David Santamaría-Pérez, Raquel Chuliá-Jordán, Benedito Donizeti Botan-Neto, Ganesh Bera, Julio Pellicer-Porres, Lkhamsuren Bayarjargal, Alberto Otero-de-la-Roza and Catalin Popescu
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Synchrotron X-ray diffraction and Raman spectroscopy experiments were carried out in a diamond-anvil cell using He as a highly hydrostatic pressure transmitting medium. XRD results suggest that the initial <em>R</em>32 huntite structure persists up to 21 GPa. The Raman experiment agrees with this result but also suggests the appearance of structural defects from 10 GPa on. Birch–Murnaghan equation of state parameters were fit to the pressure–volume huntite data resulting in zero-pressure volume <em>V</em><small><sub>0</sub></small> of 611.7(2) Å<small><sup>3</sup></small>, a bulk modulus <em>B</em><small><sub>0</sub></small> of 99.5(11) GPa and a pressure derivative of the bulk modulus of <img>. At 21 GPa, huntite transforms to another trigonal phase (<em>R</em>3), designated here as huntite II. This phase persists up to at least 38 GPa, the maximum pressure reached in this study. The major structural differences between huntite and the huntite-II phase involve the tilting of the [CO<small><sub>3</sub></small>] units with respect to the basal plane and a rotation, which cause a progressive change in the coordination number of the Ca atoms, from 6 to 9. DFT calculations complement the experimental data, providing new insights into the structural response to high-pressure conditions of this magnesium–calcium double carbonate mineral.</p>","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":" 6","pages":" 3320-3329"},"PeriodicalIF":3.0000,"publicationDate":"2025-01-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2025/cp/d4cp04200j?page=search","citationCount":"0","resultStr":"{\"title\":\"Pressure-driven phase transformations on Mg3Ca(CO3)4 huntite carbonate†\",\"authors\":\"David Santamaría-Pérez, Raquel Chuliá-Jordán, Benedito Donizeti Botan-Neto, Ganesh Bera, Julio Pellicer-Porres, Lkhamsuren Bayarjargal, Alberto Otero-de-la-Roza and Catalin Popescu\",\"doi\":\"10.1039/D4CP04200J\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >Magnesium and calcium carbonate minerals are significant reservoirs of Earth's carbon and understanding their behavior under different conditions is crucial for elucidating the mechanisms of deep carbon storage. Huntite, Mg<small><sub>3</sub></small>Ca(CO<small><sub>3</sub></small>)<small><sub>4</sub></small>, is one of the two stable calcium magnesium carbonate phases, together with dolomite. The distinctive cation coordination environment of Ca atoms compared to calcite-type and dolomite structures makes huntite a comparatively less dense phase. Here we examine the behavior of a polycrystalline natural huntite sample under room-temperature compression up to 38 GPa. Synchrotron X-ray diffraction and Raman spectroscopy experiments were carried out in a diamond-anvil cell using He as a highly hydrostatic pressure transmitting medium. XRD results suggest that the initial <em>R</em>32 huntite structure persists up to 21 GPa. The Raman experiment agrees with this result but also suggests the appearance of structural defects from 10 GPa on. Birch–Murnaghan equation of state parameters were fit to the pressure–volume huntite data resulting in zero-pressure volume <em>V</em><small><sub>0</sub></small> of 611.7(2) Å<small><sup>3</sup></small>, a bulk modulus <em>B</em><small><sub>0</sub></small> of 99.5(11) GPa and a pressure derivative of the bulk modulus of <img>. At 21 GPa, huntite transforms to another trigonal phase (<em>R</em>3), designated here as huntite II. This phase persists up to at least 38 GPa, the maximum pressure reached in this study. The major structural differences between huntite and the huntite-II phase involve the tilting of the [CO<small><sub>3</sub></small>] units with respect to the basal plane and a rotation, which cause a progressive change in the coordination number of the Ca atoms, from 6 to 9. 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引用次数: 0
摘要
碳酸镁和碳酸钙矿物是地球碳的重要储集层,了解它们在不同条件下的行为对阐明深部碳储存机制至关重要。镁钙(Mg3Ca(CO3)4)与白云石是两种稳定的碳酸钙镁相之一。与方解石型和白云石结构相比,钙原子独特的阳离子配位环境使得钙是一个相对较不致密的相。在这里,我们研究了多晶天然猎人样品在室温压缩至38 GPa下的行为。以氦为高流体静压传递介质,在金刚石砧池中进行了同步加速器x射线衍射和拉曼光谱实验。XRD结果表明,在21 GPa的温度下,R32的初始结构仍然存在。拉曼实验与这一结果一致,但也表明从10gpa开始结构缺陷的出现。将Birch-Murnaghan状态方程参数拟合到压力-体积hunt数据中,得到零压体积V0为611.7(2)Å3,体积模量B0为99.5(11)GPa,体积模量B0′的压力导数= 3.51(11)。在21 GPa时,hunte转变为另一个三角相(R3),这里称为hunte II (huni -II)。这个阶段持续到至少38 GPa,这是本研究中达到的最大压力。hunte相和Hun-II相的主要结构差异包括[CO3]单元相对于基面的倾斜和Ca原子配位数的逐渐变化,从6到9。我们的实验研究将亨特特的压力范围扩大了三倍,为这种镁钙双碳酸盐矿物在高压条件下的结构响应提供了新的见解。
Pressure-driven phase transformations on Mg3Ca(CO3)4 huntite carbonate†
Magnesium and calcium carbonate minerals are significant reservoirs of Earth's carbon and understanding their behavior under different conditions is crucial for elucidating the mechanisms of deep carbon storage. Huntite, Mg3Ca(CO3)4, is one of the two stable calcium magnesium carbonate phases, together with dolomite. The distinctive cation coordination environment of Ca atoms compared to calcite-type and dolomite structures makes huntite a comparatively less dense phase. Here we examine the behavior of a polycrystalline natural huntite sample under room-temperature compression up to 38 GPa. Synchrotron X-ray diffraction and Raman spectroscopy experiments were carried out in a diamond-anvil cell using He as a highly hydrostatic pressure transmitting medium. XRD results suggest that the initial R32 huntite structure persists up to 21 GPa. The Raman experiment agrees with this result but also suggests the appearance of structural defects from 10 GPa on. Birch–Murnaghan equation of state parameters were fit to the pressure–volume huntite data resulting in zero-pressure volume V0 of 611.7(2) Å3, a bulk modulus B0 of 99.5(11) GPa and a pressure derivative of the bulk modulus of . At 21 GPa, huntite transforms to another trigonal phase (R3), designated here as huntite II. This phase persists up to at least 38 GPa, the maximum pressure reached in this study. The major structural differences between huntite and the huntite-II phase involve the tilting of the [CO3] units with respect to the basal plane and a rotation, which cause a progressive change in the coordination number of the Ca atoms, from 6 to 9. DFT calculations complement the experimental data, providing new insights into the structural response to high-pressure conditions of this magnesium–calcium double carbonate mineral.
期刊介绍:
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