M-sequence geomagnetic polarity time scale (MHTC12) that steadies global spreading rates and incorporates astrochronology constraints

dc.contributor.author Malinverno, Alberto
dc.contributor.author Hildebrandt, Jordan
dc.contributor.author Tominaga, Masako
dc.contributor.author Channell, James E. T.
dc.date.accessioned 2012-08-01T16:08:43Z
dc.date.available 2014-10-22T08:57:23Z
dc.date.issued 2012-06-30
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 Journal of Geophysical Research 117 (2012): B06104, doi:10.1029/2012JB009260. en_US
dc.description.abstract Geomagnetic polarity time scales (GPTSs) have been constructed by interpolating between dated marine magnetic anomalies assuming uniformly varying spreading rates. A strategy to obtain an optimal GPTS is to minimize spreading rate fluctuations in many ridge systems; however, this has been possible only for a few spreading centers. We describe here a Monte Carlo sampling method that overcomes this limitation and improves GPTS accuracy by incorporating information on polarity chron durations estimated from astrochronology. The sampling generates a large ensemble of GPTSs that simultaneously agree with radiometric age constraints, minimize the global variation in spreading rates, and fit polarity chron durations estimated by astrochronology. A key feature is the inclusion and propagation of data uncertainties, which weigh how each piece of information affects the resulting time scale. The average of the sampled ensemble gives a reference GPTS, and the variance of the ensemble measures the time scale uncertainty. We apply the method to construct MHTC12, an improved version of the M-sequence GPTS (Late Jurassic-Early Cretaceous, ~160–120 Ma). This GPTS minimizes the variation in spreading rates in a global data set of magnetic lineations from the Western Pacific, North Atlantic, and Indian Ocean NW of Australia, and it also accounts for the duration of five polarity chrons established from astrochronology (CM0r through CM3r). This GPTS can be updated by repeating the Monte Carlo sampling with additional data that may become available in the future. en_US
dc.description.embargo 2012-12-30 en_US
dc.description.sponsorship A.M. and J.H. were supported by NSF grant OCE 09–26306, M.T. was supported by a Woods Hole Oceanographic Institution postdoctoral scholarship, and J.E.T.C. was supported by NSF grant OCE 09–60999. en_US
dc.format.mimetype application/pdf
dc.format.mimetype text/plain
dc.identifier.citation Journal of Geophysical Research 117 (2012): B06104 en_US
dc.identifier.doi 10.1029/2012JB009260
dc.identifier.uri https://hdl.handle.net/1912/5287
dc.language.iso en_US en_US
dc.publisher American Geophysical Union en_US
dc.relation.uri https://doi.org/10.1029/2012JB009260
dc.subject Monte Carlo simulation en_US
dc.subject Geomagnetic polarity time scale en_US
dc.subject Marine magnetic anomalies en_US
dc.title M-sequence geomagnetic polarity time scale (MHTC12) that steadies global spreading rates and incorporates astrochronology constraints en_US
dc.type Article en_US
dspace.entity.type Publication
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relation.isAuthorOfPublication.latestForDiscovery d9493b3d-f964-493e-8745-42302ec575c7
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Table S1: Geomagnetic polarity time scale MHTC12.
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Table S2: Geomagnetic polarity time scale MHTC12-125.
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