TY - JOUR
T1 - Spin transition of Fe3+ in Al-bearing phase D
T2 - An alternative explanation for small-scale seismic scatterers in the mid-lower mantle
AU - Chang, Yun Yuan
AU - Jacobsen, Steven D.
AU - Lin, Jung Fu
AU - Bina, Craig R.
AU - Thomas, Sylvia Monique
AU - Wu, Junjie
AU - Shen, Guoyin
AU - Xiao, Yuming
AU - Chow, Paul
AU - Frost, Daniel J.
AU - McCammon, Catherine A.
AU - Dera, Przemyslaw
N1 - Funding Information:
This research was supported by the Carnegie/DOE Alliance Center (CDAC ) and by US NSF grants EAR-0748707 (CAREER) to S.D.J. and by EAR-1056670 and EAR-1053446 to J.F.L. Additional support was provided by the David and Lucile Packard Foundation to S.D.J. Portions of this work were performed at HPCAT (Sector 16), Advanced Photon Source (APS), Argonne National Laboratory. HPCAT operations are supported by DOE-NNSA under Award No. DE-NA0001974 and DOE-BES under Award No. DE-FG02-99ER45775 , with partial instrumentation funding by NSF. Use of the COMPRES-GSECARS gas loading system was supported by COMPRES under NSF Cooperative Agreement EAR 11-57758 and by GSECARS through NSF grant EAR-1128799 and DOE grant DE-FG02-94ER14466 . Use of the Advanced Photon Source was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences , Contract No. DE-AC02-06CH11357 .
PY - 2013/11/15
Y1 - 2013/11/15
N2 - Among dense-hydrous magnesium silicates potentially transporting H2O into Earth's deep interior, phase D (MgSi2H2O6) exhibits the highest P-T stability range, extending into the lower mantle along cold slab geotherms. We have studied the compressibility and spin state of Fe in Al-bearing phase D up to 90 GPa using synchrotron X-ray diffraction and X-ray emission spectroscopy. Fe-Al-bearing phase D was synthesized at 25 GPa and 1400 °C with approximate composition MgSi1.5Fe0.15Al0.32H2.6O6, where nearly all of the Fe is ferric (Fe3+). Analysis of Fe-Kβ emission spectra reveals a gradual, pressure-induced high-spin (HS) to low-spin (LS) transition of Fe3+ extending from 40 to 65 GPa. The fitted equation of state for high-spin Fe-Al-bearing phase D results in a bulk modulus KT0 = 147(2) GPa with pressure derivative K ' = 6.3(3). An equation of state over the entire pressure range was calculated using the observed variation in low-spin fraction with pressure and a low-spin bulk modulus of KT0 = 253(30) GPa, derived from the data above 65 GPa. Pronounced softening in the bulk modulus occurs during the spin transition, reaching a minimum at 50 GPa (~1500 km) where the bulk modulus of Fe-Al phase D is about 35% lower than Fe-Al-bearing silicate perovskite. Recovery of the bulk modulus at 50-65 GPa results in a structure that has a similar incompressibility as silicate perovskite above 65 GPa. Similarly, the bulk sound velocity of Fe-Al phase D reaches a minimum at ~50 GPa, being about 10% slower than silicate perovskite. The potential association of Fe-Al phase D with subducted slabs entering the lower mantle, along with its elastic properties through the Fe3+ spin transition predicted at 1200-1800 km, suggests that phase D may provide an alternative explanation for small-scale mid-lower mantle seismic scatterers and supports the presence of deeply recycled sediments in the lower mantle.
AB - Among dense-hydrous magnesium silicates potentially transporting H2O into Earth's deep interior, phase D (MgSi2H2O6) exhibits the highest P-T stability range, extending into the lower mantle along cold slab geotherms. We have studied the compressibility and spin state of Fe in Al-bearing phase D up to 90 GPa using synchrotron X-ray diffraction and X-ray emission spectroscopy. Fe-Al-bearing phase D was synthesized at 25 GPa and 1400 °C with approximate composition MgSi1.5Fe0.15Al0.32H2.6O6, where nearly all of the Fe is ferric (Fe3+). Analysis of Fe-Kβ emission spectra reveals a gradual, pressure-induced high-spin (HS) to low-spin (LS) transition of Fe3+ extending from 40 to 65 GPa. The fitted equation of state for high-spin Fe-Al-bearing phase D results in a bulk modulus KT0 = 147(2) GPa with pressure derivative K ' = 6.3(3). An equation of state over the entire pressure range was calculated using the observed variation in low-spin fraction with pressure and a low-spin bulk modulus of KT0 = 253(30) GPa, derived from the data above 65 GPa. Pronounced softening in the bulk modulus occurs during the spin transition, reaching a minimum at 50 GPa (~1500 km) where the bulk modulus of Fe-Al phase D is about 35% lower than Fe-Al-bearing silicate perovskite. Recovery of the bulk modulus at 50-65 GPa results in a structure that has a similar incompressibility as silicate perovskite above 65 GPa. Similarly, the bulk sound velocity of Fe-Al phase D reaches a minimum at ~50 GPa, being about 10% slower than silicate perovskite. The potential association of Fe-Al phase D with subducted slabs entering the lower mantle, along with its elastic properties through the Fe3+ spin transition predicted at 1200-1800 km, suggests that phase D may provide an alternative explanation for small-scale mid-lower mantle seismic scatterers and supports the presence of deeply recycled sediments in the lower mantle.
KW - Dense hydrous magnesium silicate
KW - Lower mantle
KW - Phase D
KW - Seismic scatterers
KW - Spin transition
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U2 - 10.1016/j.epsl.2013.08.038
DO - 10.1016/j.epsl.2013.08.038
M3 - Article
AN - SCOPUS:84884358266
SN - 0012-821X
VL - 382
SP - 1
EP - 9
JO - Earth and Planetary Science Letters
JF - Earth and Planetary Science Letters
ER -