A synthetic CaCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CaCO}_{3}$$\end{document}–SrCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {SrCO}_{3}$$\end{document} solid solution with composition Ca0.82Sr0.18\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {Ca}_{0.82}\hbox {Sr}_{0.18}$$\end{document}CO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CO}_{3}$$\end{document} was investigated by single-crystal X-ray diffraction in the pressure range between 0 and 22 GPa using different pressure-transmitting media. The samples were compressed in DACs using Ne up to ∼\documentclass[12pt]{minimal}
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\begin{document}$$\sim$$\end{document}9 GPa and Ar up to ∼\documentclass[12pt]{minimal}
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\begin{document}$$\sim$$\end{document}22 GPa. At ambient conditions, Ca0.82Sr0.18\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {Ca}_{0.82}\hbox {Sr}_{0.18}$$\end{document}CO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CO}_{3}$$\end{document} crystallizes in a monoclinic structure, isostructural to CaCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CaCO}_{3}$$\end{document}-II, Sr-calcite-II (Sr-CC-II), with space group P21/c\documentclass[12pt]{minimal}
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\begin{document}$$P2_1/c$$\end{document}, 4 formula units per unit cell, Z, a=6.4237(7)\documentclass[12pt]{minimal}
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\begin{document}$$a = 6.4237(7)$$\end{document} Å, b=5.0176(1)\documentclass[12pt]{minimal}
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\begin{document}$$b = 5.0176(1)$$\end{document} Å, c=8.1129(1)\documentclass[12pt]{minimal}
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\begin{document}$$c = 8.1129(1)$$\end{document} Å, β=108.064(1)∘\documentclass[12pt]{minimal}
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\begin{document}$$\beta = 108.064(1)^\circ$$\end{document} and V=248.60(1)\documentclass[12pt]{minimal}
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\begin{document}$$V=248.60(1)$$\end{document} Å3\documentclass[12pt]{minimal}
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\begin{document}$$^3$$\end{document} (where the number in parenthesis is 1σ\documentclass[12pt]{minimal}
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\begin{document}$$\sigma$$\end{document} uncertainties on the last digit). At 1.72(5) GPa, a structural phase transition is observed to a new monoclinic structure, Sr-calcite-IIIc (Sr-CC-IIIc), with space group P21/m\documentclass[12pt]{minimal}
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\begin{document}$$P2_1/m$$\end{document} and Z=8\documentclass[12pt]{minimal}
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\begin{document}$$Z=8$$\end{document} (a=6.2683(2)\documentclass[12pt]{minimal}
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\begin{document}$$a~=~6.2683(2)$$\end{document} Å, b=9.9220(5)\documentclass[12pt]{minimal}
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\begin{document}$$b = 9.9220(5)$$\end{document} Å, c=7.6574(6)\documentclass[12pt]{minimal}
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\begin{document}$$c = 7.6574(6)$$\end{document} Å, β=103.856(6)∘\documentclass[12pt]{minimal}
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\begin{document}$$\beta = 103.856(6)^\circ$$\end{document} and V=462.39(5)\documentclass[12pt]{minimal}
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\begin{document}$$V = 462.39(5)$$\end{document} Å3\documentclass[12pt]{minimal}
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\begin{document}$$^3$$\end{document}), different from any pure CaCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CaCO}_{3}$$\end{document} polymorph. At 12 GPa, the sample transformed to a triclinic structure, Sr-calcite-IIIb (Sr-CC-IIIb), with space group P1¯\documentclass[12pt]{minimal}
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\begin{document}$$P{\bar{1}}$$\end{document} and Z=4\documentclass[12pt]{minimal}
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\begin{document}$$a=6.059(5)$$\end{document} Å, b=6.280(2)\documentclass[12pt]{minimal}
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\begin{document}$$b=6.280(2)$$\end{document} Å, c=6.331(2)\documentclass[12pt]{minimal}
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\begin{document}$$\beta =108.89(5)^\circ$$\end{document}, γ=110.52(5)∘\documentclass[12pt]{minimal}
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\begin{document}$$\gamma =110.52(5)^\circ$$\end{document} and V=207.7(2)\documentclass[12pt]{minimal}
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\begin{document}$$^3$$\end{document}), isostructural to end-member CaCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CaCO}_{3}$$\end{document}-IIIb. Finally, at 17 GPa, a transition is observed to Sr-calcite-VI (Sr-CC-VI), with space group P1¯\documentclass[12pt]{minimal}
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\begin{document}$$P{\bar{1}}$$\end{document} and Z=2\documentclass[12pt]{minimal}
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\begin{document}$$a=3.444(3)$$\end{document} Å, b=4.985(4)\documentclass[12pt]{minimal}
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\begin{document}$$\beta =84.92(7)^\circ$$\end{document}, γ=89.00(7)∘\documentclass[12pt]{minimal}
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\begin{document}$$^3$$\end{document}), isostructural to end-member CaCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CaCO}_{3}$$\end{document}-VI, which is preserved up to the maximum investigated pressure of 22 GPa. The results of this study show the effect of Sr/Ca cationic substitution on the high-pressure behavior and physical properties of a CaCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CaCO}_{3}$$\end{document}–SrCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {SrCO}_{3}$$\end{document} solid solution. The phase evolution of Ca0.82Sr0.18CO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {Ca}_{0.82}\hbox {Sr}_{0.18}\hbox {CO}_3$$\end{document} and the crystallization of a new phase, Sr-CC-IIIc, different from the high-pressure polymorphs of end-member CaCO3\documentclass[12pt]{minimal}
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\begin{document}$$\hbox {CaCO}_{3}$$\end{document}, point to the importance of extending the study of carbonates to more complex systems than pure end-member compositions.