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MgSiO_3 phase boundaries measured in the laser-heated diamond cell

机译:在激光加热的金刚石电池中测得的MgSiO_3相界

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摘要

New data on phase equilibria in the MgSiO_3 system relevant to the stability of Mg–Si-perovskite (perovskite) are obtained in the laser-heated diamond cell using improved techniques for accurate pressure measurement and novel heating techniques eliminating temperature gradients. The data of the MgSiO_3-ilmenite (akimotoite)–perovskite phase boundary, measured in the range of 19–25.5 GPa and 1800–2350 K, are consistent with the pressure and temperature conditions generally assumed at 660 km depth and agree within the experimental uncertainties with earlier multi-anvil quench experiments. The triple point wadsleyite+stishovite–akimotoite–perovskite is at 21 GPa and 2300 K. The slope of the akimotoite–perovskite boundary is not well constrained by reversal experiments alone due to large hysteresis, but results using glass starting materials yield a value of -0.004±0.002 GPa/K. The slopes of the phase transitions to Mg–Si-perovskite in both olivine and pyroxene systems are less negative than those required to cause layering in mantle convection. At the pressure of the 660 km seismic discontinuity (23.8 GPa) the phase boundary between akimotoite and perovskite yields a slightly lower temperature than that of the ringwoodite to perovskite+periclase transition in the Mg2SiO_4 system (1900±100 K). Garnet (majorite) is not observed above 21 GPa.
机译:在MgSiO_3系统中,与Mg-Si-钙钛矿(钙钛矿)的稳定性有关的相平衡的新数据是在激光加热的金刚石电池中获得的,采用了改进的技术来进行精确的压力测量和消除温度梯度的新型加热技术。在19–25.5 GPa和1800–2350 K范围内测得的MgSiO_3-钛铁矿(akimotoite)-钙钛矿相界数据与通常假定在660 km深度的压力和温度条件一致,并且在实验不确定性范围内与早期的多砧淬火实验。三点瓦兹利石+钛辉石-akimotoite-钙钛矿的值为21 GPa和2300K。由于滞后现象较大,仅通过逆向实验不能很好地限制akimotoite-钙钛矿边界的斜率,但是使用玻璃原料得到的结果值为- 0.004±0.002 GPa / K。在橄榄石和辉石体系中,相转变为Mg-Si-钙钛矿的斜率都比引起地幔对流成层的斜率小。在660 km地震不连续性(23.8 GPa)的压力下,裸镁铁矿与钙钛矿之间的相界产生的温度略低于Mg2SiO_4系统中从菱铁矿到钙钛矿+钙蛋白酶的转变温度(1900±100 K)。在21 GPa以上未观察到石榴石(马氏体)。

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