TY - JOUR
T1 - Determination of post-perovskite phase transition boundary up to 4400 K and implications for thermal structure in D″ layer
AU - Tateno, Shigehiko
AU - Hirose, Kei
AU - Sata, Nagayoshi
AU - Ohishi, Yasuo
N1 - Funding Information:
We thank T. Komabayashi for the discussion throughout this study. K. Ohta, H. Ozawa, and E. Sugimura are acknowledged for their assistance in the synchrotron experiments. The starting material was provided by M. Murakami. We also thank N. Guignot and an anonymous referee, and the Editor for their thoughtful comments on the manuscript. X-ray diffraction measurements were conducted at SPring-8 (proposal no. 2007A0099 and 2007B0099). S.T. is supported by the Research Fellowships of the Japan Society for the Promotion of Science for Young Scientists.
PY - 2009/1/15
Y1 - 2009/1/15
N2 - We have determined the post-perovskite phase transition boundary in MgSiO3 in a wide temperature range from 1640 to 4380 K at 119-171 GPa on the basis of synchrotron X-ray diffraction measurements in-situ at high-pressure and -temperature in a laser-heated diamond-anvil cell (LHDAC). The results show a considerably high positive Clapeyron slope of + 13.3 ± 1.0 MPa/K and a transition temperature of about 3520 ± 70 K at the core-mantle boundary (CMB) pressure. The thermal structure in D″ layer can be tightly constrained from precisely determined post-perovskite phase transition boundary and the depths of paired seismic discontinuities. These suggest that temperature at the CMB may be around 3700 K, somewhat lower than previously thought. A minimum bound on the global heat flow from the core is estimated to be 6.6 ± 0.5 TW.
AB - We have determined the post-perovskite phase transition boundary in MgSiO3 in a wide temperature range from 1640 to 4380 K at 119-171 GPa on the basis of synchrotron X-ray diffraction measurements in-situ at high-pressure and -temperature in a laser-heated diamond-anvil cell (LHDAC). The results show a considerably high positive Clapeyron slope of + 13.3 ± 1.0 MPa/K and a transition temperature of about 3520 ± 70 K at the core-mantle boundary (CMB) pressure. The thermal structure in D″ layer can be tightly constrained from precisely determined post-perovskite phase transition boundary and the depths of paired seismic discontinuities. These suggest that temperature at the CMB may be around 3700 K, somewhat lower than previously thought. A minimum bound on the global heat flow from the core is estimated to be 6.6 ± 0.5 TW.
KW - core-mantle boundary
KW - in-situ X-ray diffraction
KW - lower mantle
KW - phase transition
KW - post-perovskite
UR - http://www.scopus.com/inward/record.url?scp=57749087824&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=57749087824&partnerID=8YFLogxK
U2 - 10.1016/j.epsl.2008.10.004
DO - 10.1016/j.epsl.2008.10.004
M3 - Article
AN - SCOPUS:57749087824
SN - 0012-821X
VL - 277
SP - 130
EP - 136
JO - Earth and Planetary Sciences Letters
JF - Earth and Planetary Sciences Letters
IS - 1-2
ER -