of Wood et al. (1990)
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Because the strong temperature dependence of log fO2 is similar for most oxygen buffer equilibria, it can be successfully minimized by normalizing to the fayalitemagnetitequartz (FMQ) equilibrium, to yield the so-called relative oxygen fugacity or
FMQ values (e.g. Ohmoto & Kerrick, 1977
; Frost et al., 1988
), defined in the case of the FFsM equilibrium as
FMQFFsM = log fO2(FFsM) log fO2(FMQ).
DIFFERENT ESTIMATES OF FMQFFsM
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Luhr & Aranda-Gomez (1997)
FMQFFsM values calculated using the method of Ballhaus et al. (1991)
FMQFFsM (Fig. 1a). The mean difference is
0·8 log units, but at low fO2 the estimates can be as much as 2·2 log units apart (Fig. 1b). Consequently, the
FMQFFsM values calculated following Ballhaus et al. (1991)
Fe ratio in spinel decreases (Fig. 1b). This is related to the fact that the Fe3+ contents in spinel are estimated differently for the two fO2 calculation methods. Ballhaus et al. (1991)
Fe ratio in spinel assuming stoichiometry. In contrast, the estimates with the Wood et al. (1990)
Fe [see table 6 of Luhr & Aranda-Gomez (1997)
Fe values, especially with Fe3+-poor spinels. This is critical because it has been shown (Parkinson & Arculus, 1999
FMQFFsM (up to ±2 log units).
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Consequently, the differences between the
FMQFFsM values registered in the different volcanic fields may not be as significant as suggested by Luhr & Aranda-Gomez (1997)
THE PRESSURE DEPENDENCE OF FMQFFsM
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Although the use of FMQ-normalized log fO2 values for the FFsM dampens the temperature effect, it does not compensate for pressure dependence, because
VFFsM is about half of
VFMQ [equation (2); Fig. 2a]. Thus
FMQFFsM decreases by
0·4 log unit per 1 GPa. It would be better to normalize to the nickelbunsenite equilibrium (
NNOFFsM), because in contrast to
FMQFFsM,
NNOFFsM displays a negligible pressure dependence (Fig. 2a).
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In the literature, the pressure dependence of
FMQFFsM is typically dismissed in view of the restricted pressure range of the spinel-lherzolite facies (e.g. Wood et al., 1990
FMQFFsM values are calculated with a fixed pressure (typically 1·5 GPa; e.g. Wood et al., 1990
The dataset of Luhr & Aranda-Gomez (1997)
provides a good opportunity to test the pressure dependence of
FMQFFsM, because it includes pressure estimates (after Köhler & Brey, 1990
) of spinel peridotites that apparently represent widely different depths of the lithosphere. The
FMQFFsM values of the Mexican xenoliths obtained with the method of Wood et al. (1990)
display a slight inverse correlation with pressure (Fig. 2b), which is not seen for corresponding
NNOFFsM values (Fig. 2c). The strongest pressure effects are shown by the low-pressure xenoliths from the San Quintin field.
The pressure dependence of
FMQFFsM is responsible for the slight westward increase of the mean values of
FMQFFsM retrieved with the Wood et al. (1990)
method for the four western Mexican volcanic fields (SQ, MC, DGO, VES; Fig. 3a) because this increase is not reproduced using
NNOFFsM values (Fig. 3b). Using the log fO2 estimates of Ballhaus et al. (1991)
, neither the mean
FMQFFsM values nor the mean
NNOFFsM values vary systematically among these volcanic fields (Fig. 3c and d). Only the mean value of relative oxygen fugacity for the easternmost Santo Domingo field (SD) is lower than the other three, a feature that is independent of the estimation and normalization methods. However, the small number of samples and the large uncertainties of low oxygen fugacity values retrieved using spinels of very low Fe3+ contents suggest caution in interpreting the results for the Santo Domingo field. In conclusion, the data of Luhr & Aranda-Gomez (1997)
do not sustain the systematic increase of the relative oxygen fugacity from east to west that they proposed.
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Given the large uncertainties in pressure estimates for spinel lherzolites, which show an average 1
of ±4·5 kbar with the Ca-exchange olivineclinopyroxene geobarometer of Köhler & Brey (1990)| THE SIGNIFICANCE OF RELATIVE OXYGEN FUGACITY VALUES REGARDING THE OXIDATION STATE OF THE MANTLE |
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Luhr & Aranda-Gomez (1997)
FMQFFsM that they calculated to reflect oxidation related to subduction. However, there is no reason to expect a clear correlation between
FMQFFsM and the oxidation state of peridotites. The oxygen fugacity (an intensive variable) quantifies the partitioning of Fe3+ and Fe2+ between coexisting mineral phases [equation (2)] and has no direct relation to the bulk Fe3+/
Fe (an extensive variable). Canil et al. (1994)
Luhr & Aranda-Gomez (1997)
also wonder, as have others (e.g. Ionov & Wood, 1992
; Brandon & Draper, 1996
), why there is no inverse correlation between indicators of the refractory nature and
FMQFFsM, although residual peridotites should have lost most of their Fe3+ to the melt they produced. To explain this, they invoke an overprint though oxidizing, subduction-related fluids, as has already been proposed by Wood & Virgo (1989)
, Ionov & Wood (1992)
or Brandon & Draper (1996)
for other mantle regions.
An oxidizing metasomatic overprint should increase whole-rock Fe3+/
Fe. However, all available reliable (Mössbauer based) values from metasomatized xenoliths (five samples; Canil et al., 1994
; Brandon & Draper, 1996
) fall within the normal range for spinel peridotite and garnet peridotite. In contrast, the analyses of small slices of a composite xenolith that contains the remnant of a magmatic dyke reveal high Fe3+/
Fe values that increase towards the dyke, but only moderately high
FMQFFsM values, which do not increase with whole-rock Fe3+/
Fe (McGuire et al., 1991
). The Fe3+/
Fe ratios of spinel, orthopyroxene and olivine, although greater than in comparable unmetasomatized peridotites, do not change with distance from the fluid source. Instead, the increase of whole-rock Fe3+/
Fe towards the dyke reflects the increasing modal abundance of metasomatic, Fe3+-rich amphibole (McGuire et al., 1991
).
The detailed study of McGuire et al. (1991)
demonstrates how complex the redox effect of metasomatism is, and how little is known about it. Because
FMQFFsM values alone do not necessarily give a clue to metasomatic effects, it is not surprising that opinions diverge concerning the typical values for metasomatized mantle xenoliths. Some researchers observe that modally metasomatized xenoliths plot at the high
FMQFFsM end of the sample distributions (e.g. Mattioli et al., 1989
; Wood & Virgo, 1989
; Bryndzia & Wood, 1990
; Ballhaus et al., 1991
; Woodland et al., 1992
), yet others see the opposite relationship (e.g. Chen et al., 1991
) or find no correlation beween metasomatism and relative oxygen fugacity (Ionov & Wood, 1992
).
In conclusion, Luhr & Aranda-Gomez (1997)
present no convincing evidence that the
FMQFFsM variations in their xenolith samples are related to the interaction with oxidizing fluids.
| ACKNOWLEDGEMENTS |
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I am grateful to Eduard Woermann for clarifying discussions on oxygen fugacity some years ago in Aachen. Discussions and comments by Axel Brunsmann, Gerhard Franz, Enno Zinngrebe (Berlin) and Bernard Evans (Seattle) were much appreciated. The manuscript benefited greatly from constructive reviews by Mike Toplis (Nancy), Laurence Warr (Heidelberg) and two anonymous reviewers, and from the recommendations and accurate editing of Sorena Sorensen (Washington, DC).
| FOOTNOTES |
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*Telephone: +49 (0) 6221-54-4810. Fax: +49 (0) 6221-54-4805. E-mail: dlattard{at}min.uni-heidelberg.de
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- or ß-quartz), and FFsM. The numbers plotted along the lines are the 
) and standard deviations (±1