Journal of Petrology Advance Access published online on January 19, 2008
Journal of Petrology, doi:10.1093/petrology/egm086
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A Quartz-bearing Orthopyroxene-rich Websterite Xenolith from the Pannonian Basin, Western Hungary: Evidence for Release of Quartz-saturated Melts from a Subducted Slab
1lithosphere Fluid Research Lab, Department of Petrology & Geochemistry, Institute of Geography and Earth Sciences, Eötvös University Budapest (ELTE), Pazmany Setany 1/c, Budapest, H-1117, Hungary
2Institute of Isotope Geochemistry and Mineral Resources, ETH Zürich, Sonneggstrasse 5, ETH Zentrum, 8092 Zürich, Switzerland
3Research School of Earth Sciences, Building 61 Mills Road, the Australian National University, Canberra, Act 0200, Australia
4Department of Earth Sciences, University of Florence, Via G. LA Pira, 4, Florence, 50121, Italy
5Eötvös Loránd Geophysical Institute of Hungary, Budapest, Columbus U. 17–23, H-1145, Hungary
6Department of Geosciences, Virginia Tech, Blacksburg, VA 24061, USA
Received January 31, 2007; Revised typescript accepted December 19, 2007
| ABSTRACT |
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An unusual quartz-bearing orthopyroxene-rich websterite xenolith has been found in an alkali basaltic tuff at Szigliget, Bakony–Balaton Highland Volcanic Field (BBHVF), western Hungary. Ortho- and clinopyroxenes are enriched in light rare earth elements (LREE), middle REE and Ni, and depleted in Nb, Ta, Sr and Ti compared with ortho- and clinopyroxenes occurring in either peridotite or lower crustal granulite xenoliths from the BBHVF. Both ortho- and clinopyroxenes in the xenolith contain primary and secondary silicate melt inclusions, and needle-shaped or rounded quartz inclusions. The melt inclusions are rich in SiO2 and alkalis and poor in MgO, FeO and CaO. They are strongly enriched in LREE and large ion lithophile elements, and display negative Nb, Ta and Sr anomalies, and slightly positive Pb anomalies. The xenolith is interpreted to represent a fragment of an orthopyroxene-rich body that crystallized in the upper mantle from a hybrid melt that formed by interaction of mantle peridotite with a quartz-saturated silicate melt that was released from a subducted oceanic slab. Although the exact composition of the slab melt cannot be determined, model calculations on major and trace elements suggest involvement of a metasedimentary component.
KEY WORDS: quartz; mantle; silicate melt inclusion; SiO2-rich melt; subduction; Carpathian-Pannonian Region
| INTRODUCTION AND GEOLOGICAL BACKGROUND |
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This paper describes a quartz-bearing orthopyroxene-rich websterite xenolith (sample Szg-klm01) found in alkali basaltic tuff at Szigliget [part of the Bakony–Balaton Highland Volcanic Field (BBHVF)] in western Hungary. To our knowledge, such quartz-bearing mantle xenoliths have not been described in the literature, although opx-rich olivine websterites have been reported from the ultramafic xenolith suite of the BBHVF (Bali et al., 2007
The BBHVF is located in the northern Carpathian–Pannonian Region (CPR) (Fig. 1) on the ALCAPA (ALpine–CArpathian–PAnnonian) basement mega-unit, which was transported c. 450 km eastwards from the Alpine–Dinaric System during the Paleogene–early Miocene (Kázmér & Kovács, 1985
). This process probably involved lithosphere-scale transport, as supported by the preservation of subduction-related geochemical features and deformation patterns in mantle xenoliths (Kovács & Szabó, 2008
). The driving force for displacement (late Oligocene) and subsequent extension (Miocene) is considered to be subduction roll-back of the European plate beneath the ALCAPA unit along the Carpathian arc (Csontos & Vörös, 2004
, and references therein) and collision-induced, eastward-directed mantle flow between the Apulian indenter and the stable European platform (Kovács & Szabó, 2008
, and references therein). Extensive calc-alkaline volcanic activity occurred along the Carpathian Arc during the Neogene (Fig. 1). The developing Pannonian Basin was subsequently affected by a short-lived ENE–WSW to east–west compressional event (Miocene–Pleistocene) (Fodor et al., 1999
) followed by extension. Alkaline basaltic volcanic activity occurred during the post-extension phase of basin formation (Embey-Isztin et al., 1993
), and included phreatomagmatic activity (Martin & Németh, 2004
) at Szigliget at 3·4 Ma (Balogh et al., 1986
). The alkaline basalts contain abundant lower crustal and upper mantle xenoliths (Embey-Isztin et al., 2001
, 2003
; Dobosi et al., 2003a
, 2003b
; Török et al., 2003
; Szabó et al., 2004
), providing information on the composition and evolution of the regional lithosphere.
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| PETROGRAPHY |
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The Szg-klm01 xenolith is rounded, 3 cm in diameter, and free of secondary alteration. It is composed mainly of large, tabular opx (up to 5·0 mm) and subordinate interstitial cpx (Table 1, Fig. 2a). It lacks both olivine and spinel. Opx and cpx contain large (up to 1 mm) rounded and/or euhedral, needle-shaped, transparent quartz (qz) single crystal inclusions (Fig. 2a–d). Needle-shaped qz inclusions usually occur as parallel laths in opx (Fig. 2b and c). Small (1–2 µm) CO2 fluid inclusions occasionally occur near the tip of the needle-shaped qz inclusions, whereas silicate glass is associated only very rarely with them (Fig. 2c). This xenolith differs in texture and modal composition from the peridotite and pyroxenite xenoliths described from the same locality by other workers (e.g. Embey-Isztin et al., 2001
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Silicate MI occur in both cpx and opx. All MI contain brownish to colourless silicate glass and a one-phase CO2-fluid bubble at room temperature (Fig. 2c–f). Primary MI are large (50–150 µm in diameter), rounded or negative crystal shaped (Fig. 2d–g), and occur either as isolated inclusions (Fig. 2d–f) or in clusters (Fig. 2f and g) mainly in the cores of host opx and cpx. The glass:fluid volume ratio is c. 10:1 to 15:1, and the MI never contain daughter minerals. Two generations of secondary MI (Fig. 2f–h) were distinguished. Both generations occur along healed fractures in opx and cpx (Fig. 2f–h). Secondary MI-1 are smaller (< 30 µm in diameter) than the primary MI, they have negative crystal or droplet shapes, and are composed of silicate glass and a fluid phase with variable glass: fluid ratios (Fig. 2f). They form inclusion planes cross-cutting grain boundaries (Fig. 2f). Secondary MI-2 have irregular shape (Fig. 2h). They occur along fractures close to grain boundaries where colourless silicate glass also occurs interstitially, forming <10 µm grain boundary films. In addition to the fluid bubble and silicate glass secondary MI-2 contain daughter minerals (Fig. 2h), which have approximately the same ratio in all secondary MI-2.
CO2 fluid inclusions range from 5 to 25 µm and occur in both pyroxenes as isolated inclusions or in clusters (Fig. 2b).
| ANALYTICAL TECHNIQUES |
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Raman spectroscopic analyses were conducted at ETH Zürich to identify the quartz inclusions and to determine the composition and density of the fluid inclusions and the water content of the glass. A Dilor Labram II system equipped with a 488 nm Ar+ laser source and confocal optics was used. Analysis and spectral treatment were carried out following the suggestions of Kawakami et al. (2003
Primary MI in opx were heated in a N2 atmosphere using a Linkam TS1500 heating–cooling stage at the Lithosphere Fluid Research Lab of Eötvös University, Budapest. A stepwise heating schedule was used (Student & Bodnar, 1999
, 2004
) and the experiment was quenched by turning the power off.
Major element analysis of host minerals (Table 1) was carried out using the JEOL Superprobe JXA-8600 WDS at the Electron Microprobe Laboratory of the CNR–Institute of Geosciences and Earth Resources of Florence, Italy [conditions have been described by Vaselli et al. (1996
)]. MI were analysed using a CAMECA SX50 microprobe at the Department of Geosciences, Virginia Tech [conditions have been described by Szabó et al. (1996
)] and a Jeol Superprobe JXA-8200 at the Bayerisches Geoinstitut (BGI), Germany. Analyses at the BGI were carried out with an accelerating voltage of 15 kV, beam current of 20 nA and beam size of 5 µm. Counting time for each element was 10 s. Natural and synthetic standards were used for calibration and ZAF correction was applied.
Laser ablation inductively coupled plasma mass spectrometry (LA-ICPMS) analyses were carried out at ETH Zürich, using an ArF excimer UV (193 nm) laser source at 70 mJ output energy and 10 Hz repetition rate. The beam diameter was 20–80 µm and 10 ms dwell time was used for all elements. The energy density was homogeneous across the laser beam profile (Heinrich et al., 2003
). Quantification of MI compositions followed the method of Halter et al. (2002
) and K2O from electron microprobe analysis was used as an internal standard. Sample NBS SRM 610 was used for external standardization. Results are given in Table 2.
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| RESULTS |
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Raman spectroscopy and heating experiments
Raman analyses confirm that all solid inclusions in the opx and cpx are quartz crystals with two significant vibration bands at 461·9 and 205·3 cm–1. The Raman spectra show no evidence of conversion from an earlier high-temperature polymorph (i.e. cristobalite–tridymite, e.g. Darling et al., 1997
= 1·17 g/cm3) is higher than that of any of the primary fluid inclusions in lower crustal granulite or peridotite xenoliths previously analysed from the BBHVF (Török & De Vivo, 1995
1 wt %. During heating on the Linkam stage, the MI decrepitated before complete dissolution of the CO2 fluid phase into the melt. Thus, only the onset (840–880°C; average 860°C) and termination (915–980°C; average 960°C) of glass melting were observed and recorded (Fig. 3a).
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Major and trace element chemistry
Opx in the websterite is Fe-rich (average mg-number = 81·7) and Al2O3-poor (c. 2 wt %), compared with opx in olivine websterite, lherzolite and pyroxenite xenoliths from the same area (Embey-Isztin et al., 2001
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All silicate glasses are depleted in MgO (
1·0 wt %), FeO (
3·6 wt %) and CaO (
3·3 wt %), and rich in SiO2 (58–81 wt %) and alkalis (Na2O + K2O 4·0–9·5 wt %), with variable Al2O3 contents (7·0–20·9 wt %). This last variation is most pronounced in the interstitial silicate glass (Fig. 5, Table 1). Silicate glass in primary MI in cpx and opx shows little chemical variation (Fig. 5, Table 1); however, slight differences occur in the FeO, MgO, CaO and Al2O3 contents. FeO (0·5–0·6 wt %) and MgO (
0·02 wt %) contents are lower, whereas CaO (1·93–2·56 wt %) and Al2O3 (16·2–17·2 wt %) contents are higher in cpx-hosted primary MI compared with primary MI in opx (1·5–2·8, 0·2–1·05, 1·22–1·67 and 13·6–14·4 wt %, respectively). Glasses in all primary MI display consistent high K2O/Na2O ratios (1·1–1·8). Reheated primary MI in opx have SiO2 (66–72 wt %) and MgO (0·6–1·0 wt %) contents similar to those of the most SiO2-poor and MgO-rich, non-heated MI (Fig. 5a, Table 1). Compared with the primary MI, secondary MI and interstitial glass have a wide compositional range that includes the compositions of primary MI (Fig. 5). Secondary MI-1 in both cpx and opx contain silicate glass similar in composition to glass in primary MI (Fig. 5). SiO2-rich (c. 80 wt %) interstitial glass occurs between qz and opx, whereas glass along opx–cpx boundaries and in secondary MI-2 is significantly poorer in SiO2 and enriched in other major elements (Fig. 5, Table 1).
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Cpx is strongly enriched in light rare earth elements (LREE) and middle REE (MREE) compared with heavy REE (HREE) (Table 2), with significant negative anomalies for Pb, Sr, Hf, Zr and Ti on primitive mantle-normalized trace element diagrams (Fig. 6a). These clinopyroxenes are more enriched in LREE and MREE, but more depleted in Sr than those in local peridotite, pyroxenite and granulite xenoliths (Fig. 6a and b). Opx in the studied xenolith is depleted in LREE and MREE compared with HREE (Fig. 6a, Table 2). However, both cpx and opx in the xenolith show enrichment in incompatible elements compared with cpx and opx from BBHVF peridotites (Fig. 6b). Both cpx and opx have high concentrations of Cr (4200 and 1770 ppm, respectively) and Ni (855 and 1550 ppm, respectively), the latter being about two times higher than in pyroxenes in local peridotite xenoliths (Fig. 6b).
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Primary MI in both pyroxenes were analysed for trace elements, whereas only secondary MI-1 in opx were analysed. MI compositions show a narrow range, independent of host mineral and textural features (Fig. 6c, Table 2). Primary MI and secondary MI-1 are strongly enriched in incompatible elements and display negative anomalies for Nb, Ta and Sr, and a slight positive anomaly for Pb (Fig. 6c, Table 2). The REE pattern is particularly steep (LaN/YbN 85–134).
Crystallization conditions
The coexistence of CO2 inclusions with MI suggests that the melt became saturated in CO2 during crystallization. The pressure of formation of fluid inclusions may be determined if the density (or homogenization temperature) of the inclusions and the formation temperature are known (Bodnar, 2003a
), assuming that the density does not change after trapping. However, the density may decrease during transport to the surface as a result of stretching of the host mineral (e.g. Bodnar, 2003b
) or leakage along crystal dislocations (e.g. Viti & Frezzotti, 2000
; Vityk et al., 2000
), and evidence for such re-equilibration is usually not recognizable during routine petrographic observation. As a result of re-equilibration the density of the inclusions is less than the original density of the fluid inclusion at trapping. The highest density inclusion most closely approximates the true density, but still represents the minimum entrapment conditions. Thus, in xenolith Szg-klm01, the highest density CO2 inclusion gives the closest, but still a minimum, estimate for the pressure of formation of the rock. The formation pressure of Szg-klm01 estimated using the equation of state of Mader & Berman (1991
) and assuming an entrapment temperature of 960°C (based on MI thermometry) was above 1·1 GPa (Fig. 3b).
Considering that the present-day depth to the Moho in this area is
27–30 km, which corresponds to
0·9–1·0 GPa (Lenkey, 1999
), the CO2 inclusions in this rock must have been trapped in the uppermost mantle, where the rock presumably also formed.
| DISCUSSION |
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The Szg-klm01 xenolith differs in mode, texture and phase composition from peridotite and pyroxenite xenoliths from the same volcanic field (Embey-Isztin et al., 2001
The cpx shows a much stronger enrichment in LREE and especially MREE (LaN/YbN = 8·6, SmN/YbN = 10·6) and depletion in Sr compared with cpx from local cpx- and opx-rich cumulates (LaN/YbN = 1·6–2·1 and 0·9–2·5, SmN/YbN = 2·6–4·2 and 0·2–0·7, respectively), residual peridotites (LaN/YbN = 0·4–1·1, SmN/YbN = 0·9–1·0) or granulites (LaN/YbN = 1·2–5·9, SmN/YbN = 8·2–23·3) (Fig. 6a and b).
Significant modal and chemical differences are observed between the studied xenolith and opx-rich harzburgites and orthopyroxenites from ultramafic xenolith suites from supra-subduction zone tectonic settings worldwide (e.g. Parkinson & Pearce, 1998
; McInnes et al., 2001
; Melcher et al., 2002
; Santos et al., 2002
; Cvetkovic et al., 2004
). Ultramafic xenoliths from supra-subduction zone tectonic settings usually contain refractory opx (mg-number usually >90), Cr-rich spinels and cpx displaying U-shaped chondrite-normalized REE patterns. In contrast, opx in Szg-klm01 is relatively Fe-rich (mg-number = 82) and cpx is strongly enriched in both LREE and MREE compared with HREE.
Interaction of mantle lherzolite with a SiO2-rich melt
SiO2-rich melts responsible for some mantle metasomatism can be produced by extensive reaction between peridotite and basaltic melt (Wulff-Pedersen et al., 1996
, 1999
; Neumann & Wulff-Pedersen, 1997
). The basaltic melt mainly dissolves the trace element-poor orthopyroxenes of the peridotites. Dissolution of significant amounts of wallrock opx might lead to elevated SiO2 contents in the melt, but the melt will not be silica-oversaturated and will not crystallize quartz in the upper mantle. Furthermore, dissolution of opx leads to dilution of incompatible trace element contents in the melt. Wulff-Pedersen et al. (1999
) have shown that migrating silicate melts with the highest SiO2 contents have concave (MREE-depleted) trace element patterns with marked positive anomalies of Ba and Sr. As interaction between peridotite and basaltic melt (1) does not produce qz, (2) dissolves but does not precipitate opx, and (3) produces trace element patterns of the melt that differ strongly from those observed in the MI of the studied xenolith (Fig. 6c–f), this process cannot be the source of the SiO2-rich melt.
In contrast, Arai et al. (2003
), Bianchini et al. (2004
) and Shimizu et al. (2004
) have described slab-derived qz-diorite veins cross-cutting peridotite xenoliths from Tallante, Spain. In these xenoliths, opx-rich bands developed at the boundary between peridotite and the qz-diorite vein, representing the reaction product of silicic melt and wallrock (Arai et al., 2003
; Shimizu et al., 2004
). During this reaction, olivine and clinopyroxene in the wallrock peridotite are dissolved. Olivine dissolution leads to orthopyroxene saturation in the SiO2-rich melt at the peridotite–melt interface, causing crystallization of orthopyroxene (e.g. Morgan & Liang, 2005
).
The above interpretation is consistent with phase relations in the fo–di–qz ternary at 2 GPa (Kushiro, 1969
). Experimental slab melts fall in the qz-in liquidus field (Fig. 7), so qz will crystallize first from silicic slab melts at mantle depths. In contrast, silicate melts formed by partial melting of peridotite are usually nepheline and olivine normative and fall in the ol-in liquidus field (Fig. 7). Thus, based on experimental data, the Mg/Si ratio in a continuously evolving slab–trondjhemitic melt will increase during hybridization and its composition will move first into the opx + liquid field and later to the opx + cpx cotectic line. A similar evolution is observed in natural adakites (Fig. 7). In the initial stage of hybridization, when the ratio of peridotite to SiO2-rich melt is low, a hybrid melt that is still silica-oversaturated could form and crystallize qz and opx as observed in the studied xenolith. This scenario requires a high melt/wallrock ratio, which would be maintained if the SiO2-rich melt migrated along fractures.
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Model calculations were carried out to estimate the ratio of slab melt and assimilated wallrock peridotite in the bulk composition of the studied xenolith (Fig. 7). The peridotite component was approximated using the modal and major element composition of a protogranular peridotite xenolith from the same location (Szt1017, reported by Downes et al. 1992
20 wt % of peridotite wallrock, in which the ratio of dissolved ol:cpx was 3:2 (Path B in Fig. 7). These parameters yield a cpx-free harzburgite wallrock after 30 wt % of assimilation. In the case of a significantly higher (4:1) cpx:ol dissolution ratio (Path C in Fig. 7), the reaction product will be cpx-rich. On the other hand, for such a high cpx:ol dissolution ratio, the calculations require a cpx-rich peridotite or pyroxenite for the assimilated wallrock, because the modal composition of the Szt1017 xenolith allows a maximum of 15 wt % of assimilation before cpx is completely dissolved. The high Ni and Cr concentrations in the pyroxenes and in the primary and secondary MI (Table 2) are also explained by dissolution of peridotite because mantle lherzolite contains high concentrations of these refractory elements.
Based on model calculations and petrographic evidence, the opx-rich composition of the studied xenolith can be explained by crystallization of qz + opx
qz + cpx from a hybrid melt that developed at the interface between peridotite and SiO2-rich melt after a small degree of peridotite assimilation. The hybrid melt predicted by the model calculation is SiO2- and Na2O-rich (
60 and
6 wt %, respectively), with moderate Al2O3 and low CaO contents (
15 and
4 wt %, respectively) and high mg-number (
75) (Fig. 8). It falls between the fields of peridotite partial melts (e.g. Falloon et al., 1997
; Gaetani & Grove, 1998
) and slab melts formed from metabasalts or metasediments (e.g. Rapp & Watson, 1995
; Rapp et al., 1999
; Hermann & Green, 2001
; Skjerlie & Patiño-Douce, 2002
) and is close to compositions of experimental hybrid melts (Rapp et al., 1999
) and natural adakites (Prouteau et al., 2000
; Sajona et al., 2000
); however, the mg-numbers of the experimental hybrid melts and natural adakites are lower (Fig. 8).
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Origin and significance of MI
Both heated and unheated primary MI trapped in opx have a restricted range in concentration of all major elements with the exception of MgO, FeO, mg-number and SiO2 (Table 1, Fig. 5). This variability is consistent with the varying degree of host mineral crystallization on inclusion walls after entrapment of the MI and, in the case of the heated inclusions, possibly the remelting of host mineral during the heating experiments. It is well known that, following the entrapment of MI, crystallization of the host mineral on the inclusion wall might be significant (e.g. Frezzotti, 2001
To test the effect of fractional crystallization on the trace element composition of the hybrid melt, various ratios of opx, cpx (with compositions determined in this study) and a hypothetical amp were added to the average MI composition to simulate a reverse fractional crystallization path. The trace element composition of the amp was estimated based on trace element partition coefficients between cpx and amp determined for peridotites by Ionov et al. (1997
).
Addition of opx does not change the MI trace element patterns; however, all trace element concentrations decrease with increasing opx incorporation (Fig. 9a). This means that opx fractionation alone did not control the trace element pattern of the hybrid melt. Amp addition, however, leads to a decrease in the strongly incompatible element concentrations, disappearance of the positive Pb anomaly, development of negative Hf, Zr and Ti anomalies, and an increase in HREE and compatible elements (Fig. 9b). Addition of cpx to the MI has an effect similar to amp; however, the negative Hf, Zr and Ti anomalies and the decrease in the strongly incompatible element concentrations are more significant (Fig. 9c). The results of this reverse fractional crystallization calculation suggest that opx, cpx and amp fractionation from the original hybrid melt might lead to (1) slight increase in strongly incompatible elements such as Cs, Rb, Th, U and Ba, (2) development of a positive Pb anomaly, (3) disappearance of the negative Hf, Zr and Ti anomalies, and (4) a decrease in Yb, Lu, Sc, V and Cr concentrations in the residual melt (Fig. 9d). Significant trace element compositional changes, however, are observed only if there is a high degree of fractionation of these minerals (above 50%) from the hybrid melt, which is not supported by the major element compositions (Fig. 8).
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Although the exact ratios of the fractionating minerals cannot be determined, the results suggest that the composition of the slab melt did not change significantly as a result of peridotite dissolution (assimilation) and fractional crystallization (Fig. 9d). Thus, the negative high field strength element (HFSE) anomalies, which are partially seen in the MI, as well as the negative Sr anomaly, are characteristic of the slab melt and not an artefact of hybridization. This interpretation is in accordance with the results of Rapp et al. (1999
Slab melt generation, source components
The MI preserve the trace element pattern of the slab melt and MI compositions can be used to approximate the formation conditions of the melt. The low contents of HREE (LaN/YbN = 85–134) and Y (5·4–6·3 ppm) in the primary MI (Fig. 6) suggest the presence of garnet (gt) in the source (e.g. Nicholls & Harris, 1980
). The low Nb and Ta concentrations, coupled with the negative Hf, Zr and Ti anomalies in the hybrid melt (Fig. 9d), imply rutile (ru) in the source (e.g. Green & Pearson, 1987
). Garnet and rutile are typical constituents of both metabasalts and metasediments in subducted oceanic crust. Several features of the trace element composition of the MI (Fig. 6) resemble those of adakites (Fig. 6d), which have been interpreted as products of eclogite melting (Kay, 1978
). However, the low Sr content of the MI (74–116 ppm) and high K/Na ratios, and large ion lithophile element (LILE) and LREE concentrations, are not typical for adakites (>400 ppm Sr) (Fig. 6d). These features suggest that another phase that retains Sr may have been present in the source during slab melt generation and also that the source may have been enriched in incompatible trace elements and/or the degree of partial melting was small.
Ratios of incompatible elements with similar bulk partition coefficients can be used to obtain information on the composition of the source, as these are neither dependent on the degree of partial melting nor modified by crystallization processes. As such, we used Th/Rb, K/Rb, Ba/La and Ce/Pb ratios to distinguish different source components. Characteristic ratios in the MI (Table 2) are shown in Fig. 10. Ba/La ratios plot close to primitive mantle (PM) and mid-ocean ridge basalt (MORB) values (Fig. 10a), suggesting that the melt was produced by melting of an eclogite with a normal (N)-MORB or enriched (E)-MORB composition. On the other hand, the Th/Rb, Ce/Pb and K/Rb ratios of the MI plot away from both MORB and PM. As K is significantly more compatible in amphibole compared with Rb, the presence of amphibole in the source is the most likely explanation for the low K/Rb ratios. Similarly, the Th/Rb ratio can also be shifted by melting in the presence of amphibole (Fig. 10c). The Ce/Pb ratio suggests involvement of another component, probably subducted sediment. The high La/Yb ratios can be produced by melting eclogite with a MORB composition only with a low degree of partial melting (<3%) (Fig. 10b). A higher degree of melting is possible (up to 20%) if a sedimentary component is also involved, because it is characterized by an elevated La/Yb ratio (Fig. 10b). These observations, combined with the high K/Na ratios, suggest a significant contribution of melt released from subducted metasediments.
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High-pressure and -temperature experiments suggest that during melting of a metabasaltic slab at relatively high temperature and low pressure (
950–1000°C and below 2·0 GPa), plagioclase (pl) is stable in the residuum with gt, cpx and amp (Springer & Seck, 1997
1·5 GPa, >900°C) might leave behind a gt + cpx + opx (+ pl) + qz resitite (e.g. Patiño-Douce & Beard, 1995
2·4) in the clinopyroxene. Furthermore, the composition of the local lower crust inferred from granulite xenoliths of metaigneous and metasedimentary origin (Embey-Isztin et al., 2003
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Crystallization conditions of the studied xenolith (
960°C and >1·1 GPa) are close to those suggested for release of silicic melt from a subducted slab (Fig. 11). This implies that the slab-derived silicic melt did not migrate far from its source before it crystallized and trapped MI in cpx and opx. We conclude that the studied qz-bearing opx-rich websterite was formed by reaction of a slab-derived siliceous melt with a mantle peridotite. Although we cannot estimate the initial composition of the slab melt with a high degree of accuracy, the trace element pattern and the volatile content of the MI suggest that melt generation occurred at a relatively shallow depth in the presence of garnet, amphibole, rutile and probably plagioclase in the residuum. The source composition cannot be unequivocally determined; however, major and trace element ratios indicate the probable involvement of a metasedimentary component.
The origin of secondary MI and interstitial silicate glass
The secondary MI are late-stage inclusions trapped in healed fractures in opx and cpx. Secondary MI-1 have compositions that are similar to the primary MI (Figs 5 and 6), although the fluid/melt ratio in secondary MI is much more variable than in primary MI (Fig. 2). This suggests that secondary MI-1 were trapped from a melt compositionally similar to that which formed the primary inclusions, precluding the infiltration of host basalt along healed fractures during uplift. It also suggests that the source of secondary MI is the same as that of the primary MI, and possibly that the source may be the primary MI themselves. After solidification of the websterite, which contained large primary MI, the mantle experienced lower-pressure conditions, which might have led to decrepitation of the largest MI and then heterogeneous closure of the released melt in secondary MI. The inferred decrease in pressure might have been associated with the formation of the Pannonian Basin during the Miocene.
Interstitial silicate glass shows a wider compositional range than was observed for the primary and secondary MI-1 (Fig. 4, Table 1). Highly siliceous glass was found between qz and opx, whereas the glass between opx and cpx is poorer in SiO2 and richer in other major elements. Thus, the composition of the interstitial glass was probably controlled by the surrounding mineral phases (opx + qz and cpx + opx, respectively). Basalt infiltration did not play a significant role in affecting the chemistry of the interstitial glass. Thus, we attribute the formation of the interstitial melt to an in situ melting episode that occurred during uplift in the host basaltic magma. Secondary MI-2 might have been trapped from these melts.
| CONCLUSIONS |
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Mineralogical, textural and compositional data presented here provide convincing evidence that quartz-bearing opx-rich rocks can be formed in the upper mantle. The observed mineral assemblage crystallized from a hybrid melt developed at the interface between peridotite and SiO2-rich silicate melt at about 960°C and pressure in excess of 1·1 GPa. The SiO2-rich melt represents a partial melt from a subducted slab of oceanic lithosphere. The melt was released from the subducted slab at
1·5–2·0 GPa and <1000°C, leaving behind a restite of cpx + amp + gt + pl/ap(?) + ru. The trace element composition of MI in both opx and cpx suggests the involvement of a metasedimentary component during slab melting. Melt inclusions in the studied xenolith provide direct evidence for the presence, migration and evolution of slab-derived SiO2-rich melts in the sub-continental lithospheric mantle. The results of this study also support the notion that metasomatized mantle can be transported by tectonic processes and rotations to place subduction-related rocks great distances from areas where subduction was known to have occurred (see Kovács & Szabó, 2007| ACKNOWLEDGEMENTS |
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The authors thank the members of Lithosphere Fluid Research Lab and Professor David Green (RSES, ANU) for fruitful discussions. The authors owe thanks to Professor M. Wilson, Professor Hilary Downes (Birkbeck College), Dr James Beard and an anonymous reviewer for their useful suggestions on an earlier version of this paper. This work was supported by OTKA K61182 and OTKA T043686 grants to K.T. and C.S. and by the Hungarian–American TET (Science & Technology Foundation) 17/MO/01 to C.S. This is Publication 28 in the series from the Lithosphere Fluid Research Lab at Eötvös University, Budapest.
*Corresponding author. Present address: Bayerisches Geoinstitut, Universität Bayreuth, Universitätsstraße 30, D-95447 Bayreuth, Germany. Telephone: +49 (0)921 155-3729. Fax: +49 (0)921 55-3769. E-mail: Eniko.Bali{at}uni-bayreuth.de
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