Structural evolution of hemimorphite at high pressure up to 4.2 GPa

The high-pressure structural evolution of hemimorphite, Zn 4 Si 2 O 7 (OH) 2 ·H 2 O, a  = 8.3881(13), b  = 10.7179(11), c  = 5.1311(9) Å, V  = 461.30(12) Å 3 , space group Imm 2, Z  = 2, was studied by single-crystal X-ray diffraction with a diamond anvil cell under hydrostatic conditions up to 4.2 ...

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Veröffentlicht in:Physics and chemistry of minerals 2011-10, Vol.38 (9), p.679-684
Hauptverfasser: Seryotkin, Yurii V., Bakakin, Vladimir V.
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description The high-pressure structural evolution of hemimorphite, Zn 4 Si 2 O 7 (OH) 2 ·H 2 O, a  = 8.3881(13), b  = 10.7179(11), c  = 5.1311(9) Å, V  = 461.30(12) Å 3 , space group Imm 2, Z  = 2, was studied by single-crystal X-ray diffraction with a diamond anvil cell under hydrostatic conditions up to 4.2 GPa. In the pressure range of 0.0001–2.44 GPa, the unit-cell parameters change almost linearly. The phase transition (probably of the second order) with symmetry reduction from Imm 2 (hemimorphite-I) to Pnn 2 (hemimorphite-II) was found near 2.5 GPa. The structure compressibility increases somewhat above the phase transition. Namely, the initial unit-cell volume decreases by 3.6% at 2.44 GPa and by 7.2% at 4.20 GPa. The hemimorphite framework can be described as built up of secondary building units (SBU) Zn 4 Si 2 O 7 (OH) 2 . These blocks are combined to form the rods arranged along the c -axis; these rods are multiplied by basic and I -translations of orthorhombic unit cell. The symmetry reduction is caused by the rotation of the rods along their axis. In hemimorphite-I, the compression affects mainly the SBU dimensions, whereas a rectangular section of the channels having mm 2 symmetry remains practically unchanged. An appreciable decrease in this section in hemimorphite-II is determined by its oblique distortion with the loss of m planes. It results from opposite rotation of adjacent SBU, which also leads into the loss of I -translation. In hemimorphite-I, the coordination of H 2 O molecules is fourfold planar; the hydrogen-bonded hydroxyls and H 2 O molecules form infinite ribbons along the c -axis. In hemimorphite-II, an additional short H 2 O–O contact appears as a result of asymmetric deformation of the channels. The appearance of this new contact provides the possibility for re-orientation of hydrogen bonds. The planar coordination of H 2 O molecules changes to tetrahedral and the ribbons are transformed to islands (OH) 2 –H 2 O.
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In the pressure range of 0.0001–2.44 GPa, the unit-cell parameters change almost linearly. The phase transition (probably of the second order) with symmetry reduction from Imm 2 (hemimorphite-I) to Pnn 2 (hemimorphite-II) was found near 2.5 GPa. The structure compressibility increases somewhat above the phase transition. Namely, the initial unit-cell volume decreases by 3.6% at 2.44 GPa and by 7.2% at 4.20 GPa. The hemimorphite framework can be described as built up of secondary building units (SBU) Zn 4 Si 2 O 7 (OH) 2 . These blocks are combined to form the rods arranged along the c -axis; these rods are multiplied by basic and I -translations of orthorhombic unit cell. The symmetry reduction is caused by the rotation of the rods along their axis. In hemimorphite-I, the compression affects mainly the SBU dimensions, whereas a rectangular section of the channels having mm 2 symmetry remains practically unchanged. An appreciable decrease in this section in hemimorphite-II is determined by its oblique distortion with the loss of m planes. It results from opposite rotation of adjacent SBU, which also leads into the loss of I -translation. In hemimorphite-I, the coordination of H 2 O molecules is fourfold planar; the hydrogen-bonded hydroxyls and H 2 O molecules form infinite ribbons along the c -axis. In hemimorphite-II, an additional short H 2 O–O contact appears as a result of asymmetric deformation of the channels. The appearance of this new contact provides the possibility for re-orientation of hydrogen bonds. 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In the pressure range of 0.0001–2.44 GPa, the unit-cell parameters change almost linearly. The phase transition (probably of the second order) with symmetry reduction from Imm 2 (hemimorphite-I) to Pnn 2 (hemimorphite-II) was found near 2.5 GPa. The structure compressibility increases somewhat above the phase transition. Namely, the initial unit-cell volume decreases by 3.6% at 2.44 GPa and by 7.2% at 4.20 GPa. The hemimorphite framework can be described as built up of secondary building units (SBU) Zn 4 Si 2 O 7 (OH) 2 . These blocks are combined to form the rods arranged along the c -axis; these rods are multiplied by basic and I -translations of orthorhombic unit cell. The symmetry reduction is caused by the rotation of the rods along their axis. In hemimorphite-I, the compression affects mainly the SBU dimensions, whereas a rectangular section of the channels having mm 2 symmetry remains practically unchanged. An appreciable decrease in this section in hemimorphite-II is determined by its oblique distortion with the loss of m planes. It results from opposite rotation of adjacent SBU, which also leads into the loss of I -translation. In hemimorphite-I, the coordination of H 2 O molecules is fourfold planar; the hydrogen-bonded hydroxyls and H 2 O molecules form infinite ribbons along the c -axis. In hemimorphite-II, an additional short H 2 O–O contact appears as a result of asymmetric deformation of the channels. The appearance of this new contact provides the possibility for re-orientation of hydrogen bonds. 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Bakakin, Vladimir V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a405t-f251940ef92bcfefc3ee5f6c5f425abaccc8c736ebaa194fbb1976f0fc6b8be93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Channels</topic><topic>Compressibility</topic><topic>Coordination</topic><topic>Crystallography and Scattering Methods</topic><topic>Crystals</topic><topic>Deformation mechanisms</topic><topic>Diamond anvil cells</topic><topic>Earth and Environmental Science</topic><topic>Earth Sciences</topic><topic>Evolution</topic><topic>Geochemistry</topic><topic>High pressure</topic><topic>Hydrogen bonding</topic><topic>Hydrogen bonds</topic><topic>Mineral Resources</topic><topic>Mineralogy</topic><topic>Original Paper</topic><topic>Phase transitions</topic><topic>Reduction</topic><topic>Rods</topic><topic>Rotation</topic><topic>Single crystals</topic><topic>Symmetry</topic><topic>Translations</topic><topic>Unit cell</topic><topic>Water chemistry</topic><topic>X-ray diffraction</topic><topic>Zinc silicates</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Seryotkin, Yurii V.</creatorcontrib><creatorcontrib>Bakakin, Vladimir V.</creatorcontrib><collection>CrossRef</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science &amp; 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In the pressure range of 0.0001–2.44 GPa, the unit-cell parameters change almost linearly. The phase transition (probably of the second order) with symmetry reduction from Imm 2 (hemimorphite-I) to Pnn 2 (hemimorphite-II) was found near 2.5 GPa. The structure compressibility increases somewhat above the phase transition. Namely, the initial unit-cell volume decreases by 3.6% at 2.44 GPa and by 7.2% at 4.20 GPa. The hemimorphite framework can be described as built up of secondary building units (SBU) Zn 4 Si 2 O 7 (OH) 2 . These blocks are combined to form the rods arranged along the c -axis; these rods are multiplied by basic and I -translations of orthorhombic unit cell. The symmetry reduction is caused by the rotation of the rods along their axis. In hemimorphite-I, the compression affects mainly the SBU dimensions, whereas a rectangular section of the channels having mm 2 symmetry remains practically unchanged. An appreciable decrease in this section in hemimorphite-II is determined by its oblique distortion with the loss of m planes. It results from opposite rotation of adjacent SBU, which also leads into the loss of I -translation. In hemimorphite-I, the coordination of H 2 O molecules is fourfold planar; the hydrogen-bonded hydroxyls and H 2 O molecules form infinite ribbons along the c -axis. In hemimorphite-II, an additional short H 2 O–O contact appears as a result of asymmetric deformation of the channels. The appearance of this new contact provides the possibility for re-orientation of hydrogen bonds. The planar coordination of H 2 O molecules changes to tetrahedral and the ribbons are transformed to islands (OH) 2 –H 2 O.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer-Verlag</pub><doi>10.1007/s00269-011-0440-5</doi><tpages>6</tpages></addata></record>
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subjects Channels
Compressibility
Coordination
Crystallography and Scattering Methods
Crystals
Deformation mechanisms
Diamond anvil cells
Earth and Environmental Science
Earth Sciences
Evolution
Geochemistry
High pressure
Hydrogen bonding
Hydrogen bonds
Mineral Resources
Mineralogy
Original Paper
Phase transitions
Reduction
Rods
Rotation
Single crystals
Symmetry
Translations
Unit cell
Water chemistry
X-ray diffraction
Zinc silicates
title Structural evolution of hemimorphite at high pressure up to 4.2 GPa
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