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Anatomy of a pressure-induced, ferromagnetic-to-paramagnetic transition in pyrrhotite: Implications for the formation pressure of diamonds

机译:磁黄铁矿中压力诱导的铁磁 - 顺磁转变的剖析:对钻石形成压力的影响

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摘要

Meteorites and diamonds encounter high pressures during their formation or subsequent evolution. These materials commonly contain magnetic inclusions of pyrrhotite. Because magnetic properties are sensitive to strain, pyrrhotite can potentially record the shock or formation pressures of its host. Moreover, pyrrhotite undergoes a pressure-induced phase transition between 1.6 and 6.2 GPa, but the magnetic signature of this transition is poorly known. Here we report room temperature magnetic measurements on multidomain and single-domain pyrrhotite under nonhydrostatic pressure. Magnetic remanence in single-domain pyrrhotite is largely insensitive to pressure until 2 GPa, whereas the remanence of multidomain pyrrhotite increases 50\% over that of initial conditions by 2 GPa, and then decreases until only 33\% of the original remanence remains by 4.5 GPa. In contrast, magnetic coercivity increases with increasing pressure to 4.5 GPa. Below ∼1.5 GPa, multidomain pyrrhotite obeys Néel theory with a positive correlation between coercivity and remanence; above ∼1.5 GPa, it behaves single domain-like yet distinctly different from uncompressed single-domain pyrrhotite. The ratio of magnetic coercivity and remanence follows a logarithmic law with respect to pressure, which can potentially be used as a geobarometer. Owing to the greater thermal expansion of pyrrhotite with respect to diamond, pyrrhotite inclusions in diamonds experience a confining pressure at Earth’s surface. Applying our experimentally derived magnetic geobarometer to pyrrhotite-bearing diamonds from Botswana and the Central African Republic suggests the pressures of the pyrrhotite inclusions in the diamonds range from 1.3 to 2.1 GPa. These overpressures constrain the mantle source pressures from 5.4 to 9.5 GPa, depending on which bulk modulus and thermal expansion coefficients of the two phases are used.
机译:陨石和钻石在形成或随后的演化过程中会遇到高压。这些材料通常包含磁黄铁矿的磁性夹杂物。由于磁性能对应变敏感,因此磁黄铁矿可能会记录其主体的震动或地层压力。此外,黄铁矿经历了1.6至6.2 GPa的压力诱导相变,但是这种转变的磁性特征却鲜为人知。在这里,我们报告了在非静水压力下对多畴和单畴黄铁矿的室温磁测量。直到2 GPa,单畴黄铁矿的剩磁对压力基本不敏感,而多畴黄铁矿的剩磁比初始条件高25%,比初始条件高50%,然后下降,直到原始剩磁仅剩4.5%。 GPa。相反,磁矫顽力随压力增加至4.5 GPa而增加。低于〜1.5 GPa,多畴黄铁矿服从Néel理论,矫顽力和剩磁之间呈正相关;高于〜1.5 GPa,它的行为类似于单畴,但与未压缩的单畴黄铁矿明显不同。磁矫顽力和剩磁的比率相对于压力遵循对数定律,可以用作气压计。由于磁黄铁矿相对于金刚石的热膨胀更大,金刚石中的磁黄铁矿夹杂物在地球表面受到围压。将我们的实验得出的磁性气压计应用于来自博茨瓦纳和中非共和国的含黄铁矿的钻石,表明钻石中黄铁矿夹杂物的压力范围为1.3至2.1 GPa。这些超压将地幔源压力从5.4 GPa限制到9.5 GPa,这取决于使用两相的体积模量和热膨胀系数。

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