Introduction

According to the theory of plate tectonics, ocean crust should not contain rocks older than adjacent oceanic plates in mid-ocean ridges. The discovery of unusually old rocks and minerals in the vicinity of present-day mid-ocean ridges1,2,3, which is far away from the continental margins, requires an alternative mechanism to explain how the ancient rocks have stayed at the present site without being carried away by the spreading oceanic floor. The occurrences of ancient rocks or minerals that were confirmed by absolute dating were sparse and confined in the Mid-Atlantic Ridge so far3,4. More convincing observations of ancient rocks in mid-ocean ridges of the Atlantic Ocean and other oceans are highly needed before probing their significance for the formation and evolution of the oceans. Recently, several studies, from the Southwest Indian Ridge (SWIR), used ion microprobe U–Pb geochronology of zircon to date the crystallization of igneous rocks intruded into the lower crust in these areas, providing considerable new insight into the time scales of magmatism at mid-ocean ridges5,6,7,8. These absolute dating results, however, restricted in a single segment of Atlantis Bank in the SWIR. This paper reports in-situ U–Pb age determinations for zircon in petrographic thin sections of a gabbro and a diorite dredged in the Gallieni Fracture Zone at 53°E (Fig. 1). The discovery of Jurassic zircons from the diorite, which has extreme Nd and Hf isotopic ratios consistent with a continental crustal component, suggests preservation of relic continental fragments in the Southwest Indian Ridge.

Figure 1
figure 1

Bathymetric map of the Southwest Indian Ridge floor, showing the locations of samples reported here.

(a) The base map was prepared using Generic Mapping Tools (GMT)44, using ETOPO1 bathymetric data45. (b) Oblique view of the 52–53°E segment (looking SSE) from GeoMapApp (www.geomapapp.org) and sample locations.

Full size image

Sample and Results

The SWIR separates the African and Antarctic plates and is classified as a highly oblique ultraslow-spreading ridge9, extending for nearly 8,000 km between the Bouvet and the Indian Ocean Triple Junction (Fig. 1). The rocks studied here are from the 53°E amagmatic segment between the Gallieni fracture zone (FZ) (52o20′E) and the Gazelle FZ (53o30′E), which is a typical amagmatic segment and formed at effective full spreading rates <12 km/Myr9. This section of the SWIR formed by northeastward propagation of the Indian Ocean Triple Junction between oceanic lithosphere created at the Central Indian and Southeast Indian Ridges10. The 53oE segment is floored by predominantly mantle peridotites with scarce crustal rocks11. This segment of the SWIR has been the focus of several recent dredging expeditions, including the Scripps Institution of Oceanography Indomed Expedition Leg 8, the RV Marion Dufresne Cruise 107 and the RV Dayang Yihao cruise 2111.

The samples examined here were collected during the RV Dayang Yihao Cruise 21 in 2010. Sample D4-2-3 (dredge D4-2) is from the transform wall at the end of an east–west ridge at approximately 36o40′S south of the spreading centre. Samples D1401 (dredge D1401) were collected on the northern wall of the central rift valley at approximately 35o50′S. Sample D4-2-3 is a quartz diorite intruded by plagioclase and quartz-bearing felsic vein (Fig. S1). Mineralogy of the host diorite comprises plagioclase, amphibole, minor pyroxene, quartz, ilmenite and apatite (Table S1, Fig. S1). The felsic vein cross-cuts the diorite and has graphic textures characterized by fine-grained intergrowths of plagioclase and quartz. Sample D1401 is an oxide gabbro, consisting of plagioclase, pyroxene, ilmenite and apatite. Full sample designations and detailed descriptions can be found in Zhou and Dick11.

In thin sections, zircon occurs both in the diorite/gabbro and in the felsic vein, locating at the borders between mineral grains or being included in plagioclase (Fig. 2). The analyzed zircons included in-situ zircon crystals in thin sections and fragments extracted from whole rocks using the conventional techniques, including crushing, sieving, heavy liquid and hand picking. Individual zircons were mounted in epoxy, polished and imaged in reflected light, backscattered light and cathodoluminescence (CL). Additional data and figures are shown in the Supplementary material.

Figure 2
figure 2

Representative CL images of zircon in petrographic thin sections.

Inset photomicrographs showing the location of ion probe pits.

Full size image

Zircons from sample D4-2-3 occur as subhedral to anhedral crystals, have unzoned or sector-zoned CL responses (Fig. 2). They show heavy-REE enrichment, positive Ce anomalies and negative Eu anomalies in normalized REE patterns (Fig. 3), high contents of Th (331–3157 ppm) and U (265–3967 ppm) and high Th/U ratios (av. 1.18; Table S2). These observations are characteristic of magmatic zircons12. The igneous origin of the zircons, together with the lack of evidence of deformation, recrystallization or metamorphic overgrowths, suggests that the U–Pb zircon ages reflect the timing of igneous crystallization of the sample. Zircon crystallization temperatures range from 963–851 °C with an average value of 903 ± 9 °C using the uncorrected Ti-in-zircon thermometry13 (α(SiO2) = 1). Thirty-two analyses on 32 zircon grains are reported in Table 1 and presented in Fig. 3. Analyses yield concordant U–Pb ages, with apparent 206Pb/238U ages from 188.9 to 175.2 Ma with a weighted mean age of 180.1 ± 1.0 Ma (MSWD = 1.8), which reflects the timing of igneous crystallization of the samples.

Table 1 SIMS and LA–ICPMS zircon U–Pb isotopic data for sample D4-2-3.
Full size table
Figure 3
figure 3

207Pb-corrected/230Th-disequilibria corrected ages for sample D4-2-3 (a–b) and D1401 (c–d).

Full size image

Zircons from sample D1401 are mostly euhedral, have sector and fine-scale oscillatory and/or convoluted zoning patterns. All grains are overprinted by secondary textures characterized by cloudy porous features in CL. In contrast to normal magmatic grain (Fig. 2e), zonation within most zircons is often perturbed, convoluted, or chaotic (Fig. 2d,f; Figs S3 and S4). In some instances, perturbed zonation and micro-porosity coincide with specific growth zones within euhedral, otherwise oscillatory zoned zircons, implying alteration of preexisting magmatic grains. Magmatic resorption textures characterized by areas of embayed grain boundaries and secondary luminescent band was observed in some zircons (Fig. 2e), indicating development of younger magmatic overgrowths. Qualitative electron microprobe (EDS) analysis of porous domains displays micron-scale P-, Fe-, Ca- and Cl-rich inclusions, indicating fluid inclusions or salt residues within the pores. The primitive oscillatory zoned, the secondary luminescent and the porous domains define a three stages growth of zircon. The secondary overgrowth is not constrained in this study due to insufficient width for ion probe analysis.

Titanium values largely overlap between the oscillatory zoned and the porous domains (5.4–8.1 ppm vs 5.9–10.9 ppm), which yield Ti-in-zircon temperatures from 748–689 °C with an average value of 711 ± 11 °C for oscillatory domains and 729 ± 21 °C for porous domains, both of which are significantly lower than that of D4-2-3 zircons. The oscillatory zoned and porous domains show similar HREE enrichment relative to the LREEs as well as positive Ce and negative Eu anomalies (Fig. 3), similar to D4-2-3 zircons. Average (Sm/La)N for porous zircon domains is 35 (vs 628 in oscillatory domains), reflecting La enrichment in porous domains. These features, along with the porous and chaotic CL zoning are indicative of interaction with aqueous fluids14, which is further evidenced by the higher average (Yb/Gd)N ratio of 78 for the porous domains than the average of 24 for oscillatory domains, resembling that of typical magmatic zircons (~23)15,16.

U–Pb isotopic analyses were performed on both oscillatory zoned and porous domains. Thirty-six spot analyses on 30 zircon grains were robust and clustered to give well-constrained error-weighted mean 206Pb/238U ages between 4.3 Ma and 5.8 Ma, showing two distinct age populations between oscillatory zoned and porous domains (Table 2; Fig. 3). A weighted average age of 5.38 ± 0.07 Ma (MSWD = 0.82) and a lower intercept age of 5.36 ± 0.10 are obtained for the oscillatory domains (n = 25) and a weighted average age of 4.97 ± 0.14 Ma (MSWD = 0.28) and a lower intercept age of 4.89 ± 0.11 are defined by 11 analyses on the porous domains. Since the features that characterize porous domains are generally consistent with growth or alteration during aqueous fluid-assisted processes, the weighted-average age of 5.38 ± 0.07 Ma for the oscillatory domains, that are of magmatic in origin, is taken as the best estimate for the timing of igneous crystallization. The weighted mean age of 4.97 ± 0.14 Ma for the porous zircons analyzed is interpreted to reflect crystallization of the vein that intrudes the gabbro.

Table 2 SIMS U–Pb isotopes for zircons from sample D1401.
Full size table

Hafnium isotope concentrations were collected for 40 zircon grains from sample D4-2-3 and 12 zircons for sample D1401 (Table S3). Initial 176Hf/177Hf, denoted εHf(t), is the Hf-isotopic signature of the magma at the time of zircon crystallization and hence reflect that the final derivation of the host rocks from the assumed depleted mantle. The zircon grains from D4-2-3 yielded a restricted spread of initial εHf(t) values of −2.3 to −4.5 (t = 180 Ma), with an average value of −3.2 ± 0.2 (1σ). In contrast, zircons from D1401 have highly positive εHf(t) values of +15.7 to +12.4 (av. +14.4 ± 0.7 1σ; t = 5.4 Ma), plotting at the depleted end of the mantle array17 and suggesting a juvenile rock or magma origin from mantle with a moderate- to long-term depletion of Hf relative to Lu.

Nd and Hf isotope compositions of mineral separates and the whole rock of are reported in Table S3. Initial isotopic compositions were calculated at 180 Ma for sample D4-2-3 and 5 Ma for sample D1401. The amphibole from D4-2-3 has negative εNd(t) (−2.4) and εHf(t) (−1.9) values, resembling the global Nd–Hf isotope variation of ocean island basalt within the Terrestrial Array17, implying that the sample was derived from an enriched mantle source and/or due to crustal contamination or mixing with metasomatized lithospheric mantle. The Nd and Hf isotopic compositions of the whole rock are distinct from those of amphibole. The slightly increased negative εHf(t) value of the whole rock (−2.6) can be explained by the “zircon effect”18 where unradiogenic Hf is locked in zircons and preferentially retained the Hf component even during intense overprinting. The elevated εNd value of the whole rock (−1.3) likely reflects the effect of seawater alteration and leaching on Sm–Nd isotope system of ancient submarine rocks. Interestingly, a two-point isochron age of 189 ± 9 Ma, which is coincide with the c. 180 Ma zircon U–Pb age within error, is defined by whole rock and clinopyroxene. Sample D1401 has positive εNd (+6.8) and εHf (+13.3) values, resembling those of the mafic/ultramafic rocks from the 9–25oE Southwest Indian Ridge19.

Discussion

Zircons recovered from oceanic diorite and gabbro exposed on the northern wall of the central rift valley, SWIR, typically display oscillatory and sector zoning consistent with igneous crystallization from mafic magmas. There is little magnetic data for the Gallieni Fracture Zone, so directly comparing zircon U–Pb ages with the magnetic ages is difficult. As a first-order approximation, a half-spreading rate of 4.1 ± 0.4 km/Myr is defined by the zircon age (5.38 Ma for sample D1401) versus distance from the ridge axis (~20 km; an along-axis uncertainty of 2 km is estimated based on the valley bathymetry patterns), much lower than the predicted 5.5 km/Myr on the Antarctic and African flanks of SWIR14. Anomalously older zircon ages than the predicted magnetic ages for a given portion of crust were reported in several recent studies on Atlantis Bank6,7, which were commonly interpreted to reflect assimilation of pre-existing gabbroic rocks from the mantle lithosphere6. Following this interpretation, the age range of our anomalously old samples (1.3 to 1.7 Myr) would reflect crystallization over depth of ~7 to 9 km below seafloor in the axial valley by assuming a constant spreading rate of 5.5 km/Myr. This depth would be reduced significantly when considering the geometry of the fault15,16. Alternatively, the anomalously old zircon may reflect sample spacing due to the uncertainty in location by dredging. This interpretation appears to gain support from the observation that the anomalously old zircon relative to the magnetic age, was limited to surface rocks6,7 and are not found in drill-hole samples in Atlantis Bank8. A similar discrepancy between surface and drill-hole sample occurs at Atlantis Massif in the Mid-Atlantic Ridge, where the surface samples yield an anomalously old age, whereas drill-hole samples did not15,16, supports the latter interpretation. The most likely explanation, however, is that spreading is asymmetric, roughly 10 cm/yr to the south and 4 cm/yr to the north. Similar asymmetries are common along the Southwest Indian Ridge, both by examining isochrons and the EMAG2 magnetic anomaly map20 in the GeoMapApp database. Such asymmetric north- south spreading has been confirmed at Atlantis Bank by paleomagnetics21,22,23 and zircon age dating5,6,8 where the ridge spreads at ~1 cm/yr to the south and 4 cm/yr to the north. This is the first time that zircon dating has confirmed asymmetric spreading away from the transform, as in the other cases it is the spreading direction parallel to the transform where this is documented. More distributed surface sampling combined with drilling will clarify the age discrepancy and provide a more accurate estimate of crustal inheritance.

The relatively young ages for the porous zircons may reflect solid-state recrystallization12,24,25 and/or be related to hydrothermal fluid flow associated with intrusion of felsic veins in this area, suggesting that the porous textures developed soon after crystallization of normal magmatic zircons. The initial 176Hf/177Hf compositions of the normal magmatic grains overlap those of the porous domains, suggesting that fluids catalyzing the formation of the porous zircon domains were derived essentially in situ from the magma that crystallized the zircon originally. The sample has a roughly similar range of Hf-isotope ratios, with the local ridge peridotites along the SWIR19,26, but are more radiogenic than almost all basalts analyzed thus far (except for one basalt from Discovery FZ)19.

The SWIR formed with the Mesozoic breakup of Gondwanaland. Zircons from sample D4-2-3, ~60 km south of the axial valley of the SWIR and immediately to the east of the Gallieni Transform fault, have an unusually old U–Pb age of 180.1 ± 1.0 Ma, which is comparable to the initial timing of the opening of the Indian Ocean. Are these rock/zircons erratic or in-situ? The age similarity between this ancient sample and the Karoo large igneous province magmatism (179–183 Ma)27, which is associated with the breakup of the Gondwanaland at c. 180 Ma, apparently suggest an erratic origin, such as ice-rafting and tsunami-depositing, for the ancient rocks. However, the sample location is far away from the continental margins and it is impossible to sustain the drop-stone theory unless a reasonable explanation is given for the dropping of rocks exclusively on the Gallieni FZ. The sample is thus considered in-situ or only slightly moved in origin (see below for further discussion).

Are these rock/zircons relics or formed in-situ along the spreading axis? If the rocks/zircons were formed during the generation of the magma, their age would be expected to be about ten million years at most. We thus consider two contrasting possibilities for the origin and the route of the old rock/zircons: 1) An intact Gondwana fragment on the sea-floor ever since formation; 2) A partially altered relic that once resided in shallow regions of the upper mantle and was entrained and transported to the vicinity beneath the axis. Zircon, residing in shallow regions of the upper mantle on the order of a hundred million years, would significantly lose its radiogenic lead via diffusion28, protracted residence of the fragments in the upper mantle is thus highly unlikely.

The 176Hf/177Hf ratio of 0.282630 ± 0.7 (2SD) for the whole rock of sample D4-2-3 is higher than those of the zircons (0.282609–0.282547). The zircon initial εHf values show a variation from −4.5 to −2.3, which is distinct from those of the SWIR peridotites and basalts (+13.9–+6.4)19. The unradiogenic Nd isotope (εNd(t) = −2.4), together with the wide range of initial εHf values of zircons, may suggest crustal contamination or interaction between asthenosphere-derived melts and the metasomatized lithospheric mantle in the generation of magmas. The analogous geochronology and isotopic signatures between the ancient diorite and the Karoo magmatic rocks27,29, imply that the diorite may be correlated with the Jurassic magmatic rocks that emplaced prior to the breakup of southern Gondwana and the opening of the SW Indian Ocean. The rock may represent the relicts onto the margin of the southern Gondwana during the rifting of Africa and Antarctica, possibly a mixture of juvenile and recycled crust in a continental magmatic arc30.

Unusually old ages have also been reported from the Mid-Atlantic Ridge3,4. Several possible mechanisms were introduced to explain the origin of these rocks, mostly of continental affinity, such as ceased ocean-floor31, non-spreading blocks1, oscillatory spreading4 and non-drifting slices3. However, all the explanations are difficult to verify and no convincing data for these hypothetic mechanisms have been given so far. Finding an age of 180 Ma in zircons in a quartz diorite on the SW Indian Ridge is likely to raise considerable doubt as to an ocean ridge origin of the sample. At first glance, it would seem most probable that the sample is a glacial erratic deposited on the seafloor on crust of some ~5 Ma age. Several factors make it possible to reconsider this hypothesis.

First is the condition of the rock and state of alteration, which are what would be expected for a highly evolved plutonic rock in this particular tectonic setting. Quartz diorites do occur as late differentiates in oceanic gabbro suites and crosscutting abyssal peridotites. They are not common, but they exist. Highly evolved gabbros and their differentiates are most commonly found as late shallow intrusives into gabbros and peridotites on transform walls where this sample came from, while primitive gabbros are more commonly found near segment centers32. Petrographic examination shows mafic minerals are largely replaced by green amphibole and chlorite, while plagioclase appears albitized (Fig. S1). This suggests an upper greenschist facies assemblage that is typical of late high-level intrusive rocks at ocean ridges due to hydrothermal circulation into the crust and shallow mantle near transforms. Moreover, the rock itself shows no signs of glacial scour or rounding which are common in ice-rafted dropstones deposited on the seafloor. So unlike many dropstones investigated by H. Dick over his years’ survey and sampling along the SW India Ridge, the sample is appropriate to its geologic context.

Next is the age of the sample itself. One hundred and eighty million years coincides with the Karoo volcanic event and the initiation of continental breakup. Most of the borderlands to the SW Indian Ridge along the coastline of South Africa are Archean cratonic rocks. However, on the eastern side of Africa and Madagascar lies rocks of the Neoproterozoic Pan-African Orogenic Belt, with their conjugate in East Antarctica. The Pan African Orogenic Belt is an accreted terrain, assembled during the closure of the Mozambique Ocean during the assembly of Gondwana from old island arc terrains and fragments of reworked Archean cratonic rocks. The Karoo volcanic event was widespread and its remnants are found in South America, Antarctica, Africa and Australia and would have intruded the Pan African Orogenic Belt during Gondwanan breakup.

There is substantial evidence, based on the geochemistry of the peridotites from the Dragon Bone spreading segment, immediately north of that of the dredged diorite, that the present mantle source of the SW Indian Ridge there represents such old arc-mantle wedge mantle drawn up between the plates along the ridge30. The Gallieni FZ nucleated at the margin of a bathymetric plateau lying to the north flanking the eastern side of the Madagascar Plateau. Thus it represents a fracture zone that likely formed by the breakup of an old Gondwanan continental fragment of the Pan-African Orogenic Belt only about 40 to 50 million years ago and is a relatively new and quite shallow ocean basin. Thus, it is reasonable that old Neoproterozoic arc-mantle wedge material, cross intruded by diorite during the initial phase of breakup of Gondwana, was drawn up between the diverging plates and emplaced into the wall of the Gallieni Transform.

Yet to be considered in the discussion is that the quartz diorite is undeformed. Thus, it was not emplaced into its present position in the solid-state, rafted in with delaminated mantle lithosphere. Instead it was intruded into the shallow mantle beneath the rift valley floor, before being unroofed and emplaced onto the transform wall. Mantle peridotites dredged from the Dragon Bone amagmatic segment have universally undergone such deformation and any intrusive within those rocks would have been deformed with them. However, this was not the normal thermal environment of an ocean ridge segment. First, this amagmatic segment exposes an enormous region of mantle peridotite where the sample was taken. Thus there was little volcanism at the time of emplacement of the diorite and enclosing mantle rocks to the seafloor. This can be ascribed to either very refractory mantle source material or to an extraordinarily cool upper mantle due to ultraslow spreading and the cooling effect of the adjacent 110 km offset Gallieni FZ on the upwelling mantle at the ridge transform intersection. Given the already amagmatic state of spreading, this transform edge effect33, would almost totally suppress mantle melting. In such a situation, a quartz-diorite vein, with its very low melting point (~800–1,000 °C) compared to basalt (~1,500–1,250 °C), could be remobilized as the mantle upwelled, while the enclosing peridotite was largely unaffected, to intrude at higher level, carrying its original Gondwanan zircons with it.

This scenario is a reasonable explanation for the emplacement of the quartz diorite, its intrusion into the shallow mantle beneath the rift valley floor, why it is not deformed, but preserves the ancient zircons. It is circumstantial, rather than definitive evidence that permits the possibility that the 180 Ma zircons may have been emplaced in-situ – or not.

Analyses methods and data reduction

Major-element compositions of minerals were analyzed by electron probe microanalysis with a JEOL JXA-8230 Superprobe system at Tongji University. The analyses were performed using an accelerating voltage of 15 kV and beam current of 10 nA, using a 5 μm diameter beam. Natural and synthetic mineral standards were employed for all minerals. JEOL software using ZAF corrections was employed. Representative major-element compositions of feldspar, amphibole, epidote and chlorite are given in Supplemental Table S1.

The U–Pb isotopes for zircons in thin sections were obtained with a Cameca ims1280 microprobe housed at the Institute of Geology and Geophysics, Chinese Academy of Sciences in Beijing. The Pb/U calibration was performed relative to the reference zircon Plešovice, which was analyzed repeatedly throughout each session. Operating conditions and analytical protocols are essentially the same as described by Li et al.34. A ~20  μm beam was used. U–Pb data for zircon fragments, extracted from rocks using standard crushing, heavy liquid and magnetic separation techniques and zircon trace element analyses, were obtained by LA–ICP-MS at the State Key Laboratory of Geological Processes and Mineral Resources, China University of Geosciences, using a pulsed 193 nm ArF Excimer laser coupled to an Agilent 7500 ICPMS with a spot size of 32 μm. Zircon standard 91500 was used to normalize fractionation during analysis. External calibration was performed relative to GJ-1 and NIST 610 combined with internal standardization of Si. Off-line selection and integration of background and analytic signals, time-drift correction and quantitative calibration were performed followed that of Liu et al.35.

A correction for common Pb was made using the 207Pb method36 and an age appropriate model Pb composition37. An additional correction has been made to adjust for initial 238U–230Th disequilibrium using the equations of Schärer38. Zircon commonly hosts ample U relative to Th, which will produce a deficit of radiogenic 206Pb due to an initial 230Th deficit and yield a 206Pb/238U age too young. To correct for these disequilibria for the young sample D1401, the ratio of the mineral/melt partition coefficient for Th and U for zircon (f = [Th/U]zircon/[Th/U]magma) is estimated by dividing the individual spot analyses with the Th/U ratio of bulk rock analyses for rocks collected in this area (Th/U = 2.6 ± 0.5 (95% confidence); data are compiled from PetDB (http://www.earthchem.org/petdb). Both 206Pb/238U and 207Pb/206Pb ratios are adjusted to account for Th-disequilibria, with these new ratios used to calculate a 207Pb corrected 206Pb/238U age for each analysis of sample D1401.

Zircon Hf isotope analyses were conducted in the the state Key Laboratory of Geological Processes and Mineral Resources, China University of Geosciences in Wuhan, using a Finnigan Neptune plus multi-collector ICP-MS and with a Geolas 2005 excimer ArF laser laser ablation system. All data were acquired on zircon in single spot ablation mode at a spot size of 44 μm. We applied the directly obtained βYb value from the zircon sample itself in real-time. The 179Hf/177Hf and 173Yb/171Yb ratios were used to calculate the mass bias of Hf (βHf) and Yb (βYb), which were normalised to 179Hf/177Hf = 0.7325 and 173Yb/171Yb = 1.13268539 using an exponential correction for mass bias. Interference of 176Yb on 176Hf was corrected by measuring the interference-free 173Yb isotope and using 176Yb/173Yb = 0.7963939 to calculate 176Yb/177Hf. Similarly, the relatively minor interference of 176Lu on 176Hf was corrected by measuring the intensity of the interference-free 175Lu isotope and using the recommended 176Lu/175Lu = 0.0265640 to calculate 176Lu/177Hf. We used the mass bias of Yb (βYb) to calculate the mass fractionation of Lu because of their similar physicochemical properties. The lack of correlation between 176Hf/177Hf and 176Yb/177Hf (Fig. S6) is an indicator that the corrections imposed to the 176Hf/177Hf ratio result in accurate and precise data. Off-line selection and integration of analytic signals and mass bias calibrations were performed following those of Liu et al.35.

The Lu–Hf and Sm–Nd isotope analyses for the whole rock and mineral separates were conducted on a ThermoElectron Neptune™ multi-collector (MC–) ICP-MS in the GeoAnalytical Laboratory at Washington State University. About 200 mg of clean, alteration free amphibole, pyroxene and plagioclase were hand-picked under a binocular microscope. Sample dissolution and chemical separations are described by Cheng et al.41,42 and the full data set is presented in Supplementary Tables. Epsilon Hf and Nd values were calculated using 176Hf/177Hf = 0.282785, 176Lu/177Hf = 0.0336, 143Nd/144Nd = 0.512630 and 147Sm/144Nd = 0.1960 for CHUR43.

Additional Information

How to cite this article: Cheng, H. et al. Jurassic zircons from the Southwest Indian Ridge. Sci. Rep. 6, 26260; doi: 10.1038/srep26260 (2016).