Equation of state and phase transition in KAlSi3O8 hollandite at high pressure
Equation of state and phase transition in KAlSi3O8 hollandite at high pressure
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DOI:
10.2138/am.2006.1879
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发表时间:
2006-02
影响因子:
3.1
通讯作者:
T. Ferroir;Tsuyoshi Onozawa;T. Yagi;S. Merkel;N. Miyajima;N. Nishiyama;T. Irifune;T. Kikegawa
中科院分区:
文献类型:
--
作者:
T. Ferroir;Tsuyoshi Onozawa;T. Yagi;S. Merkel;N. Miyajima;N. Nishiyama;T. Irifune;T. Kikegawa
Abstract The tetragonal hollandite structure (KAlSi3O8 hollandite) has been studied up to 32 GPa at room temperature using high-pressure in-situ X-ray diffraction techniques. A phase transformation from tetragonal I4/m phase to a new phase was found to occur at about 20 GPa. This transition is reversible on release of pressure without noticeable hysteresis and hence this new high-pressure phase is unquenchable to ambient conditions. The volume change associated with the transition is found to be small (not measurable), suggesting a second order transition. The diffraction pattern of the highpressure phase can be indexed in a monoclinic unit cell (space group I2/m), which is isostructual with BaMn8O16 hollandite. The γ angle of the monoclinic unit cell increases continuously above the transition. A Birch-Murnaghan equation of state fit to pressure-volume data obtained for KAlSi3O8 hollandite yields a bulk modulus K0 = 201.4 (7) GPa with K’0 = 4.0.