TY - JOUR
T1 - Post-spinel transition in Mg2SiO4 determined by high P - T in situ X-ray diffractometry
AU - Katsura, Tomoo
AU - Yamada, Hitoshi
AU - Shinmei, Toru
AU - Kubo, Atsushi
AU - Ono, Shigeaki
AU - Kanzaki, Masami
AU - Yoneda, Akira
AU - Walter, Michael J.
AU - Ito, Eiji
AU - Urakawa, Satoru
AU - Funakoshi, Kenichi
AU - Utsumi, Wataru
PY - 2003/4/15
Y1 - 2003/4/15
N2 - The phase boundary of the post-spinel transition in Mg2SiO4 was re-investigated by means of high P - T in situ X-ray diffractometry with a gold pressure marker in a Kawai-type apparatus. Rapid and continuous temperature changes were conducted to initiate dissociation of spinel, which tends to be inert after long annealing. Isothermal decompression at high temperature was conducted to form spinel from perovskite plus periclase. The phase boundary is located at ca. 22 GPa in the temperature range from 1550 to 2100 K, which is 1-1.5 GPa lower than the 660 km discontinuity. This discrepancy might be explained in terms of the pressure effect of thermocouple emf and inaccurate equation of state (EOS) for the pressure maker. The transition is found to be less sensitive to temperature than reported previously, with a Clapeyron slope ranging from -2 to -0.4 MPa/K. This small Clapeyron slope implies that the post-spinel transition would not be an effective barrier to mantle convection.
AB - The phase boundary of the post-spinel transition in Mg2SiO4 was re-investigated by means of high P - T in situ X-ray diffractometry with a gold pressure marker in a Kawai-type apparatus. Rapid and continuous temperature changes were conducted to initiate dissociation of spinel, which tends to be inert after long annealing. Isothermal decompression at high temperature was conducted to form spinel from perovskite plus periclase. The phase boundary is located at ca. 22 GPa in the temperature range from 1550 to 2100 K, which is 1-1.5 GPa lower than the 660 km discontinuity. This discrepancy might be explained in terms of the pressure effect of thermocouple emf and inaccurate equation of state (EOS) for the pressure maker. The transition is found to be less sensitive to temperature than reported previously, with a Clapeyron slope ranging from -2 to -0.4 MPa/K. This small Clapeyron slope implies that the post-spinel transition would not be an effective barrier to mantle convection.
KW - 660 km discontinuity
KW - High pressures and temperatures
KW - In situ X-ray diffractometry
KW - Mantle
KW - MgSiO
KW - Post-spinel transition
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U2 - 10.1016/S0031-9201(03)00019-0
DO - 10.1016/S0031-9201(03)00019-0
M3 - Article
AN - SCOPUS:0037531586
SN - 0031-9201
VL - 136
SP - 11
EP - 24
JO - Physics of the Earth and Planetary Interiors
JF - Physics of the Earth and Planetary Interiors
IS - 1-2
ER -