{"title":"汤加-凯尔马代克海沟海域路易斯维尔海脊的 Vp/Vs 结构和 Pn 各向异性","authors":"Eduardo Contreras-Reyes , Ingo Grevemeyer , Christine Peirce , Sebastián Obando-Orrego","doi":"10.1016/j.tecto.2024.230417","DOIUrl":null,"url":null,"abstract":"<div><p>The Pacific Plate within the collision zone between the Louisville Ridge and the Tonga-Kermadec Trench was formed at the Osbourn Trough, a paleo spreading center that became inactive during the Cretaceous. In this region, the trench shallows from a depth of 8–11 km to ∼6 km below sea surface, while the outer rise topography is obscured by Louisville seamounts that rise 4–5 km above the adjacent seafloor. We derive 2-D P-wave (<em>V</em><sub><em>p</em></sub>) and S-wave (<em>V</em><sub><em>s</em></sub>) velocity-depth models along a wide-angle seismic profile oriented sub-parallel to the trench axis, intersecting the 27.6°S seamount. The seismic profile is located in the down-going Pacific Plate eastwards from the trench axis (∼100 km distant at the south end and ∼ 150 km at the north end), where bending-related faulting is limited or absent. Using the derived P- and S-wave velocity-depth models we calculate the corresponding <em>V</em><sub><em>p</em></sub>/<em>V</em><sub><em>s</em></sub> ratio model which shows values of 1.7–1.85 throughout the oceanic crust either side of the Louisville Ridge where it is unaffected by magmatism associated with its formation. This range of observations lies within those documented by laboratory measurements on basalt, diabase, and gabbro. Conversely, in the vicinity of the summit of 27.6°S seamount, the relatively elevated <em>V</em><sub><em>p</em></sub>/<em>V</em><sub><em>s</em></sub> (∼1.9) ratio observed can be attributed to water-saturated cracks within the shallow sub-seabed section of the intrusive core. Beneath the seamount the uppermost mantle has a <em>V</em><sub><em>p</em></sub> ranging from 8.0 to 8.9 km/s. Comparing our P-wave model with a pre-existing model running sub-perpendicularly along the Louisville Ridge axis, we observe an anisotropy of up to ∼6% at a depth of 3–4 km below the Moho. The predominant orientation of the faster axis follows the direction of paleo spreading flow when the plate was formed at the Osbourn Trough.</p></div>","PeriodicalId":22257,"journal":{"name":"Tectonophysics","volume":"885 ","pages":"Article 230417"},"PeriodicalIF":2.7000,"publicationDate":"2024-07-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Vp/Vs structure and Pn anisotropy across the Louisville Ridge, seaward of the Tonga-Kermadec Trench\",\"authors\":\"Eduardo Contreras-Reyes , Ingo Grevemeyer , Christine Peirce , Sebastián Obando-Orrego\",\"doi\":\"10.1016/j.tecto.2024.230417\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The Pacific Plate within the collision zone between the Louisville Ridge and the Tonga-Kermadec Trench was formed at the Osbourn Trough, a paleo spreading center that became inactive during the Cretaceous. In this region, the trench shallows from a depth of 8–11 km to ∼6 km below sea surface, while the outer rise topography is obscured by Louisville seamounts that rise 4–5 km above the adjacent seafloor. We derive 2-D P-wave (<em>V</em><sub><em>p</em></sub>) and S-wave (<em>V</em><sub><em>s</em></sub>) velocity-depth models along a wide-angle seismic profile oriented sub-parallel to the trench axis, intersecting the 27.6°S seamount. The seismic profile is located in the down-going Pacific Plate eastwards from the trench axis (∼100 km distant at the south end and ∼ 150 km at the north end), where bending-related faulting is limited or absent. Using the derived P- and S-wave velocity-depth models we calculate the corresponding <em>V</em><sub><em>p</em></sub>/<em>V</em><sub><em>s</em></sub> ratio model which shows values of 1.7–1.85 throughout the oceanic crust either side of the Louisville Ridge where it is unaffected by magmatism associated with its formation. This range of observations lies within those documented by laboratory measurements on basalt, diabase, and gabbro. Conversely, in the vicinity of the summit of 27.6°S seamount, the relatively elevated <em>V</em><sub><em>p</em></sub>/<em>V</em><sub><em>s</em></sub> (∼1.9) ratio observed can be attributed to water-saturated cracks within the shallow sub-seabed section of the intrusive core. Beneath the seamount the uppermost mantle has a <em>V</em><sub><em>p</em></sub> ranging from 8.0 to 8.9 km/s. Comparing our P-wave model with a pre-existing model running sub-perpendicularly along the Louisville Ridge axis, we observe an anisotropy of up to ∼6% at a depth of 3–4 km below the Moho. The predominant orientation of the faster axis follows the direction of paleo spreading flow when the plate was formed at the Osbourn Trough.</p></div>\",\"PeriodicalId\":22257,\"journal\":{\"name\":\"Tectonophysics\",\"volume\":\"885 \",\"pages\":\"Article 230417\"},\"PeriodicalIF\":2.7000,\"publicationDate\":\"2024-07-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Tectonophysics\",\"FirstCategoryId\":\"89\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0040195124002191\",\"RegionNum\":3,\"RegionCategory\":\"地球科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"GEOCHEMISTRY & GEOPHYSICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Tectonophysics","FirstCategoryId":"89","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0040195124002191","RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"GEOCHEMISTRY & GEOPHYSICS","Score":null,"Total":0}
引用次数: 0
摘要
路易斯维尔海脊与汤加-克马德克海沟碰撞区内的太平洋板块是在奥斯本海槽形成的,奥斯本海槽是一个古扩张中心,在白垩纪期间变得不活跃。在这一区域,海沟从 8-11 千米深浅至海面以下 6 千米,而外部隆起的地形被路易斯维尔海山所遮挡,这些海山高出邻近海底 4-5 千米。我们沿着与海沟轴线次平行、与南纬 27.6 度海山相交的广角地震剖面,推导出二维 P 波(Vp)和 S 波(Vs)速度深度模型。地震剖面位于海沟轴线向东的下行太平洋板块(南端距离海沟轴线 100 千米,北端距离海沟轴线 150 千米),这里与弯曲有关的断层有限或不存在。利用推导出的 P 波和 S 波速度深度模型,我们计算了相应的 Vp/Vs 比值模型,结果显示路易斯维尔海脊两侧的整个大洋地壳的 Vp/Vs 比值为 1.7-1.85,而路易斯维尔海脊的形成未受到岩浆活动的影响。这一观测范围与实验室对玄武岩、辉绿岩和辉长岩的测量结果一致。相反,在南纬 27.6 度海山山顶附近,观察到相对较高的 Vp/Vs 比值(1.9∼1.9),这可归因于侵入岩芯浅海底段内的水饱和裂缝。在海山下面,最上层地幔的 Vp 为 8.0 至 8.9 千米/秒。将我们的 P 波模型与沿路易斯维尔海脊轴线次垂直运行的已有模型进行比较,我们观察到在莫霍面以下 3-4 千米深处的各向异性高达 ∼6%。快轴的主要方向与奥斯本海槽板块形成时的古扩张流方向一致。
Vp/Vs structure and Pn anisotropy across the Louisville Ridge, seaward of the Tonga-Kermadec Trench
The Pacific Plate within the collision zone between the Louisville Ridge and the Tonga-Kermadec Trench was formed at the Osbourn Trough, a paleo spreading center that became inactive during the Cretaceous. In this region, the trench shallows from a depth of 8–11 km to ∼6 km below sea surface, while the outer rise topography is obscured by Louisville seamounts that rise 4–5 km above the adjacent seafloor. We derive 2-D P-wave (Vp) and S-wave (Vs) velocity-depth models along a wide-angle seismic profile oriented sub-parallel to the trench axis, intersecting the 27.6°S seamount. The seismic profile is located in the down-going Pacific Plate eastwards from the trench axis (∼100 km distant at the south end and ∼ 150 km at the north end), where bending-related faulting is limited or absent. Using the derived P- and S-wave velocity-depth models we calculate the corresponding Vp/Vs ratio model which shows values of 1.7–1.85 throughout the oceanic crust either side of the Louisville Ridge where it is unaffected by magmatism associated with its formation. This range of observations lies within those documented by laboratory measurements on basalt, diabase, and gabbro. Conversely, in the vicinity of the summit of 27.6°S seamount, the relatively elevated Vp/Vs (∼1.9) ratio observed can be attributed to water-saturated cracks within the shallow sub-seabed section of the intrusive core. Beneath the seamount the uppermost mantle has a Vp ranging from 8.0 to 8.9 km/s. Comparing our P-wave model with a pre-existing model running sub-perpendicularly along the Louisville Ridge axis, we observe an anisotropy of up to ∼6% at a depth of 3–4 km below the Moho. The predominant orientation of the faster axis follows the direction of paleo spreading flow when the plate was formed at the Osbourn Trough.
期刊介绍:
The prime focus of Tectonophysics will be high-impact original research and reviews in the fields of kinematics, structure, composition, and dynamics of the solid arth at all scales. Tectonophysics particularly encourages submission of papers based on the integration of a multitude of geophysical, geological, geochemical, geodynamic, and geotectonic methods