U-series disequilibria in MORB from the Garrett Transform and implications for mantle melting
Introduction
Mid-ocean ridges are the dominant crust-producing domains on Earth. Adiabatic decompression melting of upwelling mantle peridotite produces mid-ocean ridge basalt (MORB). The composition of the melt depends on the source material, degree of melting, depths of initiation and termination of melting, how melt–solid segregation occurs, and extent of fractional crystallization and magma mixing. As numerous studies have demonstrated, considerable chemical and isotopic variability exists in MORB erupted both on and off the ridge axis (e.g., [1], [2], [3]). Off-axis basalts (e.g., seamounts and transform basalts) are subject to similar melting processes as on-axis basalts. However, they are less dominated by magma mixing processes [4], [5], [6] and thus show an even greater degree of chemical variability [7], [8], [9], [10], [11], [12], [13], [14]. However, because only a few of these MORB suites have also been measured for their isotopic compositions of Hf, Nd, Sr, and Pb (e.g., [15]), the extent to which this chemical variability reflects variations in the melting processes, as opposed to variable mixing of melts from depleted (peridotitic) and enriched (pyroxenitic) sources is not well constrained.
There is little debate that compositional variability in some MORB reflects mantle source heterogeneity. Differences in long-lived isotopes occurring over short spatial scales support the proposition of a chemically heterogeneous mantle (e.g., [16], [17], [18], [19], [20], [21]). However, the role of melting a heterogeneous mantle in generating uranium series (U-series) disequilibium and trace element fractions in MORB, remains uncertain. Source heterogeneity and its role in melting has been recently addressed by Sims et al. [15] who, based on combined measurements of U-series disequilibria (U–Th–Ra and U–Pa), radiogenic isotopic compositions (Nd, Sr, Hf, and Pb) and major and trace element abundances, propose a mantle source beneath the 9–10°N segment of the East Pacific Rise (EPR) that is chemically homogeneous over the length scale of melting. Furthermore, recent 2D modeling also shows that significant fractionation of trace element ratios and U-series nuclides can occur as a result of melting processes without requiring source heterogeneities [22], [23], [24].
U-series disequilibria often are used to constrain the timescales of melt generation, melt ascent processes and differentiation (e.g., [2], [3], [15], [17], [20], [25], [26], [27], [28], [29], [30], [31], [32], [33], [34], [35], [36], [37], [38], [39]). U-series data provide melt generation and ascent constraints because these magmatic processes operate over time scales similar to the half-lives of 230Th (t1/2≈75,400 years), 231Pa (t1/2≈33,000 years), and 226Ra (t1/2≈1,600 years). Thus, studies of disequilibria between daughter and parent isotopes ((230Th)/(238U), (231Pa)/(235U), (226Ra)/(230Th)) can be used to make deductions about magma generation and evolution. Furthermore, because secular equilibrium should exist prior to melting for all the U-series daughter–parent pairs in a mantle source, regardless of enriched or depleted character, observed U-series disequilibria reflect the melting process and not simply source variations.
Although powerful for examining melting processes, U-series disequilibria alone cannot unambiguously distinguish melt generated from a homogeneous source versus that from a heterogeneous source. In particular, variations in Th/U, a ratio of two incompatible elements, could reflect mantle source or could reflect the melting process; discriminating these two alternatives requires complementary measurement of long-lived isotope systems (Sr, Nd, and Pb) indicative of the time-integrated parent–daughter ratios of the mantle sources. When used in concert with U-series isotopes, long-lived isotopic systems enable us to better distinguish between the effects of “source” variability and melting “process” (e.g., [15], [17], [25], [34], [40]).
Here, we focus attention on the genesis of melts from a location where magma chamber processes are less active, decreasing the role of magma mixing and accumulation in lessening the magma diversity of the melting column. Specifically, we investigate basalts from the Garrett Transform, which offsets the fast-spreading southern EPR at 13°30′S. We observe correlations between U-series disequilibria, trace element concentrations, and incompatible trace element ratios, which are consistent with mixing between two end-member melts. We also observe distinct 87Sr/86Sr isotopic ratios indicating mantle source heterogeneities. However, the link between U-series disequilibria and source heterogeneity is not clear. These observations closely parallel observations from another intra-transform domain, the Siqueiros Transform (9°N EPR), both in terms of chemical and spatial characteristics.
Section snippets
Geological setting and background
The Garrett Transform is located at ∼13°30′S on EPR and forms the northern border of the longest, straightest, and fastest portion/segment of the global mid-ocean ridge system (Fig. 1). It offsets the EPR for ∼130 km in a right lateral sense and consists of three oblique intra-transform spreading centers (named Alpha, Beta, and Gamma ridges) linked by strike-slip faults and individual transform valleys [41]. Young volcanic rocks (based on submersible observation) occur primarily in
Methods
We analyzed eleven samples from the Garrett Transform for U–Th–Pa–Ra disequilibria and Sr isotopes by thermal ionization mass spectrometry (TIMS), secondary ion mass spectrometry (SIMS), plasma ionization multi-collector mass spectrometry (PIMMS), and inductively coupled plasma–mass spectrometry (ICP–MS). All of the samples were hand-picked chips of fresh glass (0.3–1.5 g). The details of sample preparation and chemistry followed a modified version of Lundstrom et al. [32], Andrews et al. [48],
Concentrations and U-series disequilibria
(230Th)/(232Th) for 7 of 11 samples was measured by SIMS, using the Cameca IMS 1270 at Woods Hole Oceanographic Institution (WHOI) [50] with 2σ errors of 2–5% (Table 3). (230Th)/(232Th) in four samples was measured by PIMMS, using a ThermoFinnigan Neptune (first at Bremen, later at WHOI) [51] with 2σ errors of 0.3–0.4%. Three samples were measured by both techniques and show good agreement within the analytical uncertainties of the two techniques. Assessing the accuracy of disequilibria
Mixing relationships
Positive correlation between Th/U and (230Th)/(238U) is a ubiquitous observation within MORB studies (e.g., [2], [15], [17], [20], [29], [30], [33], [54], [55]). Linear correlation on an equiline diagram, where both axes have a common denominator, indicate mixing between chemically distinct melts having differing Th/U and 230Th excess.
The Garrett Transform sample set produces the same trend of higher Th/U having higher (230Th)/(238U). Indeed, the Garrett data show a remarkable systematic
Conclusions
- 1.
The observed correlations between U-series disequilibria, trace element concentrations and incompatible trace element ratios in Garrett Transform lavas suggest generation of two end-member melts: one with 230Th excess, high Th and U concentrations and high K/Ti, and another with 238U excess, low Th and U concentrations and low K/Ti. These observations closely parallel observations from the Siqueiros Transform in terms of their relationship between chemical characteristics and geological setting.
Acknowledgements
We thank B. Bourdon and H. Zou for thoughtful and critical reviews. We thank L. Ball (ICP-MS, PIMMS analyst, WHOI), G. Layne (SIMS analyst, WHOI) and P. Janney (PIMMS analyst, Chicago Natural History Museum). This manuscript was prepared while FJT was a post-doctoral researcher at the University of Illinois, Urban-Champaign. This work was supported by NSF grant OCE-9910921 to CCL and NSF grants OCE-9730967 and OCE-0137325 to KWWS. The samples from the Garrett Transform were obtained by the
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