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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)

DOMINIQUE LATTARD,*

MINERALOGISCHES INSTITUT DER UNIVERSITÄT, INF 236, D-69120 HEIDELBERG, GERMANY

Received August 1, 1999; Revised typescript accepted June 26, 2000


    ABSTRACT
 TOP
 ABSTRACT
 INTRODUCTION
 SOME REMINDERS ABOUT {Delta}FMQ
 DIFFERENT ESTIMATES OF...
 THE PRESSURE DEPENDENCE OF...
 THE SIGNIFICANCE OF RELATIVE...
 REFERENCES
 
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, 1075–1112, 1997). The postulated east–west increase of the {Delta}FMQ (‘relative oxygen fugacity’, where FMQ is fayalite–magnetite–quartz) values is inherent to the method and therefore of questionable geological significance. Increases in {Delta}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
 TOP
 ABSTRACT
 INTRODUCTION
 SOME REMINDERS ABOUT {Delta}FMQ
 DIFFERENT ESTIMATES OF...
 THE PRESSURE DEPENDENCE OF...
 THE SIGNIFICANCE OF RELATIVE...
 REFERENCES
 
Luhr & Aranda-Gomez (1997)Go presented a study of 26 spinel peridotite xenoliths from five Mexican volcanic fields, disposed in a 1700 km SE–NW profile across central Mexico that spans four tectonostratigraphic terranes of the region. This comment addresses the interpretation of the oxygen fugacity data of Luhr & Aranda-Gomez (1997)Go. In comparing the {Delta}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 east–west increase of {Delta}FMQ values is inherent to the method, and therefore of questionable geological significance. Variations in {Delta}FMQ among xenoliths do not necessarily mirror oxidation or reduction processes in the mantle, and subduction-related fluids need not increase {Delta}FMQ. The paper of Luhr & Aranda-Gomez (1997)Go is a good example of a tendency to overinterpret oxygen fugacity results for mantle xenoliths.


    SOME REMINDERS ABOUT {Delta}FMQ
 TOP
 ABSTRACT
 INTRODUCTION
 SOME REMINDERS ABOUT {Delta}FMQ
 DIFFERENT ESTIMATES OF...
 THE PRESSURE DEPENDENCE OF...
 THE SIGNIFICANCE OF RELATIVE...
 REFERENCES
 
The olivine–orthopyroxene–spinel oxygen barometer that Luhr & Aranda-Gomez (1997)Go used to estimate the oxygen fugacity of the Mexican xenoliths they studied is based on the fayalite–ferrosilite–magnetite (‘FFsM’) oxygen buffer equilibrium:

Oxygen fugacity can be calculated using the equation

in which {Delta}H°T,FFsM and {Delta}S°T,FFsM are the enthalpy and entropy differences of the FFsM reaction at P° = 1 bar and temperature T, and {Delta}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)Go and of Ballhaus et al. (1991)Go have been utilized by Luhr & Aranda-Gomez (1997)Go. The volume term [equation (2)], however, is identical in all formulations and generally simplified to

assuming zero thermal expansion and compressibility terms.

Because the strong temperature dependence of log fO2 is similar for most oxygen buffer equilibria, it can be successfully minimized by normalizing to the fayalite–magnetite–quartz (FMQ) equilibrium, to yield the so-called ‘relative oxygen fugacity’ or ‘{Delta}FMQ’ values (e.g. Ohmoto & Kerrick, 1977Go; Frost et al., 1988Go), defined in the case of the FFsM equilibrium as {Delta}FMQFFsM = log fO2(FFsM) –log fO2(FMQ).


    DIFFERENT ESTIMATES OF {Delta}FMQFFsM
 TOP
 ABSTRACT
 INTRODUCTION
 SOME REMINDERS ABOUT {Delta}FMQ
 DIFFERENT ESTIMATES OF...
 THE PRESSURE DEPENDENCE OF...
 THE SIGNIFICANCE OF RELATIVE...
 REFERENCES
 
Luhr & Aranda-Gomez (1997)Go noted that the {Delta}FMQFFsM values calculated using the method of Ballhaus et al. (1991)Go are systematically lower than those from the calibration of Wood et al. (1990)Go. In view of the good correlation between the two sets of values (Fig. 1a), the authors considered only those obtained from the Wood et al. (1990)Go method. However, the slope of the correlation line between the two datasets differs significantly from unity and the deviation between the two sets increases with decreasing {Delta}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 {Delta}FMQFFsM values calculated following Ballhaus et al. (1991)Go yield a much larger range (Fig. 1a) than those obtained with the Wood et al. (1990)Go method. The difference between the results of the two estimation methods increases as the Fe3+/{Sigma}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)Go recommended calculating the Fe3+/{Sigma}Fe ratio in spinel assuming stoichiometry. In contrast, the estimates with the Wood et al. (1990)Go method employed corrected Fe3+/{Sigma}Fe [see table 6 of Luhr & Aranda-Gomez (1997)Go], but not according to the usual method (Wood & Virgo, 1989Go). Luhr & Aranda-Gomez (1997)Go give only a vague description of their correction procedure and do not demonstrate that it yields improved values. In any case, there are large uncertainties on the resulting Fe3+/{Sigma}Fe values, especially with Fe3+-poor spinels. This is critical because it has been shown (Parkinson & Arculus, 1999Go) that even a small relative error of ±1·5% in the R2O3 contents of Fe3+-poor spinels propagates to a wide range in error of {Delta}FMQFFsM (up to ±2 log units).



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Fig. 1. (a) The {Delta}FMQFFsM values determined using Ballhaus et al. [1991Go; {Delta}FMQ(B)] compared with those of Wood et al. [1990Go; {Delta}FMQ(W)]. Despite a good correlation (R = 0·94) between the two datasets, the deviation increases with decreasing {Delta}FMQFFsM. (b) Inverse correlation of the differences between the two estimates and the Fe3+/{Sigma}Fe values in spinel (determined by stoichiometry). The estimates deviate most for spinels with low Fe3+ (symbols surrounded by a shaded curve). Abbreviations for volcanic fields: SQ, San Quintin; MC, Mesa Cacaxta; DGO, Durango; VES, Ventura–Espiritu Santo; SD, Santo Domingo.

 
Consequently, the differences between the {Delta}FMQFFsM values registered in the different volcanic fields may not be as significant as suggested by Luhr & Aranda-Gomez (1997)Go.


    THE PRESSURE DEPENDENCE OF {Delta}FMQFFsM
 TOP
 ABSTRACT
 INTRODUCTION
 SOME REMINDERS ABOUT {Delta}FMQ
 DIFFERENT ESTIMATES OF...
 THE PRESSURE DEPENDENCE OF...
 THE SIGNIFICANCE OF RELATIVE...
 REFERENCES
 
Although the use of FMQ-normalized log fO2 values for the FFsM dampens the temperature effect, it does not compensate for pressure dependence, because {Delta}VFFsM is about half of {Delta}VFMQ [equation (2); Fig. 2a]. Thus {Delta}FMQFFsM decreases by ~0·4 log unit per 1 GPa. It would be better to normalize to the nickel–bunsenite equilibrium ({Delta}NNOFFsM), because in contrast to {Delta}FMQFFsM, {Delta}NNOFFsM displays a negligible pressure dependence (Fig. 2a).



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Fig. 2. (a) Dependence of log fO2 upon pressure at T = 1000°C of four oxygen buffers: NNO (dashed lines), FMQ (with {alpha}- or ß-quartz), and FFsM. The numbers plotted along the lines are the {Delta}Vs of the respective buffer reactions. Molar volumes were assumed to be constant (values at 298·15 K; from Berman, 1988Go). fO2 calculated with the GE0-CALC software (Brown et al., 1988Go). (b) {Delta}FMQFFsM and (c) {Delta}NNOFFsM values for peridotite xenoliths from five Mexican volcanic fields, plotted as a function of pressure. The {Delta}FMQFFsM values were retrieved by Luhr & Aranda-Gomez (1997)Go using the method of Wood et al. (1990)Go; the {Delta}NNOFFsM data were calculated from log fO2(FFsM) based upon Wood et al. (1990)Go (see Luhr & Aranda-Gomez, 1997Go, table 10); log fO2(NNO) values were obtained from the equation of O’Neill (1987)Go.

 
In the literature, the pressure dependence of {Delta}FMQFFsM is typically dismissed in view of the restricted pressure range of the spinel-lherzolite facies (e.g. Wood et al., 1990Go; Woodland et al., 1992Go). Pressure estimates are not made because of their large uncertainties and the {Delta}FMQFFsM values are calculated with a fixed pressure (typically 1·5 GPa; e.g. Wood et al., 1990Go; Woodland et al., 1992Go; Ballhaus, 1993Go).

The dataset of Luhr & Aranda-Gomez (1997)Go provides a good opportunity to test the pressure dependence of {Delta}FMQFFsM, because it includes pressure estimates (after Köhler & Brey, 1990Go) of spinel peridotites that apparently represent widely different depths of the lithosphere. The {Delta}FMQFFsM values of the Mexican xenoliths obtained with the method of Wood et al. (1990)Go display a slight inverse correlation with pressure (Fig. 2b), which is not seen for corresponding {Delta}NNOFFsM values (Fig. 2c). The strongest pressure effects are shown by the low-pressure xenoliths from the San Quintin field.

The pressure dependence of {Delta}FMQFFsM is responsible for the slight westward increase of the mean values of {Delta}FMQFFsM retrieved with the Wood et al. (1990)Go method for the four western Mexican volcanic fields (SQ, MC, DGO, VES; Fig. 3a) because this increase is not reproduced using {Delta}NNOFFsM values (Fig. 3b). Using the log fO2 estimates of Ballhaus et al. (1991)Go, neither the mean {Delta}FMQFFsM values nor the mean {Delta}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)Go do not sustain the systematic increase of the relative oxygen fugacity from east to west that they proposed.



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Fig. 3. Comparison between the means ({blacksquare}) and standard deviations (±1{sigma}) of the {Delta}FMQFFsM (a, c) and {Delta}NNOFFsM (b, d) values for the peridotites of each Mexican volcanic field (except the MC field), using either the calibration of Wood et al. (1990)Go (a, b), or that of Ballhaus et al. (1991)Go (c, d). In the case of the MC field, the values for the single xenolith are represented by open circles. The normalization to NNO is explained in the caption for Fig. 2. Positions along the x-axis correspond to approximate distances from the proposed Mesozoic–Cenozoic palaeotrench, with Baja California restored to its pre-rift configuration [compare fig. 9 of Luhr & Aranda-Gomez (1997)Go]. Abbreviations are as in Fig. 1.

 
Given the large uncertainties in pressure estimates for spinel lherzolites, which show an average 1{sigma} of ±4·5 kbar with the Ca-exchange olivine–clinopyroxene geobarometer of Köhler & Brey (1990)Go, the oxygen fugacities estimated with the FFsM equlibrium should be normalized to the NNO, not to the FMQ equilibrium.


    THE SIGNIFICANCE OF RELATIVE OXYGEN FUGACITY VALUES REGARDING THE OXIDATION STATE OF THE MANTLE
 TOP
 ABSTRACT
 INTRODUCTION
 SOME REMINDERS ABOUT {Delta}FMQ
 DIFFERENT ESTIMATES OF...
 THE PRESSURE DEPENDENCE OF...
 THE SIGNIFICANCE OF RELATIVE...
 REFERENCES
 
Luhr & Aranda-Gomez (1997)Go interpret the increase in {Delta}FMQFFsM that they calculated to reflect oxidation related to subduction. However, there is no reason to expect a clear correlation between {Delta}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+/{Sigma}Fe (an extensive variable). Canil et al. (1994)Go and Canil & O’Neill (1996)Go, who have studied the distribution of Fe3+ in upper-mantle assemblages using Mössbauer spectra of minerals, have concluded that ‘the complex nature of the partitioning of Fe3+ between mantle phases results in complicated patterns of the activities of the Fe3+-bearing components, and thus in calculated equilibrium fO2, which show little correlation with whole-rock Fe3+ (Canil & O’Neill, 1996Go).

Luhr & Aranda-Gomez (1997)Go also wonder, as have others (e.g. Ionov & Wood, 1992Go; Brandon & Draper, 1996Go), why there is no inverse correlation between indicators of the refractory nature and {Delta}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)Go, Ionov & Wood (1992)Go or Brandon & Draper (1996)Go for other mantle regions.

An oxidizing metasomatic overprint should increase whole-rock Fe3+/{Sigma}Fe. However, all available reliable (Mössbauer based) values from metasomatized xenoliths (five samples; Canil et al., 1994Go; Brandon & Draper, 1996Go) 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+/{Sigma}Fe values that increase towards the dyke, but only moderately high {Delta}FMQFFsM values, which do not increase with whole-rock Fe3+/{Sigma}Fe (McGuire et al., 1991Go). The Fe3+/{Sigma}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+/{Sigma}Fe towards the dyke reflects the increasing modal abundance of metasomatic, Fe3+-rich amphibole (McGuire et al., 1991Go).

The detailed study of McGuire et al. (1991)Go demonstrates how complex the redox effect of metasomatism is, and how little is known about it. Because {Delta}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 {Delta}FMQFFsM end of the sample distributions (e.g. Mattioli et al., 1989Go; Wood & Virgo, 1989Go; Bryndzia & Wood, 1990Go; Ballhaus et al., 1991Go; Woodland et al., 1992Go), yet others see the opposite relationship (e.g. Chen et al., 1991Go) or find no correlation beween metasomatism and relative oxygen fugacity (Ionov & Wood, 1992Go).

In conclusion, Luhr & Aranda-Gomez (1997)Go present no convincing evidence that the {Delta}FMQFFsM variations in their xenolith samples are related to the interaction with oxidizing fluids.


    ACKNOWLEDGEMENTS
 
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
 
*Telephone: +49 (0) 6221-54-4810. Fax: +49 (0) 6221-54-4805. E-mail: dlattard{at}min.uni-heidelberg.de Back


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 DIFFERENT ESTIMATES OF...
 THE PRESSURE DEPENDENCE OF...
 THE SIGNIFICANCE OF RELATIVE...
 REFERENCES
 
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Berman, R. G. (1988). Internally consistent thermodynamic data for minerals in the system Na2O–K2O–CaO–MgO–FeO–Fe2O3–Al2O3–SiO2–TiO2–H2O–CO2. Journal of Petrology 29, 445–522.[Abstract/Free Full Text]

Brandon, A. D. & Draper, D. S. (1996). Constraints on the origin of the oxidation state of mantle overlying subduction zones: an example from Simcoe, Washington, USA. Geochimica et Cosmochimica Acta 60, 1739–1749.[Web of Science]

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