TY - JOUR
T1 - Stability of Fe-Ni hydride after the reaction between Fe-Ni alloy and hydrous phase (δ-AlOOH) up to 1.2Mbar
T2 - Possibility of H contribution to the core density deficit
AU - Terasaki, Hidenori
AU - Ohtani, Eiji
AU - Sakai, Takeshi
AU - Kamada, Seiji
AU - Asanuma, Hidetoshi
AU - Shibazaki, Yuki
AU - Hirao, Naohisa
AU - Sata, Nagayoshi
AU - Ohishi, Yasuo
AU - Sakamaki, Tatsuya
AU - Suzuki, Akio
AU - Funakoshi, Ken ichi
N1 - Funding Information:
We thank A. Sano, Y. Higo, and T. Kondo for technical support and discussions. We also thank Y. Fukai for constructive comments. T. Kuribayashi kindly provided the diaspore crystal. We also thank to anonymous reviewers for their constructive comments. This research was supported by grants from the Japan Society for the Promotion of Science (Grant numbers: 18104009 and 22000002 ) to EO and by the “Global Education and Research Center for the Earth and Planetary Dynamics”. The experiments were performed under contract at SPring-8 (proposal numbers: 2007A1731, 2007B1476 and 2008A1145).
PY - 2012/3
Y1 - 2012/3
N2 - The hydrous mineral, δ-AlOOH, is stable up to at least the core-mantle boundary, and therefore has been proposed as a water carrier to the Earth's deep mantle. If δ-AlOOH is transported down to the core-mantle boundary by a subducting slab or the mantle convection, then the reaction between the iron alloy core and δ-AlOOH is important in the deep water/hydrogen cycle in the Earth. Here we conducted an in situ X-ray diffraction study to determine the behavior of hydrogen between Fe-Ni alloys and δ-AlOOH up to near the core-mantle boundary conditions. The obtained diffraction spectra show that fcc/dhcp Fe-Ni hydride is stable over a wide pressure range of 19-121. GPa at high temperatures. Although the temperature of formation of Fe-Ni hydride tends to increase up to 1950. K with increasing pressure to 121. GPa, this reaction temperature is well below the mantle geotherm. δ-AlOOH was confirmed to coexist stably with perovskite, suggesting that δ-AlOOH can be a major hydrous phase in the lower mantle. Therefore, when δ-AlOOH contacts with the core at the core-mantle boundary, the hydrogen is likely to dissolve into the Earth's core. Based on the present results, the amount of hydrogen to explain the core density deficit is estimated to be 1.0-2.0 wt%.
AB - The hydrous mineral, δ-AlOOH, is stable up to at least the core-mantle boundary, and therefore has been proposed as a water carrier to the Earth's deep mantle. If δ-AlOOH is transported down to the core-mantle boundary by a subducting slab or the mantle convection, then the reaction between the iron alloy core and δ-AlOOH is important in the deep water/hydrogen cycle in the Earth. Here we conducted an in situ X-ray diffraction study to determine the behavior of hydrogen between Fe-Ni alloys and δ-AlOOH up to near the core-mantle boundary conditions. The obtained diffraction spectra show that fcc/dhcp Fe-Ni hydride is stable over a wide pressure range of 19-121. GPa at high temperatures. Although the temperature of formation of Fe-Ni hydride tends to increase up to 1950. K with increasing pressure to 121. GPa, this reaction temperature is well below the mantle geotherm. δ-AlOOH was confirmed to coexist stably with perovskite, suggesting that δ-AlOOH can be a major hydrous phase in the lower mantle. Therefore, when δ-AlOOH contacts with the core at the core-mantle boundary, the hydrogen is likely to dissolve into the Earth's core. Based on the present results, the amount of hydrogen to explain the core density deficit is estimated to be 1.0-2.0 wt%.
KW - Core density deficit
KW - Hydride
KW - Hydrogen
KW - δ-AlOOH
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U2 - 10.1016/j.pepi.2012.01.002
DO - 10.1016/j.pepi.2012.01.002
M3 - Article
AN - SCOPUS:84856994292
SN - 0031-9201
VL - 194-195
SP - 18
EP - 24
JO - Physics of the Earth and Planetary Interiors
JF - Physics of the Earth and Planetary Interiors
ER -