2015
DOI: 10.1016/j.gsf.2015.02.001
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The crystal chemistry and the compressibility of silicate-carbonate minerals: Spurrite, galuskinite and tilleyite

Abstract: a b s t r a c tSpurrite Ca 5 (SiO 4 ) 2 (CO 3 ), galuskinite Ca 7 (SiO 4 ) 3 (CO 3 ) and tilleyite Ca 5 (Si 2 O 7 )(CO 3 ) 2 are three representative minerals formed in high-temperature skarns in the silicate-carbonate system. Their crystal chemistry and compressibility have been investigated using first-principles theoretical simulation. These minerals are structurally described as the combination of interwoven layers constituted by Ca polyhedra and Si polyhedra, with the [CO 3 ] triangles being "separators" … Show more

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Cited by 12 publications
(13 citation statements)
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“…A third-order Birch–Murnaghan EOS was used to fit our pressure–volume data, yielding as characteristic parameters a zero-pressure volume V 0 of 977.9(4) Å 3 , a bulk modulus B 0 of 77(1) GPa, and a first-pressure derivative B 0 ′ of 5.9(2). Notably, these experimental results compare relatively well with those obtained from theoretical calculations: V 0 = 1003.31(4) Å 3 , B 0 = 71.1(1) GPa, and B 0 ′ = 5.4(1) . The isothermal compressibility at RT was also determined up to 6.4 GPa in a second experiment using NaCl as the pressure gauge and pressure-transmitting medium.…”
Section: Resultssupporting
confidence: 81%
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“…A third-order Birch–Murnaghan EOS was used to fit our pressure–volume data, yielding as characteristic parameters a zero-pressure volume V 0 of 977.9(4) Å 3 , a bulk modulus B 0 of 77(1) GPa, and a first-pressure derivative B 0 ′ of 5.9(2). Notably, these experimental results compare relatively well with those obtained from theoretical calculations: V 0 = 1003.31(4) Å 3 , B 0 = 71.1(1) GPa, and B 0 ′ = 5.4(1) . The isothermal compressibility at RT was also determined up to 6.4 GPa in a second experiment using NaCl as the pressure gauge and pressure-transmitting medium.…”
Section: Resultssupporting
confidence: 81%
“…With regard to the values of the β angle, its variation can be considered as almost negligible. It decreases at a pace of −0.0261(9)°/GPa up to 15 GPa and then remains nearly stable at 100.86°, to be compared with the value of −0.0216(11)°/GPa obtained from theoretical calculations . A third-order Birch–Murnaghan EOS was used to fit our pressure–volume data, yielding as characteristic parameters a zero-pressure volume V 0 of 977.9(4) Å 3 , a bulk modulus B 0 of 77(1) GPa, and a first-pressure derivative B 0 ′ of 5.9(2).…”
Section: Resultsmentioning
confidence: 92%
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“…The least-squares fit of a second-order Birch−Murnaghan equation of state (BM-EoS) 33 to our experimental (theoretical) pressure-volume data of the initial phase give a zero-pressure unitcell volume, V 0 = 1131(1) Å 3 (1119.5(6) Å 3 ) and a bulk modulus, B 0 = 80(2) GPa (75.3(4) GPa). These values reflect a slightly lower compressibility than those reported by Gao and coworkers: V 0 = 1168.90(2) Å 3 , B 0 = 69.7(3) GPa, and B’ 0 = 4.0(1) from DFT calculations using the PBE prescription 34 . Post-tilleyite is only slightly more incompressible with BM-EoS characteristic parameters: V 0 = 1110(4) Å 3 (1088.7(4) Å 3 ) and B 0 = 83(3) GPa (82.1 (3) GPa), according to experimental (theoretical) results.…”
Section: Resultsmentioning
confidence: 43%