2019
DOI: 10.1029/2019gl083472
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First‐Principles Determination of the Dissociation Phase Boundary of Phase H MgSiO4H2

Abstract: Phase H (MgSiO4H2) is considered an important carrier of water into the lower mantle by the subduction of slabs. This phase has been reported to decompose into H2O ice VII and MgSiO3 bridgmanite under pressure. However, the dissociation phase boundary under the mantle pressure and temperature conditions has not been determined thus far. In this work, the dissociation phase boundary of phase H is determined by the calculation of Gibbs free energy of H2O ice VII. The stability field of phase H is found to be sig… Show more

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Cited by 12 publications
(5 citation statements)
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“…Recently discovered phase H (MgSiO4H2) stable at high pressures above 48 GPa, may preserve water in the lower mantle [8], however, later it was shown to dissociate into MgSiO3 (bridgmanite) and H2O (ice-Ⅷ) when pressure is further increased to ~52 GPa (first-principles prediction) [9] or to ~60 GPa (experiment) [10]. Furthermore, phase H is unstable at high temperatures, its upper dissociation boundary being ~1500 K [11] predicted using first-principles calculations within the quasiharmonic approximation (QHA). Such temperatures can only be found in the coldest parts of the lower mantle, in particular, in subducted lithospheric slabs, which are typically ~500 K colder than normal mantle, thus restricting possible abundance of phase H in the mantle.…”
mentioning
confidence: 99%
“…Recently discovered phase H (MgSiO4H2) stable at high pressures above 48 GPa, may preserve water in the lower mantle [8], however, later it was shown to dissociate into MgSiO3 (bridgmanite) and H2O (ice-Ⅷ) when pressure is further increased to ~52 GPa (first-principles prediction) [9] or to ~60 GPa (experiment) [10]. Furthermore, phase H is unstable at high temperatures, its upper dissociation boundary being ~1500 K [11] predicted using first-principles calculations within the quasiharmonic approximation (QHA). Such temperatures can only be found in the coldest parts of the lower mantle, in particular, in subducted lithospheric slabs, which are typically ~500 K colder than normal mantle, thus restricting possible abundance of phase H in the mantle.…”
mentioning
confidence: 99%
“…In a cold slab, Phase H, which may be transformed from phase D around the depth of 1,000 km (Tsuchiya, 2013), will undergo the dehydration reaction (normalPhase0.25emnormalH=normalBridgmanite+H2normalO $\mathrm{Phase}\,\mathrm{H}=\mathrm{Bridgmanite}+{\mathrm{H}}_{2}\mathrm{O}$) at the depth of ∼1,300–1,700 km (52–69 GPa) (Nishi et al., 2018; Ohtani et al., 2014; Tsuchiya, 2013; Tsuchiya & Umemoto, 2019; Walter et al., 2015). The form of H 2 O released by the dehydration of phase H is still debatable.…”
Section: Discussionmentioning
confidence: 99%
“…Schwager et al (2004) and Schwegler et al (2008) reported that ice-VII can be stable up to normal-mantle temperature above 50 GPa. Other studies suggest that phase H dehydrates above the melting temperature of ice-VII at 50 GPa (Goncharov et al, 2005;Kimura et al, 2014;Millot et al, 2018;Redmer et al, 2011;Tsuchiya & Umemoto, 2019), while the form of H 2 O released by the dehydration of phase H may be superionic ice (Millot et al, 2018;Redmer et al, 2011) or liquid water (Goncharov et al, 2005;Kimura et al, 2014) at 60 GPa. Here we assume that the dehydration will produce the liquid water that may migrate away.…”
Section: The Dehydration Of Phase Hmentioning
confidence: 98%
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