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Journal of Petrology | Volume 45 | Number 5 | Pages 975-1011 | 2004
Journal of Petrology 45(5) © Oxford University Press 2004; all rights reserved.
Geochemical Constraints for the Genesis of Post-collisional Magmatism and the Geodynamic Evolution of the Northern Taiwan Region
1 DEPARTMENT OF GEOSCIENCES, NATIONAL TAIWAN UNIVERSITY, PO BOX 13-318, TAIPEI 106, TAIWAN
2 ARC NATIONAL KEY CENTRE FOR THE GEOCHEMICAL EVOLUTION AND METALLOGENY OF CONTINENTS (GEMOC), DEPARTMENT OF EARTH AND PLANETARY SCIENCES, MACQUARIE UNIVERSITY, SYDNEY, N.S.W. 2109, AUSTRALIA
3 16 GIFFEN CLOSE, HOLT, CANBERRA, A.C.T. 2615, AUSTRALIA
4 DEPARTMENT OF PHYSICS AND EARTH SCIENCES, UNIVERSITY OF THE RYUKYUS, OKINAWA, JAPAN
5 INSTITUTE OF EARTH SCIENCES, ACADEMIA SINICA, PO BOX 1-55, NANKANG, TAIPEI, TAIWAN
RECEIVED NOVEMBER 14, 2002; ACCEPTED OCTOBER 21, 2003
| ABSTRACT |
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Taiwan is an active mountain belt created by the oblique collision of the northern Luzon arc with Asia. Late Pliocene extensional collapse of the northern Taiwan mountain belt (NTMB) was accompanied by magmatism that formed the Northern Taiwan Volcanic Zone (NTVZ; 2·80·2 Ma). The geochemical characteristics of the NTVZ magmas can thus provide constraints both for the mantle source composition and the geodynamic processes operating in the late orogenic stage of the region. The NTVZ volcanic rocks consist dominantly of calc-alkaline andesites and basalts, along with subordinate but heterogeneous lavas including low-K, shoshonitic and ultrapotassic magmas. From the NE to the SW in the NTVZ, the magmas show systematic compositional variations from low-K to calc-alkaline and then shoshonitic. This spatial geochemical variation, characterized by southwesterly increase in potassium and incompatible trace elements, appears to be subparallel to the southwestern part of the modern Ryukyu subduction system. SrNd isotope ratios of the NTVZ volcanic rocks (87Sr/86Sr
0·703760·70551; 143Nd/144Nd
0·512590·51301) suggest that two mantle source components are involved in the magma generation, the asthenosphere and metasomatized subcontinental lithospheric mantle. These two components are represented by the 2·6 Ma Mienhuayu high-Mg basaltic andesites and the 0·2 Ma Tsaolingshan high-Mg potassic lavas, respectively. The latter are interpreted to be the products of small-degree melting of a phlogopite-bearing, harzburgite lithospheric mantle source metasomatized recently by the nearby Ryukyu subduction zone processes. The SrNdPb isotope systematics and specific trace-element ratios of the NTVZ volcanic rocks suggest that melts derived from subducted sediments and fluids released from slab dehydration reactions were both involved in metasomatizing this mantle source. The unique spatial geochemical variation of the NTVZ volcanic rocks can be successfully modelled using variable degrees of partial melting of the mantle source regions, coupled with mixing of different melt components from depleted asthenospheric and metasomatized lithospheric mantle components beneath individual volcanic fields. It is inferred that mixing of melts from specific mantle components and the degree of partial melting are spatially and temporally related to the tectonic evolution of the northern Taiwan region, and not simply due directly to subduction zone processes. The overall NTVZ geochemical characteristics can be explained by various degrees of melting within an ascending region of the asthenospheric mantle, triggered by extensional collapse of the NTMB, and interaction of these melts with overlying fluid- and sediment-modified lithospheric mantle. KEY WORDS: Northern Taiwan Volcanic Zone; post-collisional magmatism; Pb isotopes; subduction components; geodynamics of basalt genesis
| INTRODUCTION |
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The tectonic evolution of orogenic belts is typically marked by changes in the composition of the associated magmatism (e.g. Harris et al., 1986
Taiwan is an active mountain belt created by the oblique collision between the northern Luzon arc and the Asian continent (see Teng, 1990
). Despite continuing plate convergence in central and southern Taiwan, extensional collapse has occurred in the northern part of the mountain belt since Plio-Pleistocene times. Accordingly, Teng (1996)
proposed a model for the orogenic evolution of northern Taiwan, from mountain building induced by collision to subsequent extensional collapse, lasting only a few million years. Wang et al. (1999)
proposed that post-collisional extension in the northern Taiwan mountain belt (NTMB) caused the magmatism of the Northern Taiwan Volcanic Zone (NTVZ) (Fig. 1). Compared with other collision orogens also characterized by extensional collapse (Dewey, 1988
; Platt & Visser, 1989
; Malavielle, 1993
), northern Taiwan may provide one of the most active examples of such a tectonic process. In this study, we aim to: (1) investigate the petrogenesis of the post-collisional magmatism, which displays distinctive spatial and temporal geochemical variations indicative of changes in magma source region; (2) explore metasomatism of the mantle source by different subduction components, e.g. hydrous fluids and subducted sediments; (3) track the evolution of the mantle source region during the late orogenic stage; (4) show how the geochemical trends within individual magmatic episodes can constrain the nature of geodynamic processes.
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| REGIONAL GEOLOGY: THE NTVZ |
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Located at the Asian continental margin at the boundary of the Philippine Sea plate, the island of Taiwan is not only a collision zone but also a transform region between the opposing Luzon and Ryukyu subduction systems (Fig. 1). The Ryukyu subduction and the resultant Ryukyu arctrench system, active since the Paleogene, are associated with the development of a back-arc basin, the Okinawa Trough, which has a distinct topography (>2000 m below sea level; Fig. 1) and a strong curvature. Driven by the NW movement of the Philippine Sea plate, the northern segment of the Luzon arc is generally believed to have collided with the Asian continental margin at 10 Ma (Teng, 1990
The NTVZ comprises two major onshore volcanic fields, the Tatun and Keelung Volcano Groups (TTVG and KLVG), and several offshore volcanoes (Fig. 1). The NTVZ volcanic rocks consist dominantly of andesites with calc-alkaline geochemical characteristics, similar to those commonly observed in convergent-margin lavas (e.g. Gill, 1981
). Thus, they have conventionally been regarded as the westernmost part of the Ryukyu volcanic arc (Chen, 1990
; Juang, 1993
; Chung et al., 1995b
; Teng, 1996
). The conventional view was first questioned by Chen (1997)
, who suggested an extensional rather than a subduction-related tectonic regime for magma generation. To accommodate available geophysical and geological evidence, Wang et al. (1999)
proposed that the NTVZ resulted from post-collisional extension related to the late Pliocene orogenic collapse of the NTMB. This extension may also account for the reactivation of the opening of the Okinawa Trough that commenced in the middle Miocene (Sibuet et al., 1995
) but became inactive after the arccontinent collision in Taiwan. Reactivated rifting in the Okinawa Trough started propagating to the SW from
1·5 Ma, with accompanying development of the westernmost part of the Ryukyu subduction system towards Taiwan (Chung et al., 2000
).
Radiometric age data show that the NTVZ volcanism commenced at
2·82·6 Ma and lasted throughout the Quaternary. Figure 2 summarizes existing age data for the NTVZ volcanic rocks, carried out by various dating methods including fission track, KAr and ArAr. The age data suggest that the earliest eruptions occurred in the Sekibisho (SBS) and Mienhuayu (MHY) islets and the TTVG around 2·82·6 Ma, with the youngest ages around 0·2 Ma in most of volcanic fields. In some localities, however, the volcanic ages might be younger than 0·2 Ma, as dating results are close to or even smaller than the limit of the dating methods. The age spectrum in Figure 2 shows a generally random distribution in space and time, distinct from the southwesterly younging trend of the NTVZ volcanism argued by some workers (e.g. Teng et al., 1992
; Teng, 1996
). This trend, based on limited geochronological data, was ascribed to southwesterly propagation of the Ryukyu subduction system (Teng et al., 1992
). However, when more recent age data (Juang, 1993
; Tsao, 1994
; Lee, 1996
; Wang et al., 2000
; Chung et al., 2001b
) are included, the alleged trend disappears (Fig. 2) so that the argument by Teng et al. (1992)
and Teng (1996)
is problematic.
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| SAMPLES AND ANALYTICAL METHODS |
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Samples and major-, trace-element and NdSr isotope methods
Representative volcanic samples were collected from different localities in the NTVZ for detailed geochemical investigation, including whole-rock major- and trace-element, and SrNdPb isotope determinations. Geochemical data for the SBS and Kobisho (KBS) volcanic rocks from Shinjo (1998
Powder samples were prepared using a jaw crusher and a corundum mill. Major-element compositions were determined by X-ray fluorescence (XRF) using a Rigaku® RIX 2000 spectrometer at the Department of Geosciences, National Taiwan University. The analytical uncertainties are generally better than 5% for all elements (Lee et al., 1997
). Loss on ignition was determined by routine procedures. Powdered samples weighing about 50 mg were dissolved using a HFHNO3 (10:1) mixture in screw-top Teflon Savillex® for 7 days at
100°C, followed by evaporation to dryness, refluxing in 7N HNO3 and drying again, and then dissolving the sample cake in 2% HNO3. An internal standard solution of 10 ppb Re was added and the spiked dissolutions were diluted with 2% HNO3 to a sample/solution weight ratio of 1/1000. The internal standard was used for monitoring the signal shift during inductively coupled plasma-mass spectrometry (ICP-MS) measurements using a Perkin Elmer® Elan-6000 spectrometer at Guangzhou Institute of Geochemistry, the Chinese Academy of Sciences, China, which has a good stability range within
10% variation (Liu et al., 1996
; Li, 1997
). Values recommended for the USGS rock standard BCR-1 (Govindaraju, 1994
) were used for data calibrations; the analytical errors are generally better than 5% for most trace elements. The samples were dissolved for Sr and Nd separation using routine cation-exchange column techniques. Sr and Nd isotope ratios were measured using VG354® and Finnigan MAT 262® mass spectrometers, respectively, at the Institute of Earth Sciences, Academia Sinica, Taiwan. Detailed chemical and mass spectrometric procedures were described by Chen et al. (1990)
. The isotopic ratios were corrected for mass fractionation by normalizing to 86Sr/88Sr = 0·1194 and 146Nd/144Nd = 0·7219. Long-term laboratory measurements for SRM 987 Sr and La Jolla (UCSD) Nd standards yield 0·71024 ± 0·00004 (2
) and 0·51187 ± 0·00003 (2
), respectively. During the period of the study, measurements for the NIST standard SRM 987 gave 86Sr/88Sr = 0·71023 ± 0·00001 (2
; n = 3), and for the La Jolla (UCSD) Nd standards gave 0·511867 ± 0·000006 (2
; n = 3). The overall blank contributions were 0·8 ng Sr for about 20 µg Sr and 0·3 ng Nd for about 0·6 µg Nd in the samples.
Double-spike Pb method
Chemical separation of Pb for isotope analysis was undertaken at the National Taiwan University, Taiwan and the University of the Ryukyus, Japan. Rock chips and/or powders were leached with 6N HCl at
80°C for 30 min. Then they were rinsed with distilled water before being decomposed with HF and HNO3. The Pb was separated using standard HBr anion exchange procedures in Teflon columns and the sample solution passed through the columns twice for purification. All chemical processes resulted in loss of about 50% of the Pb in chip samples and 90% in powders, respectively. Two small aliquots of the purified Pb sample were loaded onto two single Re filaments used for natural and double-spiked sample runs separately. A small drop of 207Pb204Pb double-spike solution and Pb emitter silica gelH3PO4 solution, prepared according to Gerstenberger & Haase (1997)
, were then added to the aliquot on the mix run filament. Repeated sucking back and release of the mixture with the loading pipette ensured a good samplespike mixture. Lead isotope measurements were made on a Finnigan MAT262® mass spectrometer using static multi-collector mode at the University of the Ryukyus, Japan. Data acquisition was usually performed at a filament temperature of about 10501150°C and consisted of four blocks of data per run, with each block comprising ten 16 s integrations (thus, 160 s integration time per block). Lead isotope ratios were corrected for mass fractionation by the use of a 207Pb204Pb double-spike method. A new 207Pb204Pb double-spike solution was prepared and calibrated in this study. The spike calibration is briefly described as follows.
The isotope composition of the newly prepared 207Pb204Pb double spike was calibrated with NIST Pb standard SRM 982. The standard had been measured in separate natural and mix runs with the new double spike for calibrating the isotopic compositions of the double spike. The isotopic compositions of SRM 982 in the natural runs (n = 22 in the period of analysis) were normalized to 208Pb/206Pb = 1·00016, a value recommended by Cameron et al. (1969)
and accepted in other Pb double-spike and triple-spike studies (e.g. Galer & Abouchami, 1998
; Thirlwall, 2000
). Data from these SRM 982 analyses and from double-spiked SRM 982 mix runs (n = 8) were then used to correct for mass fractionation effect and to determine the isotopic composition of the double spike. All calculations were performed by an iterative technique using an Excel spreadsheet (Woodhead et al., 1995
). The 204Pb/207Pb was determined to be
0·9921 in the newly prepared double-spike solution. Once the double-spike composition was calibrated it was tested by obtaining the isotope composition of NIST Pb Standard SRM 981 with the double-spike method. All mixed samples measured (n = 54) had Q
0·70·9 [Q = 204Pbspike/(204Pbspike + 204Pbsample)]. The double-spike calibrated SRM 981 has the following composition: 206Pb/204Pb = 16·9411 ± 42, 207Pb/204Pb = 15·4978 ± 52 and 208Pb/204Pb = 36·7185 ± 142 (2
), which agrees well with values recently reported by Galer & Abouchami (1998)
and Thirlwall (2000)
using triple-spike and double-spike methods, respectively. The external reproducibility of the SRM 981 (2SD, 54 analyses in the period of this study) is 124 ppm for 206Pb/204Pb, 112 ppm for 207Pb/204Pb and 96 ppm for 208Pb/204Pb. The overall blank contributions were 0·4 ng Pb for about 0·2 µg Pb in the samples. Accordingly, high-quality Pb isotope data were produced for this study using the double-spike method.
The major- and trace-element and SrNdPb isotopic compositions of the NTVZ volcanic rocks are presented in Tables 1 and 2, respectively.
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| WHOLE-ROCK GEOCHEMICAL COMPOSITION |
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Major-element compositions
In a plot of K2O vs SiO2 (Fig. 3a), most of the NTVZ volcanic rocks display calc-alkaline characteristics except for the SBS and MHY magmas, which are low-K, and the TLS magmas, which are shoshonitic. Volcanic rocks from the offshore volcanoes are principally mafic to intermediate, whereas the onshore volcano groups are intermediate to felsic. The mafic rocks (SiO2
55 wt %) from the various volcanic fields exhibit a trend of increasing K2O content and decreasing SiO2 content from NE to SW (Fig. 3a). In a plot of K2O vs Na2O (Fig. 3b), most of the NTVZ volcanic rocks have relatively high K2O contents, although only the TLS magmas have K2O contents higher than Na2O. The high K2O contents in some onshore volcanic fields with high SiO2 and Na2O contents may result from fractional crystallization; however, for some of the NTVZ mafic rocks fractional crystallization is not likely to be the reason for the high K2O contents (Fig. 3). As shown in Harker diagrams of CaO, Fe2O3(t), Al2O3, Cr, Sr and La vs MgO (Fig. 4), there is no significant trend of fractional crystallization for individual volcanic fields in the NTVZ, except for some onshore volcanic fields (TTVG and KYS).
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Some NTVZ volcanic rocks have high Al2O3 contents (
1720 wt %) and may be classified as high-Al basalts (e.g. Chen, 1990
0·5) in the NTVZ, whereas the MHY and TLS are relatively primitive magmas (Mg number = 0·6 and 0·8, respectively). The Mg number values for the MHY and TLS basalts are in equilibrium with the Fo contents of their olivine phencrysts (Fo = 81 and 90, resepectively) based on the calculation for olivineliquid equilibrium (Roeder & Emslie, 1970
Trace-element compositions
Mafic rocks from the individual volcanic fields in the NTVZ have distinctive trace-element characteristics. The TLS basalts have the highest compatible trace-element contents (Ni
500 ppm; Cr
1000 ppm). This characteristic, together with their major-element chemistry, is consistent with the TLS magmas being near-primary magmas. Incompatible trace-element characteristics are illustrated as chondrite-normalized rare earth element (REE) diagrams in Fig. 5 and as primitive mantle-normalized element diagrams in Fig. 6. The REE patterns of the NTVZ volcanic rocks are light REE (LREE) enriched, but the extent of enrichment is variable between the volcanic fields. The SBS and MHY mafic rocks have the lowest abundances of LREE and show relatively flat REE patterns, whereas the TLS basalts are the most LREE enriched. None of the REE patterns has an obvious negative Eu anomaly, which may indicate that plagioclase was not a fractionating phase in the NTVZ volcanic rocks.
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The primitive mantle-normalized trace-element patterns of the NTVZ volcanic rocks show significant enrichments in large ion lithophile elements (LILE) and LREE and a pronounced Pb spike (Figs 6 and 7a). Except for the MHY samples, which have relatively smooth trace-element patterns, all the NTVZ volcanic rocks have distinct high field strength element (HFSE; i.e. Nb, Ta and Ti) troughs in their patterns. The TLS magmas have the highest LILE contents, with Rb concentrations up to 2500 ppm, which is the highest reported value for terrestrial rocks (Chung et al., 2001b
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Notably, the MHY magmas do not show HFSE depletion but they show positive Pb spikes in the trace-element plots (Fig. 7b). Overall the trace-element patterns of the MHY magmas are similar to those of Miocene Taiwan intra-plate basalts (MTIB) in northwestern Taiwan (Chung et al., 1994
NdSrPb isotopic compositions
The TLS samples have the highest Sr isotope ratios (87Sr/86Sr
0·705400·70551) and lowest Nd isotope ratios (143Nd/144Nd
0·512590·51268). The MHY samples, however, have the most depleted Nd isotope ratios (143Nd/144Nd
0·512900·51301) similar to those of enriched mid-ocean ridge basalt (E-MORB; Sun et al., 1979
) and the South China Sea (SCS) seamounts (Fig. 8; Tu et al., 1992
), but more enriched than that of the Eastern Taiwan Ophiolite (ETO) representing the composition of the local mantle source of depleted MORB (Jahn, 1986
; Chung & Sun, 1992
). The isotopic composition of the SCS may represent the composition of the local mantle source of E-MORB (Tu et al., 1992
). Additionally, the MHY Nd isotope ratios are more depleted than those of typical arc and back-arc magmas in the nearby Central Ryukyu Arc (CRA) and Middle Okinawa Trough (MOT; Fig. 8; Wang, 1998
; Shinjo et al., 1999
). The MHY and some PCY Sr isotope ratios are slightly elevated so that the data plot to the right of the mantle array in the NdSr isotope diagram (Fig. 8). In terms of the Nd isotope composition, however, the other NTVZ volcanic rocks plot between the depleted MHY and enriched TLS samples. In the NdSr isotope diagram the overall data for the NTVZ show a distribution similar to that of the MTIB magmas, which have been interpreted to have originated by interaction of partial melts of ascending asthenosphere with the overlying sub-continental lithospheric mantle (SCLM) beneath the western Taiwan region (Chung et al., 1994
, 1995a
). The onshore NTVZ volcanic rocks have positive Nd model ages based on a depleted mantle reservoir (TDM
0·54·0 Ga; Table 2). The TLS magmas are unique in yielding positive ages that fall in a restricted range from 2·0 to 2·5 Ga. Other NTVZ volcanic rocks, which might have been the product of mixing of partial melts of different mantle source components, yield negative Nd model ages (not shown in Table 2).
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The NTVZ volcanic rocks have high 207Pb/204Pb and 208Pb/204Pb at a given 206Pb/204Pb ratio (Fig. 9), and all lie above the Northern Hemisphere Reference Line (NHRL) of Hart (1984)
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| DISCUSSION |
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In the following sections we consider specific aspects of the geochemical characteristics of the NTVZ volcanic rocks including spatial and temporal variations, the mantle source components involved in melt generation, and degrees of partial melting. To minimize the effects of fractional crystallization, the volcanic rocks from the KLVG [which are all intermediate to silicic in composition (SiO2
5558 wt %)] are excluded and only mafic rocks (SiO2 <54 wt %) are considered. Crustal contamination may be an important process in the petrogenesis of the volcanic rocks from the southwestern part of the NTVZ. However, as shown by a plot of 87Sr/86Sr vs SiO2 (Fig. 10a), it does not appear to have a major influence on the isotopic characteristics of the NTVZ volcanic rocks. In Fig. 10a the mixing line between the average composition of the Taiwan upper crust and the MOT basalt (assumed to have a similar mantle source to the NTVZ; see subsequent discussion) defines a steep slope, distinct from the variation trends for the individual volcanic fields in the NTVZ.
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Spatial and temporal geochemical variation in magma compositions
The spatial geochemical variation from NE to SW in the NTVZ volcanic rocks, expressed as an increase in K2O content, reduction in SiO2 content, and LILE and LREE enrichment (Figs 3 and 7a), suggests increasing involvement of an enriched mantle source component or decreasing degrees of partial melting in the petrogenesis of the most primitive mafic magmas. In terms of the SrNdPb isotope compositions (Figs 8 and 9), however, they do not show any systematic spatial variation. For instance, the KYS magmas have the second highest contents of K2O, LILE and LREE among the NTVZ (lower only than the highest TLS magmas; Figs 5, 6 and 7a), whereas they have relatively higher Nd and lower Sr isotope ratios compared with the other NTVZ volcanic rocks (Fig. 8). Thus, the NdSr isotope composition of the NTVZ volcanic rocks does not support a southwesterly increasing involvement of an enriched source component.
The La/Yb ratios in the NTVZ mafic rocks increase with La concentration (Fig. 10b) and also with NE to SW progression (Fig. 10c). This increase in the La/Yb ratios could not result from increased involvement of an enriched mantle source component because there is no supporting evidence from the NdSrPb isotope compositions. The La/Yb variation trend plots within that defined by partial melting of a local enriched MORB mantle source estimated for the MOT in the garnet and spinel facies (Fig. 10b; Table 3) and is not controlled by amount of the residual garnet. Consequently, the degree of partial melting in the NTVZ mantle source may play the dominant role in this chemical variation.
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The geochemical characteristics of the NTVZ volcanic rocks show not only a spatial variation but also a change with eruption age. Older (
2·82·6 Ma) volcanic rocks from the SBS and MHY are low-K (Fig. 3a), followed by the dominantly calc-alkaline series of the PCY and TTVG (
2·10·2 Ma), then finally by the recent (
0·2 Ma) high-K to shoshonitic volcanism of the KBS, KYS and TLS. The earliest SBS and MHY magmas have the lowest LILE and LREE abundances, whereas the youngest KYS and TLS magmas are extremely enriched in LILE and LREE. The PCY and TTVG magmas erupted at an intermediate time and show transitional abundances of the trace elements (Fig. 7a). The 143Nd/144Nd ratios of the earliest SBS and MHY magmas extend up to 0·51301; however, the youngest TLS magmas have the lowest 143Nd/144Nd ratio of 0·51260. Figure 10d shows that the highest Nd isotopic ratios occur in the earlier NTVZ magmas, and vice versa. These data indicate that in the mantle source region an enriched component became more important in the generation of the younger NTVZ magmas. In summary, the spatial variation of the NTVZ volcanic rocks reflects differences in the degrees of partial melting, whereas their isotopic change with time suggests changes in compositions of the mantle source components beneath the NTVZ.
Mantle source components
The asthenospheric mantle and subcontinental lithospheric mantle (SCLM) source components
The MHY and TLS magmas are the most two primitive melts in the NTVZ, which might shed light on the mantle source components. The TLS magmas are highly magnesian (MgO
15 wt %; Mg number
8083) and potassic (K2O
5 wt %; K2O/Na2O
1·63·0) with enriched LILE and LREE contents but relatively low basaltic components (i.e. Al2O3
12 wt %, total Fe2O3
7·5 wt % and CaO
7·5 wt %). They have the lowest Nd and highest Sr isotopic ratios among the NTVZ. Their overall geochemical characteristics are comparable with those of the Group I ultrapotassic rocks defined by Foley et al. (1987)
, such as orogenic lamproites from central Italy, Spain and Tibet. On this basis, Chung et al. (2001b)
suggested that the TLS magmas resulted from partial melting of a phlogopite-bearing harzburgitic source in the SCLM that underwent a recent metasomatism by subduction-derived fluids. Thus, an enriched SCLM is one of the potential mantle source components for the NTVZ volcanic rocks. The TLS Nd model ages also strongly suggest an SCLM origin. Nd model ages ranging from 2·0 to 2·5 Ga are consistent with ReOs model ages for sulphides in peridotite mantle xenoliths entrained by the MTIB (TRD
1·9
2·3 Ga; Wang et al., 2003
) indicating the presence of Proterozoic SCLM domains beneath northern Taiwan. On the other hand, the MHY magmas have high MgO contents (
5·98·1 wt %, Mg number
0·6) relative to SiO2 (
52·854·5 wt %), with moderate enrichment in LILE and LREE but no apparent HFSE depletion (Fig. 7b). They have high basaltic components (i.e. CaO
7·78·5 wt %, total Fe2O3
10·211·8 wt % and TiO2
1·41·8 wt %) reflecting a fertile mantle source. Although their elevated SiO2 contents (
52·854·5 wt %) could indicate fractional crystallization, the high-Mg characteristics of the MHY magmas suggest a primitive nature for these silica-saturated magmas (Wang et al., 2002
). These high-Mg basaltic andesites have the highest Nd isotope ratios and relatively elevated Sr isotopic ratios. The geochemical characteristics of the MHY magmas are similar to those of the MTIB magmas in northwestern Taiwan (Chung et al., 1994
, 1995a
) and almost the same as those of high-Mg andesites from Iriomote-jima, southern Ryukyus (Shinjo, 1999
; Fig. 7b); both are considered to be examples of intra-plate volcanism caused by extensional tectonic activity on the Asian continental margin in the Miocene. Similar to the most depleted SCS and NTIB samples (Tu et al., 1992
; Chung et al., 1994
, 1995a
), the MHY lavas have high Nd isotopic ratios (143Nd/144Nd
0·512900·51301), which suggest a similar mantle source to the local enriched asthenospheric mantle. This source is not the same as the SCLM that produced the TLS magmas. It is also difficult to ascribe the MHY magmas to an SCLM source because such a source with a Nd isotopic ratio of up to
0·51301 is probably too refractory to produce the high degree of partial melting required for the MHY magmas (Fig. 10b). Thus, Wang et al. (2002)
suggested that the MHY magmas were derived from an asthenospheric mantle source with E-MORB characteristics. The high Sr isotopic ratios (87Sr/86Sr
0·704380·70453; Wang et al., 2002
) of the MHY magmas are inferred to be derived by fluxing of aqueous slab fluids with no sedimentary components into the mantle source region. This process is analogous to that suggested for the petrogenesis of some island arc tholeiites in the South Sandwich and the IzuBoninMariana arcs (e.g. Pearce et al., 1995
; Taylor & Nesbitt, 1998
).
Subduction components
The inferred mantle source components for the NTVZ magmas, the SCLM and the asthenospheric mantle, are both interpreted to be metasomatized by subduction components. In terms of SrNdPb isotope compositions (Figs 8, 9 and 11a), the involvement of a sedimentary component in the mantle source region for the NTVZ magmas is strongly indicated. Using mantle xenoliths entrained within the Miocene intra-plate basalts in northwestern Taiwan and southeastern China as samples of the SCLM with no recent subduction metasomatism, mixing calculations based on their NdSr isotope compositions show that 3% subducted sediments would need to be added to the unmetasomatized SCLM to yield a possible source for the TLS magmas (Table 4; Fig. 11b). A depleted mantle source infiltrated by varying amounts of sediment-derived melts may explain the compositional trend for the NTVZ magmas in the NdSr and PbPb isotope diagrams (Figs 8 and 9). However, there is no systematic SrNdPb isotopic variation within the NTVZ distribution paralleling the present-day Ryukyu Trench and a variable sediment flux into the mantle source is difficult to conceive. In addition, the high Nd and Sr isotopic ratios for the MHY magmas and specific incompatible element ratios in the TLS magmas, e.g. Nb/U
0·8, Ce/Pb
2, Rb/Cs
8 and Ba/Rb
1, are not consistent with simple source sediment contamination. Chung et al. (2001b)
suggested that another type of non-magmatic enrichment is required. On the basis of mineralaqueous fluid experiments (Keppler, 1996
; Tatsumi & Kogiso, 1997
; Ayers, 1998
), we suggest this enrichment agent to be a hydrous fluid derived from the subducting slab. The distinction between sediment melt and slab-derived fluid is clearly shown by a Nb/La vs Ba/Rb plot (Fig. 12).
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Whereas the MHY magmas, with their distinct E-MORB affinity (Nb/La
1), reflect an origin from an asthenospheric source, the TLS and other NTVZ volcanic rocks with Nb/La <1 can be interpreted to be derived from an SCLM altered by subduction-related metasomatism. The TLS magmas have extremely low Ba/Rb ratios, which indicate fluid-dominated metasomatism of the source rather than sediment melting as shown by the other NTVZ volcanic rocks. As the slab-derived fluid has similar 143Nd/144Nd ratios to MORB but with unique specific trace-element ratios, and the sediment melt displays lower 143Nd/144Nd ratios with different trace-element ratios, plots of Nb/U and Ce/Pb vs 143Nd/144Nd can discriminate the extent of involvement of both subduction components in the metasomatism (Table 4; Fig. 13).
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The average composition of the continental sediments on Taiwan was chosen to represent that of the subducted terrigenous sediments (Lan et al., 1990
Other evidence for fluid-dominated metasomatism of the mantle source might come from generation of high-Al basalts in the NTVZ. High-Al basalts have been considered to be primary melts from large degrees (
5060%) of partial melting of eclogites in subducting plates (e.g. Brophy & Marsh, 1986
; Myers et al., 1986
). However, considering the difficulty of deriving large-degree partial melts from the old and cold subducting Philippine plate (
45 Ma) in the Ryukyu subduction system, high-Al basalts in the NTVZ are most likely to be the result of fractional crystallization rather than representing primary melts. Alternatively, Gaetani et al. (1993)
pointed out that the presence of water in the mantle wedge above a subduction zone can significantly alter the compositional path followed by residual liquids, and modify the types and compositions of crystals that accumulate at the site of cooling. Accordingly, under hydrous conditions, early crystallization of plagioclase is suppressed so that aluminium contents in residual liquids increase to yield high-Al basalts (Fig. 14a). Figure 14b shows that most of the NTVZ volcanic rocks lie along the olivine clinopyroxene cotectic for hydrous crystallization. This suggests that their mantle source region might be hydrous. The SBS lavas, all high-Al basalts, plot closest to the olivineclinopyroxeneplagioclase ternary eutectic, indicating that high-Al basalts in the NTVZ are not primary melts but have undergone some fractional crystallization.
|
In comparison with the MTIB in northwestern Taiwan erupted prior to the Taiwan arccontinent collision (Chen, 1990
10 Ma (e.g. Teng, 1990
The mixing of mantle source components and partial melting conditions
The mixing trend in Fig. 13 also suggests that mixing of partial melts of enriched asthenospheric mantle and subduction-metasomatized SCLM could explain the geochemical characteristics of the NTVZ volcanic rocks. Although the MHY magmas have lower values than the P-ETO, they still plot at the other end of the mixing trend (Fig. 13a). The MHY mantle source might have been fluxed by slab-derived fluid but not sediment melts, so their Ce/Pb ratios are much lower (Fig. 13b). The effect from the slab-derived fluid is not clear for Nb/U probably because the MHY magmas have higher Nb contents similar to E-MORB. A similar mixing trend is observed in the NdSr isotope diagram (Fig. 8), in which the other NTVZ volcanic rocks lie along a mixing trend between the depleted MHY and enriched TLS mantle sources despite the elevated Sr isotopic ratios of the MHY magmas. A simple source sediment contamination model is not preferred because variable sediment flux in the NTVZ mantle sources unrelated to NTVZ distribution would be highly unlikely to lead to systematic isotopic variation among the NTVZ. Alternatively, we propose that variable mixing of melts from the depleted asthenospheric mantle at the site of formation of the MHY magmas, and the subduction-metasomatized SCLM where the TLS magmas formed could satisfy most of the geochemical characteristics of the NTVZ magmas. The proportions of the melts from the metasomatized SCLM mixing with asthenospheric melts can be calculated based on the NTVZ NdSr isotopic ratios: 1217% for the SBS,
20% for the KBS,
13% for the PCY,
30% for the TTVG and
20% for the KYS, respectively (Fig. 8), using compositions of the MHY and TLS magmas as the two end-members. In the calculation, the most enriched Sr isotope value of E-MORB (87Sr/86Sr = 0·70308; Sun et al., 1979
) instead of that of the MHY magmas was used because the MHY magmas have elevated Sr isotope ratios as a result of subduction-fluid flux. The degree of partial melting also plays an important role in controlling the spatial geochemical variation among the NTVZ, which the simple source sediment contamination model can not decipher.
The mantle xenoliths entrained within the MTIB are dominantly refractory harzburgites (Yang et al., 1987
), so this part of the SCLM is not a productive magma source. Whereas the fluid-dominated metasomatism substantially lowers the solidus temperature of the refractory SCLM, the TLS magmas, indicative of the most fluid-dominated metasomatized SCLM source, still show extremely low degrees of partial melting. Using the Batan sub-arc phlogopite-bearing harzburgites from the Philippines (Maury et al., 1992
) (which are the analogue of the TLS mantle source and generated similarly high-K magmas) as the starting source material in the graphical concentration ratio (CR) method of Maaloe (1994)
, <2% of partial melting is estimated for the TLS magmas (Table 3; Fig. 15). Thus, except for the MHY and TLS magmas, which are separately derived from the asthenospheric and lithospheric mantle, most of the NTVZ magmas are the products of variable degrees of partial melting of asthenospheric mantle, variously contaminated by melts from the metasomatized SCLM during ascent.
|
The degrees of partial melting for the NTVZ can be evaluated by the CR method using an enriched MORB mantle source as the starting source material, which is estimated from basalts in the MOT with a subduction flux similar to that for the MHY magmas (Table 3; Fig. 15). We suggest that the parental magmas of the offshore volcanic fields in the NTVZ were generated by larger degrees of partial melting (820%) than the onshore fields (25%). A southwestward decrease in degree of partial melting is also revealed, which is evident in the plot using dominantly mantle-derived elements or conservative elements (e.g. Nb and Yb; Pearce & Parkinson, 1993
Petrogenetic model
To test our hypothesis, modelling of trace-element concentrations in the mantle sources and melts was carried out. Non-modal batch melting was assumed and the compositions of the mantle sources for the MHY and TLS magmas were used as starting points. As Wang et al. (2002)
suggested that asthenospheric mantle ascended to
6070 km depth to generate the MHY magmas at
2·6 Ma, we assume that all melts, including the TLS melts from the SCLM, occur in the garnet stabilizing field of the mantle. Using the trace-element partition coefficients of Halliday et al. (1995)
, Johnson (1998)
and Schmidt et al. (1999)
, the trace-element compositions of the MHY and TLS mantle sources were calculated from the average lava compositions using the estimated degrees of partial melting shown in Fig. 15 (8% for the MHY and 2% for the TLS), and appropriate source and melt modes (garnet lherzolites for the MHY and phlogopitegarnet harzburgites for the TLS; see Table 5 for details). Having thus established the trace-element compositions of the enriched asthenospheric and metasomatized SCLM source components, the trace-element composition of the asthenospheric melts can be derived for the individual NTVZ volcanic fields. Finally, a simple mixing calculation based on the estimated compositions of the asthenospheric melts and those from the metasomatized SCLM, using the proportions shown in Fig. 8 for the individual NTVZ volcanic fields, provides their model trace-element compositions. The model trace-element compositions are plotted in Fig. 16 compared with the actual compositions of the NTVZ magmas (except for the MHY and TLS magmas used as end-members). Although the model compositions for the NTVZ do not perfectly coincide with their actual values in Fig. 16, the geochemical variation trends of the NTVZ magmas are successfully modelled by this method.
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| GEODYNAMIC MODEL |
|---|
|
|
|---|
Wang et al. (1999)
Models involving a retreating subduction zone (e.g. Lonergan & White, 1996
), slab detachment or break-off (e.g. Davies & von Blankenburg, 1995
), delamination (e.g. Bird, 1979
) and convective removal of the lithosphere (e.g. Houseman et al., 1981
) have been used to explain post-collisional extension. All these processes cause upwelling of the asthenosphere and this will perturb the original thermal gradient. Consequences that follow are magma generation and sequential extension. Combining the magmatic history with other constraints based on the tectonic evolution of an area may lead to a more robust dynamic model (e.g. Turner et al., 1999
).
Relative to the present-day location of Taiwan, the initial arccontinent collision started in the NE at
10 Ma and propagated southwestward corresponding to the relative motion between the Philippine and Eurasian plates (Suppe, 1984
). According to the sedimentary record (Teng, 1990
), the collision activity was most intensive at
65 Ma, resulting in an uplift of nearly 4000 m above sea level (Fig. 1). Meanwhile, both the arc and associated back-arc volcanism in the middle part of Ryukyu subduction experienced a hiatus in the period of 62 Ma (Letouzey & Kimura, 1986
; Kamata & Kodama, 1994
; Park, 1996
). This indicates a feedback relationship between the Taiwan collision and the development of the part of the Ryukyu subduction system near northern Taiwan.
Severe compressional forces near the northern Taiwan region probably stalled the Philippine Sea plate subduction so this slab could not encroach beneath the region. Consequently, the Ryukyu subduction re-established and re-generated arc and back-arc volcanism at a later stage. Two phases of the Okinawa Trough opening at 106 and
2 Ma (Miki, 1995
; Sibuet et al, 1998
) may respond to the re-establishment of the Ryukyu subduction system. The thickened lithosphere caused by arccontinent collision would have also prevented western propagation of the Ryukyu subduction system (Fig. 17a). This model differs from previous ones suggesting that the Ryukyu subduction zone was able to continue developing in the northern Taiwan region (Chen, 1990
; Teng et al., 1992
; Teng, 1996
).
|
Several lines of evidence also support the interpretation that the NTVZ is unlikely to be part of the Ryukyu Arc. They include a horizontal displacement (of about 150 km) from the western end of the actual Ryukyu volcanic arc (Iriomotejima; Fig. 1) to the NTVZ, and the fact that the north-dipping Benioff zone of the subducting Philippine Sea plate is now sitting
200250 km beneath the NTVZ (Eguchi & Uyeda, 1983
100 km for the normal Ryukyu Arc. There are apparent differences in the duration of volcanism between the NTVZ and the Ryukyu Arc, as the latter became dormant in the earliest Pliocene (Shinjo, 1998
The geochemical characteristics of the MHY asthenospheric melts indicate that significant upwelling of asthenosphere to 6070 km depth has occurred since
2·6 Ma (Wang et al., 2002
) at the time of initiation of the NTVZ activity (Fig. 17b). Taking account of the continental crustal thickness of
30 km in northern Taiwan (Yeh et al., 1989
), emplacement of the MHY magmas suggests that part of the SCLM was removed or thinned to let the underlying asthenosphere upwell to sufficiently shallow depths for decompressional melting to occur. Because the collision started to the NE of present-day Taiwan close to the MHY, this is inferred to have been the region of thickest lithosphere, and most likely to be removed subsequently, similar to the scenario described for Tibetan post-collisional magmatism by Turner et al. (1996)
. Actually the NTVZ distribution along the underlying northern Taiwan metamorphic basement, which represents parts of the Taiwan orogen and is characterized by folded and tilted Tertiary strata resulting from the collision (Fig. 1; Wageman et al., 1970
; also named the southern TaiwanSinzi Folded Zone), strongly suggests a link between generation of the NTVZ and collapse of the Taiwan orogen. Seismic profiles show that offshore northeastern Taiwan has been characterized by high-angle normal faults, which have been reactivated from pre-existing, collision-induced reverse faults, since late Pliocene times (Hsiao et al., 1998
; Kong et al., 2000
; Fig. 1). On this basis, Teng (1996)
proposed that extensional collapse of the NTMB took place in Plio-Pleistocene times. The uplift history revealed by the Taiwan basement rocks and sedimentary accumulation in the foreland basins suggests that there was a major acceleration in the rate of uplift of the arccontinent collision zone and an increase in the sediment accumulation rate at
32·5 Ma, following steady-state uplift since
8 Ma (Teng, 1990
, fig. 8). This supports a model of rapid uplift after parts of the SCLM were removed or attenuated.
The SBS, TTVG and later PCY (
2·1 Ma) magmas show HFSE depletion (Fig. 7a), indicating a likely greater involvement of subduction components in the metasomatized asthenospheric mantle and/or the SCLM. The SBS and PCY magmas, both offshore and close to the MHY field, are also low-K and calc-alkalic magmas produced by higher degrees of partial melting and with higher 143Nd/144Nd (
0·512840·51289 and 0·51289 0·51297, respectively). The TTVG magmas are calc-alkaline and have lower 143Nd/144Nd (
0·51268 0·51280). The correlation might suggest that upwelling of the asthenosphere was shallower offshore, so that higher-degree asthenospheric melts were generated with less contamination by the overlying metasomatized SCLM, and vice versa (Fig. 17b). As a result of the continuing collision in central and southern Taiwan, post-collisional extension induced by asthenosphere upwelling diminished southwestward.
Magmatism during the initial stage of NTVZ activity was dominantly sourced from the asthenospheric mantle (i.e. the MHY, SBS and PCY). These magmas represent higher degrees of partial melting (820%) consistent with that predicted from decompressional melting of the ascending asthenosphere up to
6070 km depth (1020%). Some extensive late PlioceneQuaternary subsurface magmatic fields distributed within the Taiwan orogen basement have been identified on seismic profiles (Fig. 1; Sun & Hsu, 1991
; Hsiao et al., 1998
). The volume of these subsurface volcanic fields is apparently larger than the NTVZ although no direct age and geochemical data for the magmatic rocks are available. However, it is evident that large amounts of volcanic activity have occurred offshore northeastern Taiwan since the late Pliocene.
After
2·6 Ma the subducting Philippine Sea plate resumed its westward motion to penetrate progressively into the region beneath the NTMB because parts of the collision-thickened lithosphere that were creating a barrier had been removed (Fig. 17c). Meanwhile, the Ryukyu subduction system developed its southernmost extension corresponding to the movement of the Philippine Sea plate. The reopening of the Okinawa Trough started at
2 Ma after a hiatus (Letouzey & Kimura, 1986
; Park, 1996
; Sibuet et al., 1998
), and its fast southwestward propagation at
126 mm/yr reached the I-Lan plain, in NE Taiwan (Liu, 1995
) with a very strong curvature. This part of the Okinawa Trough [named SPOT (southernmost part of Okinawa Trough) by Chung et al. (2000)
] is structurally and geochemically different from its central part. The SPOT back-arc magmas are bimodal andesites and rhyolites, exhibiting typical subduction magma-type characteristics similar to those of the CRA and MOT magmas (Chung et al., 2000
). Compared with the MHY magmas with intra-plate geochemical affinities, it is most likely that initial magmatism first occurred within the NTVZ outside the topographical Okinawa Trough, rather than within the trough.
The NTVZ magmas erupted from 2 to 1 Ma consist dominantly of calc-alkalic rocks and display significantly HFSE depletion (Fig. 7a) in contrast to the earlier NTVZ magmas with low-K characteristics. These were widely emplaced at the PCY, KLVG and TTVG localities (Fig. 17c), which extend onshore from an inferred upwelling centre offshore. Greater enrichment in LILE and LREE than the earlier magmas suggests that the proportion of lithospheric components was increasing (Fig. 7a). All phenomena at this stage indicate that subsequent thermal perturbation in the SCLM and the propagation of extension followed asthenospheric upwelling.
The final stages of volcanism show most activity in the KBS, PCY, TTVG, KYS and TLS fields (Fig. 17d) with striking geochemical variations in the magmas. The most recent (
0·2 Ma) magmas at KBS, KYS and TLS have high-K calc-alkaline to shoshoniticultrapotassic characteristics with extreme enrichment in LILE and LREE but HFSE depletion (Fig. 7a). The TLS magmas represent an extreme end-member magma type indicative of small-degree partial melts of phlogopite-bearing harzburgitic SCLM. A series of recent volcanic arcs, about 80100 km above the Benioff zone of the subducting Philippine plate, and representing the western end of the Ryukyu Arc, were formed in the SPOT (Sibuet et al., 1998
; Chung et al., 2000
). The SPOT is an atypical back-arc spreading setting, which was formed before or at least synchronously with its arctrench counterpart (Fig. 17d; Wang et al., 1999
; Chung et al., 2000
). This combination of tectonic and magmatic processes consequently led to a unique collisionextensionsubduction context in this region. Sadeghi et al. (2000)
reported low-velocity anomalies in the uppermost mantle at a depth of 40 km beneath the northern Taiwan region, but beyond the SPOT area, and these might be evidence for the asthenosphere upwelling in the NTMB.
Most models for post-collisional magmatism predict that it should progress from potassic lithosphere-derived melts to intra-plate asthenospheric melts with time (e.g. Pearce et al., 1990
; Turner et al., 1992
, 1993
, 1996
; Platt & England, 1993
; Maheo et al., 2002
). However, Turner et al. (1999)
reported that post-collisional magmatism in the BeticAlboran domain in SE Spain exhibits the reverse progression and suggested that this could be due to significant differences in the amount of thickened crust in different collision zones. A general model was proposed for post-collisional magmatism in Tibet where the thickened crust (
70 km) is twice normal thickness. However, the BeticAlboran domain may not have had such thickened crust, so that the asthenosphere could upwell to higher levels (e.g. less than 5060 km) after convective removal of some of the thickened lithosphere and thus induce decompressional melting to generate asthenospheric melts first (Turner et al., 1999
). Thus, the rheology of both plates in collision, the extent of the collision and the velocity of plate convergence are important controls on the geochemical characteristics and time interval between the onset of collision and the generation of post-collisional magmatism. In the northern Taiwan region we also observe a reverse geochemical pattern for magma suites starting with asthenospheric melts then proceeding to lithospheric melts. The scale of the collision in the Taiwan region is much smaller than that in Tibet, so it is easier to document in detail the different successive magma series within a short time span from the onset of collision in the NTVZ, thus providing constraints for a post-collisional magmatism in a distinctive geodynamic domain similar to that of the BeticAlboran domain.
| CONCLUSIONS |
|---|
|
|
|---|
The geochemical characteristics of the NTVZ volcanic rocks indicate that they resulted from the upwelling of asthenosphere in response to post-collisional extension associated with collapse of the NTMB in Plio-Pleistocene times. Their spatial and temporal geochemical variation can be explained and semi-quantitatively modelled by variations in degrees of partial melting, and in the mixing proportions of two dominant end-member source mantle types beneath individual magma fields, which may be distinguished in terms of their geographical location and age of volcanism. The spatial variation of the NTVZ volcanic rocks largely reflects partial melting variations, whereas the changes in isotopic composition with time suggest changes in the compositions of the mantle source components beneath the NTVZ.
The dominant mantle components are the asthenospheric mantle and the SCLM that had undergone metasomatism by subduction processes associated with the Ryukyu subduction system. The subduction-related metasomatism of the SCLM has geochemical characteristics indicating the involvement of both slab-derived fluid and sediment-derived melts that infiltrated the mantle source region of the NTVZ during the build-up of the NTMB. Thus, the arc signatures evident in most of the NTVZ volcanic rocks do not mean that the NTVZ is part of the Ryukyu Arc, as these are not direct melts induced by subduction processes, but extension-induced melts formed significantly after active subduction ceased and that were contaminated by the overlying SCLM (which had inherited subduction components). The retreating subduction zone and slab detachment or break-off models are unlikely to be able to explain the generation of the NTVZ volcanic fields.
It is suggested that the MHY melts represent asthenospheric melting after parts of the thickened lithosphere had been removed (or attenuated) and asthenosphere upwelling took place to shallow depths (
6070 km). Subsequent emplacement of calc-alkaline magmas indicates increasing involvement of the SCLM in the magma generating process resulting from heating by the newly juxtaposed hotter asthenosphere. Finally the TLS potassic magmas erupted as a result of melting dominantly of the metasomatized SCLM itself. The NTVZ magma series progression is distinct from that predicted by general models for post-collisional magmatism based on the Tibetan post-collisional magmatism, but similar to that of the BeticAlboran domain. This may be a consequence of the different scales of these collision zones.
| ACKNOWLEDGEMENTS |
|---|
We thank C. Y. Lee and X. H. Li for their help in arranging XRF and ICP-MS analysis, and C.-H. Chen, F. T. Yang and C.-H. Lo at NTU, T. Y. Lee at NTNU, Taiwan, and M. Zhang at GEMOC, Macquarie University, Australia, for thoughtful discussions. Thanks also go to R. Maas of Melbourne University for supplying silica gelH3PO4 solution, and to G. Mortimer of ANU, RSES, for supplying SRM 981 and 982, the ANU double-spike solution and the Excel spreadsheets for double-spike calculation in the early stage of this work. The manuscript was significantly improved by constructive journal reviews from Y. Tatsumi, S. Turner, H. Williams, an anonymous reviewer and the Editor M. Wilson. This study benefited from research grants supported by the National Science Council, Taiwan. Refining of concepts and writing was done while K.-L. Wang was in receipt of a Macquarie University Research Fellowship. This is GEMOC Publication 335.
| FOOTNOTES |
|---|
* Corresponding author. Present address: GEMOC, Department of Earth and Planetary Sciences, Macquarie University, Sydney, N.S.W. 2109, Australia. Fax: 61-2-9850 8943. E-mail: kwang{at}els.mq.edu.au
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