HR: 0800h
AN: U41A-0731 [Abstracts]
TI: Experimental Insights on the Thermochemical State of the Lower Mantle: Convection, Chemical
Heterogeneities, and the D" layer
AU: * Badro, J
EM: badro@lmcp.jussieu.fr
AF: Institut de Physique du Globe de Paris, Laboratoire de Mineralogie Cristallographie (UMR CNRS 7590), 140
rue de Lourmel, Paris, 75015
France
AU: Fiquet, G
EM: fiquet@lmcp.jussieu.fr
AF: Institut de Physique du Globe de Paris, Laboratoire de Mineralogie Cristallographie (UMR CNRS 7590), 140
rue de Lourmel, Paris, 75015
France
AU: Guyot, F
EM: guyot@lmcp.jussieu.fr
AF: Institut de Physique du Globe de Paris, Laboratoire de Mineralogie Cristallographie (UMR CNRS 7590), 140
rue de Lourmel, Paris, 75015
France
AB:
We report recent findings in the field of high-pressure mineral physics with important implications for Earth's lower mantle.
We find that the two main constituents of the lower mantle, namely (Mg,Fe)SiO$_3$ - magnesium silicate perovskite - and
(Mg,Fe)O - magnesiow\"ustite -, undergo electronic transitions at lower mantle pressures, in which iron is transforms from
the high-spin state to the low-spin state. The transformations should profoundly alter the thermochemical state of Earth's
lower mantle. Minerals bearing high-spin iron have characteristic absorption lines in the near-infrared, hindering radiative
conductivity at lower-mantle temperatures. These absorption lines shift in low-spin iron-bearing minerals to the visible
range (green to violet), and their intrinsic intensities decrease; the minerals thus become transparent in the near-infrared
and their radiative conductivity (and therefore total thermal conductivity) increases. Other issues at stake are that of
melting temperature or iron partitioning between mineral phases or even between various crystallographic sites of a mineral
phase. The two transition pressures correspond to the bottom third of the lower mantle (70 GPa, 1700 km depth), and to the
last 300 km above the core-mantle boundary (120 GPa, 2600 km depth); these regions have very special geophysical signatures,
since chemical heterogeneities have been reported in the bottom third of the lower mantle, and that the bottom 300 km of
Earth's mantle is constituted by the D" layer. Our observations could provide a mineral physics basis for these two regions
of Earth's lower mantle. The implications of these transitions on the dynamics of the lower mantle will be discussed.
DE: 5109 Magnetic and electrical properties
DE: 3630 Experimental mineralogy and petrology
DE: 3924 High-pressure behavior
DE: 3954 X ray, neutron, and electron spectroscopy and diffraction
DE: 1025 Composition of the mantle
SC: Union [U]
MN: 2004 AGU Fall Meeting