{"title":"羽毛板相互作用","authors":"Shichun Huang","doi":"10.1029/2024AV001464","DOIUrl":null,"url":null,"abstract":"<p>Age progressive volcanic trends, known as hotspot tracks, are thought to be produced by partial melting of buoyant mantle plumes rising from the deep mantle (Morgan, <span>1971</span>; Wilson, <span>1963</span>). Hotspot tracks record the relative motion between plates and mantle plumes, and they are used to reconstruct the history of plate motion and to constrain the geochemical heterogeneity within the mantle, which are important to our understanding of mantle dynamics (e.g., Koppers et al., <span>2021</span>; Weis et al., <span>2023</span>).</p><p>Through a careful examination of isotopic, geochronological, and plate motion reconstruction data, Jackson et al. (<span>2024</span>) argued that certain Cretaceous (87–106 Ma) Magellan seamounts north of the Ontong-Java Plateau (OJP) may have been produced by the Samoan plume. This finding places the Samoan hotspot track among the longest-lived ones. However, there is a significant gap in volcanic activity from 24 to 87 Ma, excluding the 44 Ma Malaita volcanism. Raising the question, what mechanism could produce a 63 Ma gap in an otherwise enduring hotspot track?</p><p>It has long been observed that most hotspot tracks manifest as discrete volcanoes, exemplified by the long-lived Hawaii-Emperor Volcanic Chain, rather than continuous ridges. It is suggested that the locations of these volcanoes are controlled by fractures within the lithosphere, facilitating the migration of plume-generated magma (e.g., Hieronymus & Bercovici, <span>1999</span>). Consequently, discrete volcanoes are anticipated along hotspot tracks.</p><p>To explain the bilaterally zoned hotspot tracks (e.g., Abouchami et al., <span>2005</span>; Huang et al., <span>2011</span>; Weis et al., <span>2011</span>), Rohde et al. (<span>2013</span>) argued that mantle plumes originating from the lower mantle may bifurcate at the mantle transition zone (Figure 1a). Because of the different mantle viscosities in the upper and lower mantle, a plume might rise much slower in the lower mantle compared to in the upper mantle. To maintain the same plume flux, a plume would become thinner in the upper mantle, which may lead to plume bifurcation at the mantle transition zone (Rohde et al., <span>2013</span>). Alternatively, it is also possible that after entering the upper mantle, a plume fragments into discrete upwelling diapirs rather than maintaining a continuous flow (Figure 1a), resulting in volcanic activity gaps along hotspot tracks.</p><p>However, neither of these theories explains the prolonged absence of volcanism within a significant period (24–87 Ma) of the Samoan hotspot track. Jackson et al. (<span>2024</span>) noted that during this particular period of time, the Samoan plume was under the thick OJP. Mantle plumes ascend adiabatically, with a steeper pressure-temperature slope compared to that of the mantle solidus. As such, plumes start to melt and produce magma when reaching shallow depths (low pressure). The upwelling stops at the base of rigid lithosphere, halting partial melting. Jackson et al. (<span>2024</span>) argued that the OJP's lithosphere is sufficiently thick to inhibit the plume's ascent to a shallow enough depth for melting, thus precluding volcanic activity and creating a seamount-free corridor (Figure 1b).</p><p>However, if the lithosphere is not thick enough to completely prevent a plume from melting and if a plume contains both an enriched lithology with a lower melting point and a refractory lithology with a higher melting point, the enriched lithology will melt preferentially (e.g., Phipps Morgan, <span>2001</span>; Stracke & Bourdon, <span>2009</span>). This results in magmas produced under thicker lithosphere having more enriched geochemical signatures (Figure 1b), as observed at the Emperor Seamount Chain (Frey et al., <span>2005</span>; Regelous et al., <span>2003</span>) and the Magellan seamounts, the Cretaceous Samoan volcanoes (Jackson et al., <span>2024</span>).</p><p>Key geochemical signatures linking Magellan seamount lavas to Samoa include their distinctively high <sup>87</sup>Sr/<sup>86</sup>Sr and low <sup>143</sup>Nd/<sup>144</sup>Nd ratios, characteristic of the Enriched Mantle 2 (EM-2) mantle endmember, which is indicative of recycled ancient continental material in their mantle source (Jackson et al., <span>2007</span>). However, it remains to be better elucidated where the Samoan plume, and mantle plumes in general, originates from. Are mantle endmembers, such as EM-2, inferred based on geochemical data of plume-derived lavas related to large mantle structures imaged by seismic waves, such as Large Low-Shear-Velocity Provinces (LLSVPs) in the deep mantle (e.g., Huang et al., <span>2011</span>; Koppers et al., <span>2021</span>; Weis et al., <span>2011</span>, <span>2023</span>)?</p><p>The findings of Jackson et al. (<span>2024</span>) suggest that the global plume flux might be underestimated if based solely on hotspot volcanic flux, as plume productivity can be suppressed under thick lithosphere. Furthermore, the isotopic compositions of erupted hotspot lavas may not be representative of their mantle source characteristics, as they are biased toward the enriched endmembers. If the enriched mantle endmembers contain recycled ancient surface materials, such as sediments, continental and oceanic crusts, their proportions in mantle plumes may be overestimated. They all hold significant implications for advancing our understanding of mantle dynamics.</p><p>The authors declare no conflicts of interest relevant to this study.</p>","PeriodicalId":100067,"journal":{"name":"AGU Advances","volume":"5 5","pages":""},"PeriodicalIF":8.3000,"publicationDate":"2024-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2024AV001464","citationCount":"0","resultStr":"{\"title\":\"Plume-Plateau Interaction\",\"authors\":\"Shichun Huang\",\"doi\":\"10.1029/2024AV001464\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Age progressive volcanic trends, known as hotspot tracks, are thought to be produced by partial melting of buoyant mantle plumes rising from the deep mantle (Morgan, <span>1971</span>; Wilson, <span>1963</span>). Hotspot tracks record the relative motion between plates and mantle plumes, and they are used to reconstruct the history of plate motion and to constrain the geochemical heterogeneity within the mantle, which are important to our understanding of mantle dynamics (e.g., Koppers et al., <span>2021</span>; Weis et al., <span>2023</span>).</p><p>Through a careful examination of isotopic, geochronological, and plate motion reconstruction data, Jackson et al. (<span>2024</span>) argued that certain Cretaceous (87–106 Ma) Magellan seamounts north of the Ontong-Java Plateau (OJP) may have been produced by the Samoan plume. This finding places the Samoan hotspot track among the longest-lived ones. However, there is a significant gap in volcanic activity from 24 to 87 Ma, excluding the 44 Ma Malaita volcanism. Raising the question, what mechanism could produce a 63 Ma gap in an otherwise enduring hotspot track?</p><p>It has long been observed that most hotspot tracks manifest as discrete volcanoes, exemplified by the long-lived Hawaii-Emperor Volcanic Chain, rather than continuous ridges. It is suggested that the locations of these volcanoes are controlled by fractures within the lithosphere, facilitating the migration of plume-generated magma (e.g., Hieronymus & Bercovici, <span>1999</span>). Consequently, discrete volcanoes are anticipated along hotspot tracks.</p><p>To explain the bilaterally zoned hotspot tracks (e.g., Abouchami et al., <span>2005</span>; Huang et al., <span>2011</span>; Weis et al., <span>2011</span>), Rohde et al. (<span>2013</span>) argued that mantle plumes originating from the lower mantle may bifurcate at the mantle transition zone (Figure 1a). Because of the different mantle viscosities in the upper and lower mantle, a plume might rise much slower in the lower mantle compared to in the upper mantle. To maintain the same plume flux, a plume would become thinner in the upper mantle, which may lead to plume bifurcation at the mantle transition zone (Rohde et al., <span>2013</span>). Alternatively, it is also possible that after entering the upper mantle, a plume fragments into discrete upwelling diapirs rather than maintaining a continuous flow (Figure 1a), resulting in volcanic activity gaps along hotspot tracks.</p><p>However, neither of these theories explains the prolonged absence of volcanism within a significant period (24–87 Ma) of the Samoan hotspot track. Jackson et al. (<span>2024</span>) noted that during this particular period of time, the Samoan plume was under the thick OJP. Mantle plumes ascend adiabatically, with a steeper pressure-temperature slope compared to that of the mantle solidus. As such, plumes start to melt and produce magma when reaching shallow depths (low pressure). The upwelling stops at the base of rigid lithosphere, halting partial melting. Jackson et al. (<span>2024</span>) argued that the OJP's lithosphere is sufficiently thick to inhibit the plume's ascent to a shallow enough depth for melting, thus precluding volcanic activity and creating a seamount-free corridor (Figure 1b).</p><p>However, if the lithosphere is not thick enough to completely prevent a plume from melting and if a plume contains both an enriched lithology with a lower melting point and a refractory lithology with a higher melting point, the enriched lithology will melt preferentially (e.g., Phipps Morgan, <span>2001</span>; Stracke & Bourdon, <span>2009</span>). This results in magmas produced under thicker lithosphere having more enriched geochemical signatures (Figure 1b), as observed at the Emperor Seamount Chain (Frey et al., <span>2005</span>; Regelous et al., <span>2003</span>) and the Magellan seamounts, the Cretaceous Samoan volcanoes (Jackson et al., <span>2024</span>).</p><p>Key geochemical signatures linking Magellan seamount lavas to Samoa include their distinctively high <sup>87</sup>Sr/<sup>86</sup>Sr and low <sup>143</sup>Nd/<sup>144</sup>Nd ratios, characteristic of the Enriched Mantle 2 (EM-2) mantle endmember, which is indicative of recycled ancient continental material in their mantle source (Jackson et al., <span>2007</span>). However, it remains to be better elucidated where the Samoan plume, and mantle plumes in general, originates from. Are mantle endmembers, such as EM-2, inferred based on geochemical data of plume-derived lavas related to large mantle structures imaged by seismic waves, such as Large Low-Shear-Velocity Provinces (LLSVPs) in the deep mantle (e.g., Huang et al., <span>2011</span>; Koppers et al., <span>2021</span>; Weis et al., <span>2011</span>, <span>2023</span>)?</p><p>The findings of Jackson et al. (<span>2024</span>) suggest that the global plume flux might be underestimated if based solely on hotspot volcanic flux, as plume productivity can be suppressed under thick lithosphere. Furthermore, the isotopic compositions of erupted hotspot lavas may not be representative of their mantle source characteristics, as they are biased toward the enriched endmembers. If the enriched mantle endmembers contain recycled ancient surface materials, such as sediments, continental and oceanic crusts, their proportions in mantle plumes may be overestimated. They all hold significant implications for advancing our understanding of mantle dynamics.</p><p>The authors declare no conflicts of interest relevant to this study.</p>\",\"PeriodicalId\":100067,\"journal\":{\"name\":\"AGU Advances\",\"volume\":\"5 5\",\"pages\":\"\"},\"PeriodicalIF\":8.3000,\"publicationDate\":\"2024-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2024AV001464\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"AGU Advances\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1029/2024AV001464\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"GEOSCIENCES, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"AGU Advances","FirstCategoryId":"1085","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1029/2024AV001464","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"GEOSCIENCES, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
年龄递增的火山趋势,即所谓的热点轨迹,被认为是由从地幔深处上升的浮力地幔羽流部分熔化产生的(Morgan,1971 年;Wilson,1963 年)。热点轨迹记录了板块和地幔羽流之间的相对运动,可用于重建板块运动的历史和约束地幔内的地球化学异质性,这对我们了解地幔动力学非常重要(例如,Koppers et al、通过对同位素、地质年代和板块运动重建数据的仔细研究,Jackson 等人(2024 年)认为,翁通-爪哇海台(OJP)以北的某些白垩纪(87-106 Ma)麦哲伦海山可能是由萨摩亚羽流产生的。这一发现使萨摩亚热点轨迹成为最长寿的热点轨迹之一。然而,除去 44 Ma 的马莱塔火山活动之外,从 24 Ma 到 87 Ma 的火山活动存在明显的差距。人们早就注意到,大多数热点轨道表现为离散的火山,例如长寿的夏威夷-皇帝火山链,而不是连续的山脊。有人认为,这些火山的位置受岩石圈内断裂的控制,有利于羽状岩浆的迁移(例如,Hieronymus & Bercovici, 1999)。为了解释双侧分带的热点轨道(如 Abouchami 等人,2005 年;Huang 等人,2011 年;Weis 等人,2011 年),Rohde 等人(2013 年)认为,源自下地幔的地幔羽流可能会在地幔过渡带分叉(图 1a)。由于上地幔和下地幔的地幔粘度不同,羽流在下地幔中的上升速度可能比在上地幔中慢得多。为了保持相同的羽流通量,羽流在上地幔中会变得更细,这可能会导致羽流在地幔过渡带分叉(Rohde 等人,2013 年)。或者,羽流在进入上地幔后,也可能分裂成离散的上涌二叠体,而不是保持连续的流动(图1a),从而导致沿热点轨道出现火山活动间隙。然而,这两种理论都无法解释萨摩亚热点轨道在相当长的时期内(24-87 Ma)长期没有火山活动的原因。Jackson等人(2024年)指出,在这一特定时期,萨摩亚羽流处于厚厚的OJP之下。地幔羽流是绝热上升的,与地幔固结层相比,其压力-温度斜率更陡。因此,羽流在到达浅层(低压)时开始熔化并产生岩浆。上升流在刚性岩石圈底部停止,部分熔化也随之停止。杰克逊等人(2024 年)认为,大洋交界处的岩石圈足够厚,足以抑制羽流上升到足够浅的深度进行熔化,从而排除了火山活动,形成了无海山走廊(图 1b)。然而,如果岩石圈厚度不足以完全阻止羽流熔化,如果羽流同时包含熔点较低的富集岩性和熔点较高的难熔岩性,富集岩性将优先熔化(例如Phipps Morgan, 2001; Stracke & Bourdon, 2009)。这导致在较厚岩石圈下产生的岩浆具有更丰富的地球化学特征(图 1b),如在皇帝海山链(Frey 等人,2005 年;Regelous 等人,2003 年)和麦哲伦海山、白垩纪萨摩亚火山(Jackson 等人,2024 年)观察到的那样、将麦哲伦海隆熔岩与萨摩亚联系起来的关键地球化学特征包括其明显的高87Sr/86Sr和低143Nd/144Nd比率,这是富集地幔2(EM-2)地幔末段的特征,表明其地幔源中有回收的古大陆物质(Jackson等人,2007年)。然而,萨摩亚羽流和一般地幔羽流的来源还有待进一步阐明。地幔内含物,如 EM-2,是否是根据与地震波成像的大型地幔结构(如深地幔中的大型低剪切速度省(LLSVPs))有关的羽状熔岩的地球化学数据推断出来的(如 Huang 等,2011 年;Koppers 等,2007 年)?Jackson等人(2024年)的研究结果表明,如果仅仅基于热点火山通量,全球羽流通量可能会被低估,因为在厚岩石圈下羽流的生产力会受到抑制。此外,喷发的热点熔岩的同位素组成可能不能代表其地幔源特征,因为它们偏向于富集的内含物。
Age progressive volcanic trends, known as hotspot tracks, are thought to be produced by partial melting of buoyant mantle plumes rising from the deep mantle (Morgan, 1971; Wilson, 1963). Hotspot tracks record the relative motion between plates and mantle plumes, and they are used to reconstruct the history of plate motion and to constrain the geochemical heterogeneity within the mantle, which are important to our understanding of mantle dynamics (e.g., Koppers et al., 2021; Weis et al., 2023).
Through a careful examination of isotopic, geochronological, and plate motion reconstruction data, Jackson et al. (2024) argued that certain Cretaceous (87–106 Ma) Magellan seamounts north of the Ontong-Java Plateau (OJP) may have been produced by the Samoan plume. This finding places the Samoan hotspot track among the longest-lived ones. However, there is a significant gap in volcanic activity from 24 to 87 Ma, excluding the 44 Ma Malaita volcanism. Raising the question, what mechanism could produce a 63 Ma gap in an otherwise enduring hotspot track?
It has long been observed that most hotspot tracks manifest as discrete volcanoes, exemplified by the long-lived Hawaii-Emperor Volcanic Chain, rather than continuous ridges. It is suggested that the locations of these volcanoes are controlled by fractures within the lithosphere, facilitating the migration of plume-generated magma (e.g., Hieronymus & Bercovici, 1999). Consequently, discrete volcanoes are anticipated along hotspot tracks.
To explain the bilaterally zoned hotspot tracks (e.g., Abouchami et al., 2005; Huang et al., 2011; Weis et al., 2011), Rohde et al. (2013) argued that mantle plumes originating from the lower mantle may bifurcate at the mantle transition zone (Figure 1a). Because of the different mantle viscosities in the upper and lower mantle, a plume might rise much slower in the lower mantle compared to in the upper mantle. To maintain the same plume flux, a plume would become thinner in the upper mantle, which may lead to plume bifurcation at the mantle transition zone (Rohde et al., 2013). Alternatively, it is also possible that after entering the upper mantle, a plume fragments into discrete upwelling diapirs rather than maintaining a continuous flow (Figure 1a), resulting in volcanic activity gaps along hotspot tracks.
However, neither of these theories explains the prolonged absence of volcanism within a significant period (24–87 Ma) of the Samoan hotspot track. Jackson et al. (2024) noted that during this particular period of time, the Samoan plume was under the thick OJP. Mantle plumes ascend adiabatically, with a steeper pressure-temperature slope compared to that of the mantle solidus. As such, plumes start to melt and produce magma when reaching shallow depths (low pressure). The upwelling stops at the base of rigid lithosphere, halting partial melting. Jackson et al. (2024) argued that the OJP's lithosphere is sufficiently thick to inhibit the plume's ascent to a shallow enough depth for melting, thus precluding volcanic activity and creating a seamount-free corridor (Figure 1b).
However, if the lithosphere is not thick enough to completely prevent a plume from melting and if a plume contains both an enriched lithology with a lower melting point and a refractory lithology with a higher melting point, the enriched lithology will melt preferentially (e.g., Phipps Morgan, 2001; Stracke & Bourdon, 2009). This results in magmas produced under thicker lithosphere having more enriched geochemical signatures (Figure 1b), as observed at the Emperor Seamount Chain (Frey et al., 2005; Regelous et al., 2003) and the Magellan seamounts, the Cretaceous Samoan volcanoes (Jackson et al., 2024).
Key geochemical signatures linking Magellan seamount lavas to Samoa include their distinctively high 87Sr/86Sr and low 143Nd/144Nd ratios, characteristic of the Enriched Mantle 2 (EM-2) mantle endmember, which is indicative of recycled ancient continental material in their mantle source (Jackson et al., 2007). However, it remains to be better elucidated where the Samoan plume, and mantle plumes in general, originates from. Are mantle endmembers, such as EM-2, inferred based on geochemical data of plume-derived lavas related to large mantle structures imaged by seismic waves, such as Large Low-Shear-Velocity Provinces (LLSVPs) in the deep mantle (e.g., Huang et al., 2011; Koppers et al., 2021; Weis et al., 2011, 2023)?
The findings of Jackson et al. (2024) suggest that the global plume flux might be underestimated if based solely on hotspot volcanic flux, as plume productivity can be suppressed under thick lithosphere. Furthermore, the isotopic compositions of erupted hotspot lavas may not be representative of their mantle source characteristics, as they are biased toward the enriched endmembers. If the enriched mantle endmembers contain recycled ancient surface materials, such as sediments, continental and oceanic crusts, their proportions in mantle plumes may be overestimated. They all hold significant implications for advancing our understanding of mantle dynamics.
The authors declare no conflicts of interest relevant to this study.