Karsten M. Haase
Christoph Beier
Fabian Kemner- GeoZentrum Nordbayern, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Erlangen, Germany
The interaction of deep mantle plumes with lithospheric plates is one fundamental concept of plate tectonics. Based on observations mainly made on the Hawaiian volcanoes the compositional evolution of hotspot volcanoes is believed to reflect the variation of partial melting and source composition as the plate moves across the different melting zones of the mantle plume. The model predicts the formation of several magmatic stages that differ in composition. In order to test this model, we compare published compositional and age data from the intraplate volcanoes of the Hawaii, Society, Marquesas and Samoa hotspots on the older part of the Pacific Plate. The compiled data indicate that most volcanoes display variations within and between several magmatic series, and in most cases the more evolved lavas are associated with the voluminous shield stage. The Hawaiian volcanoes show up to four different series ranging from tholeiites to nephelinites/melilitites, whereas the other hotspots mainly erupt two magmatic series consisting of transitional basalts and basanites. Submarine preshield stages at the Society and Marquesas hotspots resemble those observed at Hawaii. The large variation of primitive magmas in the Hawaiian plume as opposed to the other Pacific intraplate systems may reflect the higher temperatures, higher buoyancy flux, and extreme chemical heterogeneity at Hawaii. The shield stage activity at all four hotspots lasts for 1 million years indicating similar widths of the melting zone, although the temperatures of the distinct mantle plumes vary considerably. The relatively depleted shield stage magmatism typically overlaps by ~200 kyrs with the formation of the more enriched postshield magmas indicating that the two melting and magma ascent systems exist contemporaneously.
Introduction
One of the fundamental features of the plate tectonic model is the interaction of lithospheric plates with so-called hotspots or melting anomalies that are likely caused by deep mantle plumes (Wilson, 1963; Morgan, 1971). Recent models suggest that there are different source regions from which deep mantle plumes ascend. They may either rise directly from the core-mantle boundary or from large low-velocity regions in the lower mantle (e.g., Courtillot et al., 2003; Jellinek and Manga, 2004; French and Romanowicz, 2015). The underlying assumption is that, during the period of most voluminous eruptions of the so-called shield stage, the active volcanic system is situated above the center of the melting anomaly providing the required excess heat, anomalously fertile (pyroxenite) rich mantle, and/or volatiles causing melting (e.g., Liu and Chase, 1991; Putirka et al., 2007; Herzberg and Asimov, 2008; Hofmann and Farnetani, 2013). As the plate moves across the mantle plume the degree and source of partial melting vary, leading to chemical and isotopic variations in the magmas feeding the volcanoes (Frey et al., 1990; Woodhead, 1992). Thus, age-progressive volcanic chains are formed with life-times of up to 80 million years (Duncan and Richards, 1991; Clouard and Bonneville, 2005) and, in some cases even exceeding 90 million years, e.g., at the Louisville seamount chain (Koppers et al., 2011). Within many of these chains the volcanoes seem to show a systematic compositional evolution ranging from tholeiitic to alkaline basalts with decreasing age (McDougall and Duncan, 1980; Woodhead, 1992). This magma evolution model is largely based on the Hawaiian volcanic chain because the Hawaii-Emperor Chain represents the best-studied plume track globally both from the subaerial and submarine edifices. According to the observations on the Hawaiian volcanoes four different magmatic stages were postulated to exist in intraplate volcanoes; (1) a preshield stage. (2) a shield stage. (3) a postshield stage, and (4) a rejuvenated stage (Clague and Dalrymple, 1987; Frey et al., 1990). The eruptive volumes increase through the preshield stage and reach a maximum during the shield stage when 80 to 95% of the entire volume of the volcano is produced. After the shield stage the erupted volumes decrease leading, in some cases, to several million years of volcanic quiescence before small volumes of lavas may erupt during the rejuvenated (or posterosional) stage (Clague and Dalrymple, 1987; Frey et al., 1990). The distinct Hawaiian eruption stages have been recently questioned because they are mainly based on subaerial sampling and volcanic evolution, and do not reflect gradual changes in magma compositions (Clague and Sherrod, 2014). According to the model, the magma composition of the hotspot volcanoes varies from highly SiO2-undersaturated preshield alkaline basalts to tholeiitic shield basalts and then again to alkaline SiO2-undersaturated postshield lavas. The mantle plume model suggests that the different stages reflect the different parts of the mantle plume. Little is known about the preshield stage because these lavas are probably covered by the later voluminous shield lavas, but this early stage indicates the arrival of the lithospheric plate at the edge of the melting anomaly. Increasing degrees of partial melting occur as the lithosphere moves across the mantle plume with the shield stage representing the largest degrees of melting in the plume center and the most voluminous volcanism. As the plate continues to move over the plume the degree of melting decreases during the postshield stage. The generation of the highly SiO2-undersaturated posterosional or rejuvenated stage magmas is not well-understood because many of these magmas form several million years after the plate passed the mantle plume (Garcia et al., 2010; Konter and Jackson, 2012). The duration of the shield stage and the composition of the magmas yield important insights into the composition, temperature and structure of the mantle plume and the melting processes. Additionally, the determination of the absolute plate velocities relative to mantle plumes depends on the understanding of the composition and duration of the shield stage (McDougall and Duncan, 1980). However, so far there has been little effort to compare the shield stages of volcanoes from different hotspots in order to define potential similarities and differences (Woodhead, 1992). Most recent studies have concentrated on the definition of mantle sources using radiogenic isotope compositions (e.g., Hofmann, 2003; Jackson and Dasgupta, 2008; White, 2010) but did not take into account the evolution of major and incompatible element compositions of the lavas on the scale of a single volcanic system.
Here, we compile and use the ages and compositions of lavas from the Hawaii, Society, Samoa, and Marquesas volcanic chains on the older portions of the Pacific Plate, where lithosphere thickness and motion should be comparable and thus similarities in magma genesis and duration of volcanism are expected. We selected these four hotspots because they are comparable in their setting and because many of their volcanoes are reasonably well-studied (see Supplementary Material). Indeed, we find very similar patterns of volcanic activity in all of these hotspots but we also note several features that are difficult to explain within the framework of the plume model. The Hawaiian plume is believed to represent the hottest mantle plume with the highest buoyancy flux on Earth (Davies, 1988; Sleep, 1990), yet the duration of shield volcanism in the other Pacific hotspots is similar (~1 million years) suggesting similar widths of the melting zones. Additionally, the Hawaiian hotspot volcanoes erupt lavas indicating both higher and lower degrees of partial melting than the other three hotspots investigated in this study which may indicate either a very heterogeneous nature of the mantle plume (including more pyroxenitic and carbonatitic sources), or more extreme melting conditions due to the higher temperature and a stronger buoyancy flux of the plume.
Geological Setting of the Pacific Hotspots
The Hawaii-Emperor chain of age-progressive volcanoes represents the type example of hotspot volcanism caused by a deep mantle plume (Wilson, 1963; Morgan, 1972). The Hawaiian intraplate volcanoes vary in size from the largest volcanic edifices on Earth with a height of some 10 km to much smaller volcanoes and accordingly, the volume estimates of the Hawaiian volcanoes range from 9,000 to 74,000 km3 (Clague and Sherrod, 2014). The Hawaiian Islands are the best-studied intraplate volcanoes on Earth and the Hawaii volcanic chain consists of 21 islands and several islets that show an age progression from SSE to NNW (e.g., Clague and Dalrymple, 1987; Sharp and Clague, 2006; O'Connor et al., 2013). The Hawaiian intraplate volcanoes lie on oceanic crust of Cretaceous age ranging from 87 to 94 million years (Detrick et al., 1981; Müller et al., 2008). The age progression of shield volcanism of the Hawaiian Islands implies an average velocity of the Pacific Plate of 10 cm/yr across the plume (Clague and Sherrod, 2014). However, the exact rate of age progression may differ as a result of the plume moving south (Tarduno et al., 2003). Additionally, several volcanoes show volumetrically small stages of rejuvenated volcanism occurring up to 5.5 million years after initiation of the volcanism (Clague and Sherrod, 2014; Thordarson and Garcia, 2018). A strong buoyancy flux of Hawaii is reflected by large magma volumes as indicated by the size of the volcanic islands (Sleep, 1990). The present-day position of the front of the plume melting zone is beneath Loihi seamount ~35 km SE of the coast of Big Island (e.g., Moore et al., 1982; Watson and McKenzie, 1991). The detailed sampling of many Hawaiian volcanoes led to the model of four stages of magmatic evolution although much of this variation is based on subaerial lavas whereas submarine data have only recently been included into the existing model (Clague and Sherrod, 2014). The youngest Hawaiian volcanoes are in their shield or postshield stages and rejuvenated lavas are only known from Lanai, Molokai, Koolau, Kauai, and Niihau (Sinton et al., 2017; Thordarson and Garcia, 2018). The decreasing postshield magma production also leads to the establishment of magma reservoirs at the base of the crust, so that postshield lavas frequently are hawaiitic and mugearitic rather than basaltic in composition (e.g., Clague, 1987; Frey et al., 1990).
The Society Islands are part of French Polynesia, a region of an anomalously high rate of intraplate volcanism (Adam et al., 2010). Several aligned and age-progressive volcanoes form the ~800 km long Society Island chain (Dymond, 1975; Guillou et al., 2005). The islands formed on late Cretaceous oceanic crust increasing in age from 66 million years at Mehetia in the southeast to 84 million years at Maupiti in the northwest of the island chain (Müller et al., 2008). The ages of the volcanism decrease from 4.5 million years at Maupiti to less than 0.3 million years at Mehetia yielding a velocity of 11.3 cm/yr for the Pacific Plate (Duncan et al., 1994; Uto et al., 2007). The best-studied island is Tahiti consisting of two volcanoes with stratigraphically defined and chemically distinct shield and postshield stages (Duncan et al., 1994; Hildenbrand et al., 2004). Other older volcanoes like Moorea and Huahine also consist of shield volcanoes with a caldera forming toward the end of the volcanism and later postshield lavas and intrusions (Guillou et al., 2005). The position of the present-day melting anomaly of the Society hotspot is located southeast of Tahiti evident from volcano-seismic activity at the submarine flanks of Mehetia and numerous submarine active volcanoes (Talandier and Okal, 1984; Devey et al., 1990; Binard et al., 1992).
The Marquesas volcanic chain consists of eight large islands between the about 5.0 to 5.5 million year-old Eiao in the NW, and the 1.0 to 1.5 million year-old Fatu Hiva in the southeast (Guillou et al., 2014). The youngest volcanism with ages < 0.5 million years occurs at a seamount SE of Fatu Hiva (Desonie et al., 1993) and at the Marquesas Fracture Zone some 100 km south of Fatu Hiva (Révillon et al., 2017). The Pacific Plate moves with a velocity of ~10.5 cm/yr across the Marquesas mantle plume (McDougall and Duncan, 1980; Révillon et al., 2017) and lithospheric ages are on the order of 50 million years (Müller et al., 2008). The Marquesas islands consist of large shield volcanoes like, for example, the Tekao volcano on Nuku Hiva that have been suggested to mainly consist of olivine tholeiites (Guillou et al., 2014). These shield volcanoes frequently collapsed and the shield lavas were then covered by more incompatible element-enriched alkaline lavas, like the Taiohae formation on Nuku Hiva (Guillou et al., 2014). Similar patterns of volcanic evolution are observed at Ua Huka with the Hikitau shield volcano followed by the alkaline Hane lavas.
The Samoa volcanic chain is an ~1,300 km long complex structure consisting of numerous seamounts and seven islands with the oldest ages of 13.2 million years occurring on the westernmost seamount and the youngest ages in the east, indicating a hotspot origin (Koppers et al., 2008, 2011). The age progression appears to be restricted to the shield volcanism of the Samoan chain whereas rejuvenated volcanism without systematic age progression occurs on many of the eastern islands (Natland, 1980; Koppers et al., 2011). The easternmost and youngest portion of the Samoan chain apparently consists of two parallel seamount chains with the youngest activity at the Vailulu'u submarine volcano in the north (Hart et al., 2000) and the Malu Malu volcano in the south (Koppers et al., 2011). The age variation along the chain suggest that the ~100 million year-old lithospheric plate moves at a velocity of ~7.2 cm/yr across the Samoa mantle plume (Koppers et al., 2008; McDougall, 2010). The volcanism of the Samoa Islands has been suggested to evolve from tholeiitic to mildly alkaline basalts to highly alkaline post-erosional basalts, for example, on Upolu and Savai'i (Natland, 1980; McDougall, 2010) but the large volume of the late highly alkaline eruptions is notable (Konter and Jackson, 2012). The complex and abundant rejuvenated volcanism of the eastern Samoan chain is attributed to the geodynamic situation close to the Tonga subduction zone that may cause fracturing or flexuring of the lithosphere as well as additional mantle upwelling (e.g., Natland, 1980; Konter and Jackson, 2012; Strak and Schellart, 2018).
Results
The Comparison of the Compositional Variation of the Hotspot Lavas
We compiled data on the age and chemical composition of lavas from volcanoes of the hotspots of Hawaii, Society, Marquesas, and Samoa (data sources can be found in the Supplementary Material), all situated on the older portion of the Pacific Plate (Figure 1). The total alkali-silica (TAS) classification of the lavas combined with the division line for tholeiitic and alkaline lavas from Hawaii (Macdonald and Katsura, 1964) reveals that only the Hawaiian volcanoes show a pronounced tholeiitic stage whereas the other three hotspots erupt mainly alkaline and transitional basalts and rare tholeiites (Figure 2). Many of the Hawaiian volcanoes like Kaua'i and Koolau show highly variable lava compositions ranging from tholeiitic basalts to basanites and nephelinites and melilitites (Figure 2a). Field observations combined with geochemistry suggest that all Hawaiian volcanoes evolve through a voluminous stage of tholeiitic eruptions followed by increasingly alkaline lavas with alkali basalts, basanites, and nephelinites (Clague and Dalrymple, 1987). Additionally, Molokai and West Maui volcanoes erupted lavas that are significantly more evolved than the alkali basalts. The other hotspot volcanoes typically show variations between alkali basalts and basanites and most more evolved lavas are also related to the alkali basalts (Figure 2). The young volcanic edifices of the Society hotspot with the island Mehetia and the seamounts Teahitia and Rocard apparently consist of basanite and more evolved lavas like trachytes and phonolites. In contrast, alkali basalts and few tholeiites occur on Tahiti and older volcanoes like Maupiti, Moorea, and Huahine (Figure 2b).
Figure 1. Overview map of the Central and Northern Pacific including the Hawaiian, Marquesas, Samoa, and Society island chains.
Figure 2. The total alkalies-silica (TAS) diagram (Le Bas et al., 1986) for lavas from different volcanoes of the (a) Hawaiian, (b) Society, (c) Marquesas, and (d) Samoa hotspots. The dashed line shows the distinction between alkaline and tholeiitic lavas after Macdonald and Katsura (1964). Data sources can be found in the Supplementary Material.
The Nb/Zr ratio has been widely used to distinguish the different magma series because these incompatible elements are not fractionated during crystallization processes (Figure 3) and are sensitive to source composition because Nb/Zr correlates, for example, with Sr isotope ratios (Clague and Dalrymple, 1988). There is a broad negative correlation between the SiO2 content of the magmas and Nb/Zr, for example, in the Hawaiian lavas, where the tholeiites have the lowest Nb/Zr and the alkaline magmas increasingly higher Nb/Zr (Figure 3). Thus, although there are also differences in Nb/Zr among the Hawaiian shield stage lavas (Frey et al., 1994), the Hawaiian tholeiites in general have Nb/Zr ratios of 0.05 to 0.11 (Figure 3a). The lavas with the lowest Nb/Zr at the Society hotspot range from 0.09 to 0.16, at the Marquesas islands between 0.08 to 0.14, and at Samoa between 0.12 and 0.18 (Figure 3). The mafic lavas with lower SiO2 typically have higher Nb/Zr and the most extreme Nb/Zr of 0.38 are found in nephelinites and melilitites at Kaua'i volcano (Figure 3a). Basanites of the young Mehetia volcano in the Society hotspot have similar Nb/Zr to the alkali basalts from the older volcanoes like Maupiti and Huahine (Figure 3b). On the other hand, the alkali basalts from the young Vailulu volcano in Samoa are much higher in Nb/Zr than alkali basalts from the older volcanoes Ta'u and Tutuila (Figure 3d).
Figure 3. The variation of Nb/Zr ratios with SiO2 contents for the lavas from the (a) Hawaiian, (b) Society, (c) Marquesas, and (d) Samoa hotspots. The Nb/Zr ratio remains constant during much of the magma evolution and is generally not affected by fractional crystallization. The differences of Nb/Zr ratios in lavas from the same volcanoes reflect different magma series of volcanic stages. The lavas with the lowest Nb/Zr typically represent the shield stage as outlined by the gray bars. Data sources can be found in the Supplementary Material.
The range of SiO2 for primitive magmas with 12 to 15 wt.% MgO varies considerably between the different hotspots (Figure 4). The control lines for addition of olivine with forsterite (Fo) contents of 88 are also shown because most lavas with MgO contents >10 wt.% probably formed by addition, lavas with MgO < 10 wt.% by fractionation of olivine (±clinopyroxene and plagioclase). Primitive lavas (MgO > 5 wt.%) of the Hawaiian volcanoes show a range from 36 to 52 wt.% SiO2, whereas those of the Societies, Marquesas and Samoa all range from 41 to 48 wt.% SiO2 (Figure 4), i.e., they cover a much smaller range compared to Hawaii. Most volcanoes show well-defined increasing different trends of SiO2 with decreasing MgO implying parental magmas with different SiO2 contents.
Figure 4. The variation of SiO2 vs. MgO contents in the lavas from the (a) Hawaiian, (b) Society, (c) Marquesas, and (d) Samoa hotspots. The SiO2 contents typically increase with decreasing MgO due to crystal fractionation processes. Lavas with 12–15 wt.% MgO represent near-primary compositions of magmas from the mantle and their range is indicated by the gray box. Note that the Hawaiian volcanoes show a much larger range of SiO2 contents (36–52 wt.%) for these primary magmas than the other hotspots (41–48 wt.%). The two black lines show the addition of olivine with forsterite (Fo) contents of 88 in 5% increments indicated by the crosses. Data sources can be found in the Supplementary Material.
The variation of incompatible element ratios with SiO2 is most pronounced in the chondrite-normalized Ce/Yb ratios [= (Ce/Yb)N]. The (Ce/Yb)N of the lavas from all hotspots display a negative correlation toward the lowest SiO2 contents of each volcano (Figure 5). This trend can be defined for the primitive Hawaiian lavas of Koolau volcano on Oahu and Kaua'i as (Ce/Yb)N = −2.5xSiO2 + 115. The correlation trend is plotted into the diagrams of the lavas from the other hotspot volcanoes for comparison. Whereas, many of the most primitive lavas of the Marquesas hotspot lie close to this trend, the Society and Samoa hotspot lavas have higher (Ce/Yb)N for a given SiO2 content (Figure 5) and lack an obvious correlation for the Society lavas.
Figure 5. The variation of chondrite-normalized Ce/Yb ratios with SiO2 contents of the lavas from the (a) Hawaiian, (b) Society, (c) Marquesas, and (d) Samoa hotspots. Note that there is a negative correlation between the (Ce/Yb)N and the lowest SiO2 content. Different magma series have relatively constant (Ce/Yb)N but crystal fractionation leads to increasing SiO2 contents. The average trend of the variation observed at Koolau and Kaua'i is shown in all diagrams for comparison. Data sources can be found in the Supplementary Material.
The Variation of the Chemical Composition With the Age
The Nb/Zr ratios plotted against the age of the volcanism (Figure 6) reveal significant changes of lava composition with time in the Hawaii, Society and Marquesas hotspot volcanoes. Unfortunately, there are few samples with both geochemical and age data available from the Samoan hotspot so that we cannot show the variation with age for this hotspot. The earliest age-dated stages of the different volcanoes typically have the lowest Nb/Zr whereas later erupted lavas have higher Nb/Zr ratios (Figure 6). We interpret this to represent the transition from the shield to the postshield stage that often appears to be gradual, for example, at West Maui, Tahiti, and Tahuata (Figure 6). We cannot define the timing at which the preshield stages changed to shield volcanism because of a lack of coexisting preshield lavas for the shield and postshield stages shown here. However, the duration of the shield stage as indicated by the occurrence of lavas with low Nb/Zr can be defined to be on the order of 1 million years in the case of West Maui, Koolau, and Kaua'i in the Hawaiian hotspot (Figure 6a). The shield stage appears to last for similar periods of time at the well-studied volcanoes of Tahiti in the Societies, and Tahuata and Ua Huka in the Marquesas. Toward the end of the shield stage defined by the low Nb/Zr ratios, volcanoes at all three hotspots show a coeval eruption of more enriched lavas with an overlap of several 100 kyrs (Figure 6). In the case of Hawaiian volcanoes and the Tahiti and Huahine volcanoes in the Societies the change to more enriched postshield lavas is relatively small. The Hawaii data display the large age and compositional difference of the rejuvenated lavas compared to the shield and postshield lavas (Figure 6a). The relatively well-studied volcanoes in the Marquesas show a similar pattern with much higher Nb/Zr lavas erupting after a 1 million year-long break at Ua Huka whereas the rejuvenated lavas at Fatu Hiva and Tahuata erupt subsequent to the shield and postshield stage (Figure 6c).
Figure 6. Variation of the Nb/Zr ratios in the lavas with age for the best-studied volcanoes of the (a) Hawaii, (b) Society, and (c) Marquesas hotspots. Note that error bars are shown for most ages but are typically smaller than the symbols. The chemical variation of the lavas with age implies changes in the magma formation and mantle source. The red box in (a) indicates the range of eruption ages and compositions of the shield lavas at Waianae volcano. Note also that there is considerable overlap between shield stage volcanism and later more enriched postshield or rejuvenated volcanism in Kaua'i, Tahiti, Huahine, Tahuata, and Fatu Hiva. Data sources can be found in the Supplementary Material.
Discussion
The Compositional Variation of the Submarine Preshield Volcanic Stage
Because the preshield stage of the oceanic intraplate volcanism at hotspots occurs at great water depths and are covered by the younger stages, little is known about these eruptions and the composition of the lavas. Basanitic to tholeiitic basalts were recovered from Loihi seamount SE of the island of Hawaii (Figure 2a) and these lavas were interpreted to reflect initiation of melting at the plume edge beneath the lithosphere (Moore et al., 1982). Clague and Sherrod (2014) suggest that preshield lavas can be observed at the four Hawaiian volcanoes Loihi, Kilauea, Kohala, and perhaps Hualalai, whereas lavas of this stage are buried at most other volcanoes. The submarine young volcanoes at the other three studied hotspots also differ from the subaerial lavas. At the Society hotspot, lavas at the young Mehetia and Teahitia volcanoes are more SiO2-undersaturated basanites than the subaerial alkali basalts of Tahiti, Huahine, or Moorea (Figure 2b) although the Nb/Zr ratios are similar (Figure 3b). Both the submarine and subaerial lavas recovered from the youngest island Mehetia are basanites (Figure 2b) indicating that the volcano may still be in the preshield stage of volcanism of the Society hotspot. Thus, similarly to the case in Hawaii, the young preshield alkaline melts may have formed by lower degrees of melting than the transitional basalts of the later subaerial shield stage. Devey et al. (2003) suggested that the preshield stage at the Society hotspot formed by melting of the most incompatible element-enriched source which could explain the high Nb/Zr ratios. Additionally, the small preshield volcanoes at the Society hotspot like Rocard erupted relatively evolved lavas with trachytic composition (Figure 2b) indicating longer times of stagnation in the lithosphere before a stable magma system with larger volumes of magma is established (Devey et al., 2003). Little is known about the youngest volcanism of the Marquesas hotspot because this volcanism occurs at the submarine Marquesas Fracture Zone but the lavas recovered from two small young seamounts are tephritic (Révillon et al., 2017), i.e., more alkaline than the alkali basalts of the Marquesas shield stage lavas (Figure 2c). In contrast, the lavas from the young submarine Vailulu volcano at the eastern end of the Samoan chain have similar transitional basaltic compositions to those from the older subaerial volcanoes (Figure 2d) but higher Nb/Zr (Figure 3d). Thus, with the exception of Samoa the preshield submarine volcanism at the three hotspots of Hawaii, Society and Marquesas appears to be more alkaline than the later subaerial shield stages which probably indicates lower degrees of partial melting during the earliest volcanic stage.
Variation of Shield Stage Lava Compositions
The shield stage of a volcano is generally defined by structural and stratigraphic observations of the most voluminous eruptive stage yielding 85 to 90% of a volcano (Clague and Sherrod, 2014). The observations at the subaerial parts of the volcanoes indicate that tholeiitic basalts erupt during the shield stage but that there is a chemical transition to the alkaline postshield stage (e.g., Chen et al., 1991; Sinton et al., 2017). The tholeiitic basalts of the Hawaiian shield stage have the lowest Nb/Zr ratios of all Hawaiian lavas (Figure 3a) which was pointed out previously (Clague and Dalrymple, 1988; Frey et al., 1994). The well-studied shield lavas in the Hawaiian volcanoes are tholeiitic basalts but in the other hotspots the shield lavas are tholeiitic to alkali basaltic (Figure 2). The shield lavas of Tahiti are relatively well-defined based on field observations and a well-dated ~1 million year-long stage with eruption of transitional basaltic lavas with relatively low Nb/Zr (Figure 6). Similarly, Moorea and Huahine volcanoes in the Society hotspot largely consist of transitional basalts that lie on the division line in Figure 2 and are interpreted as shield stage lavas. We suggest that all shield stage lavas of the studied Pacific hotspot volcanoes are typically the least incompatible element-enriched samples, i.e., those with the lowest alkali content, Nb/Zr and (Ce/Yb)N but they also display relatively high SiO2 contents (Figures 2–4, 6). Whereas, the variable SiO2 content largely reflects differences in degree and mean pressure of melting (Green et al., 2001), the incompatible element ratios mainly reflect differences in composition of the mantle source composition (Frey et al., 1978). Thus, we conclude in agreement with previous studies (e.g., Frey et al., 1991; Duncan et al., 1994; Farnetani and Hofmann, 2010) that the shield stage of the different hotspot volcanoes represents the highest degrees of partial melting although only the Hawaiian hotspot shows voluminous tholeiitic shield stage basalts. The recurrent relatively high degrees of partial melting beneath thick lithospheric plates support the formation in a long-lived melting anomaly probably caused by thermal or chemical mantle plumes. The covariation of SiO2 and incompatible element ratios (Figures 3, 5) indicates that the degree of partial melting varies with source composition in agreement with melting of variably enriched mantle sources.
The different volcanoes of most hotspots show very similar compositions in their shield stages (Figures 2, 3) implying that the variation in major and incompatible element source compositions and melting process with time is relatively small although there are significant differences in terms of radiogenic isotope compositions (e.g., Abouchami et al., 2005; Payne et al., 2013). This can best be explained by thermally and compositionally homogenous melting zones in the different hotspots over time periods of several million years. Such a systematic homogeneity is especially observed at the Hawaiian shield volcanoes but the estimated volumes of the youngest volcanoes vary from ~9,000 km3 for West Maui to ~74,000 km3 for Mauna Loa (Clague and Sherrod, 2014). Even if a significant variation of degree of eutectic melting may produce tholeiitic magmas, the incompatible element ratios would be variably diluted which is not observed. Thus, while the recurrent geochemical composition of shield tholeiites implies a constant degree of melting during the shield stage the magma production varies by a factor of 8. This may imply that the erupted magma volume above mantle plumes may not be simply related to the degrees of partial melting.
The lavas from the Hawaiian hotspot indicate a larger variation in primitive magma compositions than those from the other Pacific hotspots (Figure 4). Experiments suggest that the large variation of SiO2 contents in Hawaiian primary magmas between 36 and 52 wt.% requires low-degree melting of CO2-rich mantle (e.g., Brey and Green, 1975; Clague and Frey, 1982; Cousens and Clague, 2015) on the one hand, and melting of pyroxenite-rich mantle on the other hand (e.g., Hauri, 1996). In contrast, the other three hotspot magmas range from basanites, alkali basalts, to rare tholeiitic basalts (Figure 2) most of which have been produced experimentally by variable degrees of partial melting of peridotite bearing some CO2 (Takahashi and Kushiro, 1983; Hirose, 1997; Green et al., 2001; Dasgupta et al., 2007). This relatively restricted compositional variation of the mantle sources in the other three hotspots may indicate that CO2-rich components and pyroxenite are absent and the source probably mainly consists of garnet peridotite.
Age Variation of Shield Stages
The plume model predicts that the shield stage of the volcanoes should reflect the plate velocity and the width of the central plume melting zone. In the case of the hotspots beneath the old and thick Pacific Plate the width of the plume should be the most important parameter directly related to both composition and age of the erupted melts. The definition of the period of time for the shield stage of each volcano is difficult to establish because the beginning cannot be established due to volcano growth and rare samples from the preshield stages. Preshield lavas were sampled and age-dated at the Loihi, Kilauea, and Kohala volcanoes of the Hawaiian hotspot and are typically basanites and alkali basalts (Clague and Sherrod, 2014). As discussed above the preshield stages are poorly defined at the other hotspots and we suggest that early submarine stages of intraplate volcanism may have a different magmatic evolution compared to the Hawaiian volcanoes. Because of the unknown initiation of shield volcanism the age range observed in the compiled ages for shield stage lavas are minimum ages. The compiled data for the well-studied Hawaiian volcanoes Koolau, West Maui, and Kauai show relatively low Nb/Zr ratios for ~1 million years (Figure 6) indicating that the shield stage of Hawaiian volcanoes may typically last ~1 million years, whereas earlier studies suggested relatively short shield stages <0.5 million years (Frey et al., 1990). The well-studied lavas from Tahiti and those from Hiva Oa, Tahuata, and Ua Huka in the Marquesas suggest that the shield stage of these volcanoes also lasted ~1 million years (Figure 6). The Pacific Plate moves with the same velocity of ~10 cm/yr across the Hawaii, Society and Marquesas plumes (Gripp and Gordon, 2002). Thus, the apparent similarity of the duration of the shield stage in the different hotspots indicates similar widths of ~100 km for the central melting anomalies. This observation is surprising considering that the buoyancy fluxes and likely the temperatures are distinct between the different plumes (Davies, 1988; Sleep, 1990). The variation of magma compositions indicates that the degree of melting varies and, for example, the alkaline shield lavas of the Marquesas formed at lower degrees of melting than the tholeiites of Hawaii implying that the Hawaii plume has a higher temperature than the other plumes (Herzberg and Asimov, 2008). We thus conclude that the widths of the melting anomalies are not linked to the temperature of the plumes but may be rather be affected by the velocity of the plate and the resulting plume shear. The similarity in melting zone width may be due to the horizontal spreading of the ascending plume by the relatively fast Pacific Plate (Farnetani and Hofmann, 2010) that may affect plumes with lower buoyancy more than the strong Hawaiian plume. This also implies that there will be no simple correlation between duration of the respective volcanic stages and the physical properties of the plume. The occurrence of more enriched signatures in the Samoa, Marquesas and Society islands may largely reflect mantle heterogeneity due to the smaller buoyancy flux as compared to the Hawaiian mantle plume in which much of this heterogeneity may be overprinted by the extensive melting regime.
The Transition From the Shield to the Postshield and Rejuvenated Stages
Large geochemical differences between shield lavas occur at Samoa but some volcanoes of this hotspot appear to erupt very large volumes of postshield and rejuvenated lavas, too, probably reflecting the tectonic influence of the Tonga subduction zone on mantle melting (Natland, 1980; Konter and Jackson, 2012). Thus, the Samoan intraplate volcanism deviates from the more regular pattern of volcano evolution of the other Pacific hotspots. Hence, the Hawaiian model may not be easily applicable to other intraplate volcanoes. Toward the end of the shield stage, more enriched lavas with higher Nb/Zr ratios are observed at West Maui and Kaua'i but also at Tahiti, Tahuata, and Fatu Hiva (Figure 6) implying that the formation of postshield magmas overlaps with that of the shield stage by up to 200 kyrs. This evolution has been described previously for Hawaiian volcanoes (Clague and Sherrod, 2014; Sinton et al., 2017), but seems to be a typical feature also observed in lavas from other Pacific hotspots. Interestingly, a few samples at Kauai, Tahuata, and Fatu Hiva suggest that the volcanoes erupt the most enriched lavas contemporaneously to the final shield and the postshield lavas (Figure 6). The variation of age and Nb/Zr ratios displays a significant overlap of the lavas formed during the different stages and there appears to be a period toward the end of the shield stage when relatively SiO2-rich and less incompatible element-enriched lavas erupt parallel to more alkaline and enriched postshield stage lavas (Figure 6). This overlap requires at least two separate magma systems in the mantle feeding the eruptions at the top with limited mixing occurring in between the different ascent systems. The postshield magmas are typically more alkaline than the shield magmas and probably formed by lower degrees of partial melting. A numerical dynamic model of the Hawaiian plume (Farnetani and Hofmann, 2010) suggests that the postshield magmas represent deeper melts than the shield magmas which is in agreement with the lower SiO2 contents and higher (Ce/Yb)N of the melts (Figure 5). We conclude that the melting zone of many mantle plumes produces different melts for about 200 kyrs and that these magmas rise in separate systems to the surface. At a plate velocity of 10 cm/yr this period of time suggests an ~20 km wide zone of overlap in the melting region feeding the different magmas which will be on the scale of a single volcanic system.
Putting the Hawaiian Model to a Test
The compilation of the chemical and age data for the four Pacific hotspot lavas indicates that Hawaii is unusual in the chemical variation of the lavas (Figure 4), but that there are similar patterns of magma evolution from alkaline submarine preshield eruptions to relatively SiO2-rich shield lavas and then more alkaline postshield and rejuvenated lavas. Only Samoa seems to show a different evolution where the youngest submarine stage at Vailulu resembles that of subaerial shield stages at older volcanoes and where rejuvenated lavas appear to be extremely abundant. However, more data with better age resolution are required to test the applicability of the Hawaiian model at the Samoan volcanoes. In the well-studied Marquesas and Society hotspot volcanoes the change from shield to postshield and rejuvenated volcanism is comparable to that observed at Hawaiian volcanoes (Figure 6). The interpretation of the preshield volcanism is similarly complicated for Hawaii, Society, and Marquesas because this stage is mainly known from few samples from single submarine volcanoes without a clear relation to shield volcanism. We suggest that the Hawaiian model explains the observed systematic variation of magma composition with time as a reflection of variable degrees of partial melting due to movement of the plate across a plume.
Some inter-shield variability within the Marquesas, Society, and the Hawaiian island chain (Figure 3) can be observed between the islands of the northern- and islands of the southern groups (Abouchami et al., 2005; Payne et al., 2013). The physically different source components contribute to the formation of the shield volcanoes over small spatial distances of less than few km's (Pietruszka and Garcia, 1999) strongly supporting the complex and heterogeneous nature of plumes and their surrounding mantle material. The presence of tholeiitic, large degree melts during the shield stages may be restricted to large, stationary plume systems that preferentially have larger buoyancy fluxes leading to larger degrees of partial melting. On the other hand, the extremely enriched and SiO2-undersaturated melts of the Hawaiian rejuvenated magmas may indicate either more variable mantle sources or remelting of enriched sources by the extremely hot Hawaiian plume. We conclude that the evolution of ocean island volcanoes through distinct volcanological, petrological, and geochemical stages does not strictly follow the Hawaiian model and chemical variation is smaller but that the compositional changes between the different stages are clearly discernable.
Conclusions and outlook
The limited age and compositional data of lavas from the Pacific hotspots reveal systematic variations of magma composition with age in most volcanoes where the late lavas are typically more enriched in incompatible elements and more alkaline than those of the shield stage. The Society and Marquesas hotspots show basanitic submarine volcanism apparently preceding the shield stage with alkali basaltic magmas. This variation most likely reflects the movement of the lithospheric plate across a thermal mantle plume forming a zoned melting anomaly with variable degrees of partial melting. However, more data with combined chemical and age constraints are required to better define the evolution of the intraplate magmatic systems. Existing data indicate that the shield stages of the well-studied volcanoes last about 1 million years and seem to similar for both strong and weak plumes. Because the velocity of the Pacific Plate is similar at the studied hotspots this implies similar sizes of the melting anomalies although the temperatures in the mantle plumes differ. The overlap of shield and postshield stage volcanism for up to 200 kyrs is also typical at different hotspots and indicates about 20 km wide transitional melting zone at the flank of the plume during which there are contemporaneous eruptions of both shield stage and postshield stage melts through distinctively different channels of ascent. More age and geochemical data of stratigraphically controlled samples are required from different volcanoes in order to understand the trends of magma evolution, melting processes, and mantle dynamics.
Author Contributions
CB and KH compiled data, wrote the manuscript, and prepared the figures. FK worked on the initial data compilation and filtering and contributed ideas.
Conflict of Interest Statement
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Acknowledgments
We thank the editor Adriano Pimentel for inviting this contribution and for his patience during the completion of this manuscript. We acknowledge the helpful and constructive reviews by J. G. Shellnutt, I. E. M. Smith, and D. Geist that have considerably improved the quality of this work. CB acknowledges support by I. MacLeod. We acknowledge funding by the Deutsche Forschungsgemeinschaft (DFG) through grant BE4459/7-1.
Supplementary Material
The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/feart.2018.00242/full#supplementary-material
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Keywords: hawaii, samoa, society, marquesas, geochemistry, mantle melting, hotspots
Citation: Haase KM, Beier C and Kemner F (2019) A Comparison of the Magmatic Evolution of Pacific Intraplate Volcanoes: Constraints on Melting in Mantle Plumes. Front. Earth Sci. 6:242. doi: 10.3389/feart.2018.00242
Received: 15 June 2018; Accepted: 14 December 2018;
Published: 04 January 2019.
Edited by:
Adriano Pimentel, Centro de Informação e Vigilância Sismovulcânica dos Açores (CIVISA), PortugalReviewed by:
J. Gregory Shellnutt, National Taiwan Normal University, TaiwanIan Ernest Masterman Smith, The University of Auckland, New Zealand
Dennis Geist, National Science Foundation (NSF), United States
Copyright © 2019 Haase, Beier and Kemner. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Christoph Beier, Y2hyaXN0b3BoLmJlaWVyQGZhdS5kZQ==