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DAC measurement of perovskite conductivity and implications for the distribution of mineral phases in the lower mantle
Author(s) -
Duba Alfred G.,
Wanamaker Barbara J.
Publication year - 1994
Publication title -
geophysical research letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.007
H-Index - 273
eISSN - 1944-8007
pISSN - 0094-8276
DOI - 10.1029/94gl01165
Subject(s) - wüstite , electrical resistivity and conductivity , perovskite (structure) , olivine , mantle (geology) , conductivity , stishovite , materials science , mineralogy , silicate perovskite , geology , pyroxene , magnetite , metallurgy , geochemistry , chemistry , crystallography , quartz , electrical engineering , engineering
Measurements of the electrical conductivity of olivine buffered by magnesiowüstite can increase by more than two orders of magnitude if as little as 2 × 10 −3 percent of the magnesiowüstite is allowed to form a parallel conduction path between the electrodes. These results are used, in concert with recent petrologic studies of the distribution of iron between perovskite and magnesiowüstite that have been synthesized from iron‐bearing olivine, to show how most of the inconsistencies in diamond‐anvil‐cell electrical conductivity measurements of perovskite may be explained by the presence of highly conductive, through‐going magnesiowüstite layers in laser‐heated samples, including those synthesized from pyroxene. Without electrical conductivity measurements on perovskite uncontaminated with secondary phases, current laboratory data can be interpreted—within constraints provided by the electrical conductivity of the mantle from geomagnetic studies—as requiring that either the conductivity of perovskite is not much different from magnesiowüstite or that magnesiowüstite in the lower mantle is distributed heterogeneously as an interconnected through‐going phase.