The high-pressure behaviour and the P-induced structure evolution of a natural cancrinite from Cameroun (Na6.59Ca0.93[Si6.12Al5.88O24](CO3)1.04F0.41•2H2O, a = 12.5976(6) Å, c =5 .1168(2) Å, space group: P63) were investigated by in situ single-crystal X-ray diffraction under hydrostatic conditions up to 6.63(2) GPa with a diamond anvil cell[1]. The P-V data were fitted with an isothermal Birch-Murnaghan-type equation of state (BM EoS) truncated to the 3rd-order, giving the following elastic parameters: V0 = 702.0(7) Å3, KV0 = 51(2) GPa and KV' = 2.9(4). Linearized BM EoS was used to fit the a-P and c-P data, giving the following parameters: a0 = 12.593(5) Å, Ka0 = 64(4) GPa, Ka' = 4.5(9), and c0 = 5.112(3) Å, Kc0 = 36(1) GPa, Kc' = 1.9(3). A subtle change of the elastic behaviour appears to occur at P > 4.62 GPa, and so the elastic behaviour was also described on the basis of BM EoS valid between 0.0001 – 4.62 and 5.00 – 6.63 GPa, respectively. The high-pressure structure refinements allowed the description of the main deformation mechanisms responsible for the anisotropic compression of cancrinite. The low-temperature structure evolution of the same natural cancrinite was also investigated by means of in-situ single-crystal X-ray diffraction[2]. The V-T data exhibit a trend without any evident thermoelastic anomaly, with a thermal expansion coefficient αV = 38(7) •10^(-6) K^(-1) (between 100 and 293 K). Seven structure refinements showed that the same mechanisms observed at high pressure, mainly govern the low-T structure evolution. A study of a natural sample of balliranoite (Na4.47Ca2.86K0.10[Si5.96Al6.04O24](CO3)0.62(SO4)0.33Cl2.03, a = 12.680(1) Å, c = 5.3141(5) Å, S.G.: P63) at high pressure and low temperature is in progress. Preliminary P-V data up to 4.93 GPa were fitted with a BM EoS truncated to the 2nd order (II-BM EoS), giving the following refined parameters: V0 = 735.6(9) Å3, KV0 = 48.0(14) GPa. A fit with a II-BM EoS, applied to the P-V data of cancrinite within the range 0.0001-4.62 GPa, gave the following parameters: V0 = 702.5(5) Å3, KV0 = 48.8(6) GPa, showing similar volume compressibility. However, a different elastic anisotropy is observed (Ka0:Kc0 = 2.14:1 in cancrinite; Ka0:Kc0 = 1.40:1 in balliranoite). Structure refinements of balliranoite from high pressure and low temperature diffraction data will lead to the description of the P/T-induced structure evolution, allowing a comparative crystal-chemistry analysis of this class of materials. References 1.P. Lotti, G.D. Gatta, N. Rotiroti, F. Càmara Am. Mineral. (2012), 97, 872−882. 2.G.D. Gatta, P. Lotti, V. Kahlenberg, U. Haefeker Mineral Mag. (2012, in press).

Comparative thermo-elastic behaviour of the isotypic cancrinite and balliranoite / P. Lotti, G.D. Gatta, N. Rotiroti, F. Camara. ((Intervento presentato al 41. convegno Congresso Associazione Italiana di Cristallografia tenutosi a Verona nel 2012.

Comparative thermo-elastic behaviour of the isotypic cancrinite and balliranoite

P. Lotti
Primo
;
G.D. Gatta
Secondo
;
N. Rotiroti
Penultimo
;
F. Camara
2012

Abstract

The high-pressure behaviour and the P-induced structure evolution of a natural cancrinite from Cameroun (Na6.59Ca0.93[Si6.12Al5.88O24](CO3)1.04F0.41•2H2O, a = 12.5976(6) Å, c =5 .1168(2) Å, space group: P63) were investigated by in situ single-crystal X-ray diffraction under hydrostatic conditions up to 6.63(2) GPa with a diamond anvil cell[1]. The P-V data were fitted with an isothermal Birch-Murnaghan-type equation of state (BM EoS) truncated to the 3rd-order, giving the following elastic parameters: V0 = 702.0(7) Å3, KV0 = 51(2) GPa and KV' = 2.9(4). Linearized BM EoS was used to fit the a-P and c-P data, giving the following parameters: a0 = 12.593(5) Å, Ka0 = 64(4) GPa, Ka' = 4.5(9), and c0 = 5.112(3) Å, Kc0 = 36(1) GPa, Kc' = 1.9(3). A subtle change of the elastic behaviour appears to occur at P > 4.62 GPa, and so the elastic behaviour was also described on the basis of BM EoS valid between 0.0001 – 4.62 and 5.00 – 6.63 GPa, respectively. The high-pressure structure refinements allowed the description of the main deformation mechanisms responsible for the anisotropic compression of cancrinite. The low-temperature structure evolution of the same natural cancrinite was also investigated by means of in-situ single-crystal X-ray diffraction[2]. The V-T data exhibit a trend without any evident thermoelastic anomaly, with a thermal expansion coefficient αV = 38(7) •10^(-6) K^(-1) (between 100 and 293 K). Seven structure refinements showed that the same mechanisms observed at high pressure, mainly govern the low-T structure evolution. A study of a natural sample of balliranoite (Na4.47Ca2.86K0.10[Si5.96Al6.04O24](CO3)0.62(SO4)0.33Cl2.03, a = 12.680(1) Å, c = 5.3141(5) Å, S.G.: P63) at high pressure and low temperature is in progress. Preliminary P-V data up to 4.93 GPa were fitted with a BM EoS truncated to the 2nd order (II-BM EoS), giving the following refined parameters: V0 = 735.6(9) Å3, KV0 = 48.0(14) GPa. A fit with a II-BM EoS, applied to the P-V data of cancrinite within the range 0.0001-4.62 GPa, gave the following parameters: V0 = 702.5(5) Å3, KV0 = 48.8(6) GPa, showing similar volume compressibility. However, a different elastic anisotropy is observed (Ka0:Kc0 = 2.14:1 in cancrinite; Ka0:Kc0 = 1.40:1 in balliranoite). Structure refinements of balliranoite from high pressure and low temperature diffraction data will lead to the description of the P/T-induced structure evolution, allowing a comparative crystal-chemistry analysis of this class of materials. References 1.P. Lotti, G.D. Gatta, N. Rotiroti, F. Càmara Am. Mineral. (2012), 97, 872−882. 2.G.D. Gatta, P. Lotti, V. Kahlenberg, U. Haefeker Mineral Mag. (2012, in press).
English
13-set-2012
cancrinite ; balliranoite ; high pressure ; equation of state
Settore GEO/06 - Mineralogia
Settore GEO/09 - Georisorse Miner.Appl.Mineral.-Petrogr.per l'amb.e i Beni Cul
Presentazione
Intervento inviato
Comitato scientifico
Congresso Associazione Italiana di Cristallografia
Verona
2012
41
Associazione Italiana di Cristallografia
Convegno nazionale
P. Lotti, G.D. Gatta, N. Rotiroti, F. Camara
Comparative thermo-elastic behaviour of the isotypic cancrinite and balliranoite / P. Lotti, G.D. Gatta, N. Rotiroti, F. Camara. ((Intervento presentato al 41. convegno Congresso Associazione Italiana di Cristallografia tenutosi a Verona nel 2012.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2434/219560
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