Electromagnetic constraints on a melt region beneath the central Mariana back-arc spreading ridge

dc.contributor.author Matsuno, Tetsuo
dc.contributor.author Evans, Rob L.
dc.contributor.author Seama, Nobukazu
dc.contributor.author Chave, Alan D.
dc.date.accessioned 2012-12-10T20:10:17Z
dc.date.available 2014-10-22T08:57:23Z
dc.date.issued 2012-10-25
dc.description Author Posting. © American Geophysical Union, 2012. This article is posted here by permission of American Geophysical Union for personal use, not for redistribution. The definitive version was published in Geochemistry Geophysics Geosystems 13 (2012): Q10017, doi:10.1029/2012GC004326. en_US
dc.description.abstract An electrical resistivity profile across the central Mariana subduction system shows high resistivity in the upper mantle beneath the back-arc spreading ridge where melt might be expected to exist. Although seismic data are equivocal on the extent of a possible melt region, the question arises as to why a 2-D magnetotelluric (MT) survey apparently failed to image any melt. We have run forward models and inversions that test possible 3-D melt geometries that are consistent with the MT data and results of other studies from the region, and that we use to place upper bounds on the possible extent of 3-D melt region beneath the spreading center. Our study suggests that the largest melt region that was not directly imaged by the 2-D MT data, but that is compatible with the observations as well as the likely effects of melt focusing, has a 3-D shape on a ridge-segment scale focused toward the spreading center and a resistivity of 100 Ω-m that corresponds to ∼0.1–∼1% interconnected silicate melt embedded in a background resistivity of ∼500 Ω-m. In contrast to the superfast spreading southern East Pacific Rise, the 3-D melt region suggests that buoyant mantle upwelling on a ridge-segment scale is the dominant process beneath the slow-spreading central Mariana back-arc. A final test considers whether the inability to image a 3-D melt region was a result of the 2-D survey geometry. The result reveals that the 2-D transect completed is useful to elucidate a broad range of 3-D melt bodies. en_US
dc.description.embargo 2013-04-25 en_US
dc.description.sponsorship TM and NS are supported by the scientific program of “TAIGA” (Trans-crustal Advection and In situ reaction of Global sub-seafloor Aquifer)” sponsored by the MEXT of Japan, and are also supported by the JSPS for Grant-In-Aid for Scientific Research (21244070). Participation in the Marianas experiment by RLE and ADC was supported by NSF grant OCE0405641. en_US
dc.format.mimetype application/pdf
dc.identifier.citation Geochemistry Geophysics Geosystems 13 (2012): Q10017 en_US
dc.identifier.doi 10.1029/2012GC004326
dc.identifier.uri https://hdl.handle.net/1912/5604
dc.language.iso en_US en_US
dc.publisher American Geophysical Union en_US
dc.relation.uri https://doi.org/10.1029/2012GC004326
dc.subject Back-arc spreading ridge en_US
dc.subject Central Mariana Trough en_US
dc.subject Electrical resistivity structure en_US
dc.subject Upper mantle melting en_US
dc.title Electromagnetic constraints on a melt region beneath the central Mariana back-arc spreading ridge en_US
dc.type Article en_US
dspace.entity.type Publication
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relation.isAuthorOfPublication.latestForDiscovery c7d0ac88-6302-41d3-b3d4-af8103395155
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