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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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. |
doi_str_mv | 10.1007/s00269-011-0440-5 |
format | Article |
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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.</description><identifier>ISSN: 0342-1791</identifier><identifier>EISSN: 1432-2021</identifier><identifier>DOI: 10.1007/s00269-011-0440-5</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer-Verlag</publisher><subject>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</subject><ispartof>Physics and chemistry of minerals, 2011-10, Vol.38 (9), p.679-684</ispartof><rights>Springer-Verlag 2011</rights><rights>Physics and Chemistry of Minerals is a copyright of Springer, (2011). All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a405t-f251940ef92bcfefc3ee5f6c5f425abaccc8c736ebaa194fbb1976f0fc6b8be93</citedby><cites>FETCH-LOGICAL-a405t-f251940ef92bcfefc3ee5f6c5f425abaccc8c736ebaa194fbb1976f0fc6b8be93</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s00269-011-0440-5$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s00269-011-0440-5$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>315,781,785,27929,27930,41493,42562,51324</link.rule.ids></links><search><creatorcontrib>Seryotkin, Yurii V.</creatorcontrib><creatorcontrib>Bakakin, Vladimir V.</creatorcontrib><title>Structural evolution of hemimorphite at high pressure up to 4.2 GPa</title><title>Physics and chemistry of minerals</title><addtitle>Phys Chem Minerals</addtitle><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.</description><subject>Channels</subject><subject>Compressibility</subject><subject>Coordination</subject><subject>Crystallography and Scattering Methods</subject><subject>Crystals</subject><subject>Deformation mechanisms</subject><subject>Diamond anvil cells</subject><subject>Earth and Environmental Science</subject><subject>Earth Sciences</subject><subject>Evolution</subject><subject>Geochemistry</subject><subject>High pressure</subject><subject>Hydrogen bonding</subject><subject>Hydrogen bonds</subject><subject>Mineral Resources</subject><subject>Mineralogy</subject><subject>Original Paper</subject><subject>Phase transitions</subject><subject>Reduction</subject><subject>Rods</subject><subject>Rotation</subject><subject>Single crystals</subject><subject>Symmetry</subject><subject>Translations</subject><subject>Unit cell</subject><subject>Water chemistry</subject><subject>X-ray diffraction</subject><subject>Zinc silicates</subject><issn>0342-1791</issn><issn>1432-2021</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><sourceid>AFKRA</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp1kM1KAzEUhYMoWKsP4C7gOvUmk8zPUqpWoaCgrkMm3HSmTJsxyQi-jc_ikzllBFeu7uJ851z4CLnksOAAxXUEEHnFgHMGUgJTR2TGZSaYAMGPyQwyKRgvKn5KzmLcAoxhoWbk9iWFwaYhmI7ih--G1Po99Y42uGt3PvRNm5CaRJt209A-YIxDQDr0NHkqF-L7a_VszsmJM13Ei987J2_3d6_LB7Z-Wj0ub9bMSFCJOaF4JQFdJWrr0NkMUbncKieFMrWx1pa2yHKsjRlBV9e8KnIHzuZ1WWOVzcnVtNsH_z5gTHrrh7AfX2ohcgFFKXg5UnyibPAxBnS6D-3OhE_NQR9k6UmWHmXpgyytxo6YOnFk9xsMf8v_l34AHbZtuA</recordid><startdate>20111001</startdate><enddate>20111001</enddate><creator>Seryotkin, Yurii V.</creator><creator>Bakakin, Vladimir V.</creator><general>Springer-Verlag</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>AFKRA</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>KB.</scope><scope>PCBAR</scope><scope>PDBOC</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope></search><sort><creationdate>20111001</creationdate><title>Structural evolution of hemimorphite at high pressure up to 4.2 GPa</title><author>Seryotkin, Yurii V. ; 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 & Engineering Collection</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>Natural Science Collection</collection><collection>Earth, Atmospheric & Aquatic Science Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Materials Science Database</collection><collection>Earth, Atmospheric & Aquatic Science Database</collection><collection>Materials Science Collection</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><jtitle>Physics and chemistry of minerals</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Seryotkin, Yurii V.</au><au>Bakakin, Vladimir V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structural evolution of hemimorphite at high pressure up to 4.2 GPa</atitle><jtitle>Physics and chemistry of minerals</jtitle><stitle>Phys Chem Minerals</stitle><date>2011-10-01</date><risdate>2011</risdate><volume>38</volume><issue>9</issue><spage>679</spage><epage>684</epage><pages>679-684</pages><issn>0342-1791</issn><eissn>1432-2021</eissn><abstract>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.</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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source | Springer Online Journals Complete |
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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