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Structural evolution of a 2M1 phengite mica up to 11 GPa: an in situ single-crystal X-ray diffraction study

机译:最高11 GPa的2M 1 云母云母的结构演化:原位单晶X射线衍射研究

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The structural evolution at high pressure of a natural 2M 1-phengite [(K0.98Na0.02)Σ=1.00(Al1.55Mg0.24Fe0.21Ti0.02)Σ=2.01(Si3.38Al0.62)O10(OH)2; a = 5.228(2), b = 9.057(3), c = 19.971(6)Å, β = 95.76(2)°; space group: C2/c] from the metamorphic complex of Cima Pal (Sesia Zone, Western Alps, Italy) was studied by single-crystal X-ray diffraction with a diamond anvil cell under hydrostatic conditions up to ~11 GPa. A series of 12 structure refinements were performed at selected pressures within the P range investigated. The compressional behaviour of the same phengite sample was previously studied up to ~25 GPa by synchrotron X-ray powder diffraction, showing an irreversible transformation with a drastic decrease of the crystallinity at P > 15–17 GPa. The elastic behaviour between 0.0001 and 17 GPa was modelled by a third-order Birch–Murnaghan Equation of State (BM-EoS), yielding to K T0 = 57.3(10) GPa and K′ = ∂K T0/∂P = 6.97(24). The single-crystal structure refinements showed that the significant elastic anisotropy of the 2M 1-phengite (with β(a):β(b):β(c) = 1:1.17:4.60) is mainly controlled by the anisotropic compression of the K-polyhedra. The evolution of the volume of the inter-layer K-polyhedron as a function of P shows a negative slope, Fitting the P–V(K-polyhedron) data with a truncated second-order BM-EoS we obtain a bulk modulus value of K T0(K-polyhedron) = 26(1) GPa. Tetrahedra and octahedra are significantly stiffer than the K-polyhedron. Tetrahedra behave as quasi-rigid units within the P range investigated. In contrast, a monotonic decrease is observed for the octahedron volume, with K T0 = 120(10) GPa derived by a BM-EoS. The anisotropic response to pressure of the K-polyhedron affects the P-induced deformation mechanism on the tetrahedral sheet, consisting in a cooperative rotation of the tetrahedra and producing a significant ditrigonalization of the six-membered rings. The volume of the K-polyhedron and the value of the ditrigonal rotation parameter (α) show a high negative correlation (about 93%), though a slight discontinuity is observed at P >8 GPa. α increases linearly with P up to 7–8 GPa (with ∂α/∂P ≈ 0.7°/GPa), whereas at higher Ps a “saturation plateau” is visible. A comparison between the main deformation mechanisms as a function of pressure observed in 2M 1- and 3T-phengite is discussed.
机译:天然2M 1 -菲格[[K 0.98 Na 0.02 Σ= 1.00 (Al 1.55 Mg 0.24 Fe 0.21 Ti 0.02 Σ= 2.01 ( Si 3.38 Al 0.62 )O 10 (OH) 2 ; a = 5.228(2),b = 9.057(3),c = 19.971(6)Å,β= 95.76(2)°;通过单晶X射线衍射和金刚石砧室在高达约11 GPa的静压条件下研究了Cima Pal(意大利西阿尔卑斯山,Sesia区)变质复合物的空间群:C2 / c]。在所研究的P范围内的选定压力下,进行了一系列12项结构改进。先前通过同步加速器X射线粉末衍射研究了相同的锂铁矿样品的压缩行为,最高可达〜25 GPa,显示出不可逆转变,并且在P> 15-17 GPa时结晶度急剧降低。通过三阶Birch-Murnaghan状态方程(BM-EoS)对0.0001至17 GPa之间的弹性行为进行建模,得出K T0 = 57.3(10)GPa和K'=∂K T0 /∂P= 6.97(24)。单晶结构细化表明,2M 1 -方晶石(β(a):β(b):β(c)= 1:1.17:4.60)的显着弹性各向异性主要是由K-多面体的各向异性压缩控制。层间K-多面体的体积随P的变化呈负斜率,将P–V(K-多面体)数据与截断的二阶BM-EoS拟合,我们得到的体积模量值为K T0 (K-多面体)= 26(1)GPa。四面体和八面体比K多面体坚硬得多。四面体在研究的P范围内表现为准刚性单位。相反,观察到八面体的体积单调减少,其中BM-EoS推导了K T0 = 120(10)GPa。各向异性对K多面体压力的响应会影响P诱导的四面体片上的变形机制,这包括四面体的协同旋转并产生六元环的显着三角化。尽管在P> 8 GPa处观察到轻微的不连续性,但K多面体的体积和三角旋转参数(α)的值显示出很高的负相关性(约93%)。当P达到7–8 GPa时,α线性增加(withα/∂P≈0.7°/ GPa),而当Ps较高时,则出现“饱和平台”。讨论了在2M 1 -和3T-辉石中观察到的主要变形机制与压力的关系。

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