Small shear modulus of cubic CaSiO3 perovskite
Ca‐perovskite (CaPv) is considered to be one of the most abundant minerals in the Earth's lower mantle (LM). Furthermore, previous static calculations and mean‐field theory suggest that it has a much larger shear modulus than bridgmanite (MgPv). In this study, the elasticity of cubic CaPv was r...
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Veröffentlicht in: | Geophysical research letters 2015-04, Vol.42 (8), p.2718-2726 |
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description | Ca‐perovskite (CaPv) is considered to be one of the most abundant minerals in the Earth's lower mantle (LM). Furthermore, previous static calculations and mean‐field theory suggest that it has a much larger shear modulus than bridgmanite (MgPv). In this study, the elasticity of cubic CaPv was reinvestigated using the density functional constant‐temperature first principles molecular dynamics method under the correct conditions to simulate its elasticity. Our new results clearly demonstrate that cubic CaPv has comparable bulk and slightly smaller shear moduli than Fe‐bearing MgPv. This is because the boundary condition for the supercell used in this study allows for the rotational phonon motion of SiO6 octahedra under strain, which predominantly affects the decrease in C11 and C44. Acoustic wave velocities determined from the elastic moduli indicate that cubic CaPv has slower velocities and larger densities than Fe‐bearing MgPv and preliminary reference Earth model in the LM. This suggests that if CaPv‐rich material exists, it can accumulate in the lowermost LM and produce a seismically low‐velocity anomaly.
Key Points
Smaller G of CaPv due to rotational relaxation of SiO6 octahedra for strain
Cubic CaPv has slower elastic velocities in the lower mantle
SiO6 framework controls elastic properties in the lower mantle |
doi_str_mv | 10.1002/2015GL063446 |
format | Article |
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Key Points
Smaller G of CaPv due to rotational relaxation of SiO6 octahedra for strain
Cubic CaPv has slower elastic velocities in the lower mantle
SiO6 framework controls elastic properties in the lower mantle</description><identifier>ISSN: 0094-8276</identifier><identifier>EISSN: 1944-8007</identifier><identifier>DOI: 10.1002/2015GL063446</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Anisotropy ; Bearing ; Boundary conditions ; Ca-perovskite ; Computer simulation ; Density ; Dynamics ; Earth ; Earth mantle ; Elasticity ; first principles ; Functional anatomy ; Iron ; Lower mantle ; Mantle ; Mathematical models ; Mean field theory ; Methods ; Minerals ; Modulus of elasticity ; Molecular dynamics ; Movement ; Shear ; Shear modulus ; Temperature ; Temperature effects ; Velocity ; Wave velocity</subject><ispartof>Geophysical research letters, 2015-04, Vol.42 (8), p.2718-2726</ispartof><rights>2015. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4392-15e86ef4704a5e9a9f8c2564f7ea58af5e1fe5e536618779deb3cf165ae305103</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2F2015GL063446$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2F2015GL063446$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,778,782,1414,1430,11501,27911,27912,45561,45562,46396,46455,46820,46879</link.rule.ids></links><search><creatorcontrib>Kawai, Kenji</creatorcontrib><creatorcontrib>Tsuchiya, Taku</creatorcontrib><title>Small shear modulus of cubic CaSiO3 perovskite</title><title>Geophysical research letters</title><addtitle>Geophys. Res. Lett</addtitle><description>Ca‐perovskite (CaPv) is considered to be one of the most abundant minerals in the Earth's lower mantle (LM). Furthermore, previous static calculations and mean‐field theory suggest that it has a much larger shear modulus than bridgmanite (MgPv). In this study, the elasticity of cubic CaPv was reinvestigated using the density functional constant‐temperature first principles molecular dynamics method under the correct conditions to simulate its elasticity. Our new results clearly demonstrate that cubic CaPv has comparable bulk and slightly smaller shear moduli than Fe‐bearing MgPv. This is because the boundary condition for the supercell used in this study allows for the rotational phonon motion of SiO6 octahedra under strain, which predominantly affects the decrease in C11 and C44. Acoustic wave velocities determined from the elastic moduli indicate that cubic CaPv has slower velocities and larger densities than Fe‐bearing MgPv and preliminary reference Earth model in the LM. This suggests that if CaPv‐rich material exists, it can accumulate in the lowermost LM and produce a seismically low‐velocity anomaly.
Key Points
Smaller G of CaPv due to rotational relaxation of SiO6 octahedra for strain
Cubic CaPv has slower elastic velocities in the lower mantle
SiO6 framework controls elastic properties in the lower mantle</description><subject>Anisotropy</subject><subject>Bearing</subject><subject>Boundary conditions</subject><subject>Ca-perovskite</subject><subject>Computer simulation</subject><subject>Density</subject><subject>Dynamics</subject><subject>Earth</subject><subject>Earth mantle</subject><subject>Elasticity</subject><subject>first principles</subject><subject>Functional anatomy</subject><subject>Iron</subject><subject>Lower mantle</subject><subject>Mantle</subject><subject>Mathematical models</subject><subject>Mean field theory</subject><subject>Methods</subject><subject>Minerals</subject><subject>Modulus of elasticity</subject><subject>Molecular dynamics</subject><subject>Movement</subject><subject>Shear</subject><subject>Shear modulus</subject><subject>Temperature</subject><subject>Temperature effects</subject><subject>Velocity</subject><subject>Wave velocity</subject><issn>0094-8276</issn><issn>1944-8007</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp9kEtLw0AUhQdRsFZ3_oCA69R7552lFJsqwYL1sRym6R1Mm5qaadT-eysVceXq3MX33QOHsXOEAQLwSw6o8gK0kFIfsB5mUqYWwByyHkC2u7nRx-wkxgUACBDYY4Ppytd1El_It8mqmXd1F5MmJGU3q8pk6KfVRCRrapv3uKw2dMqOgq8jnf1knz2Orh-G47SY5DfDqyItpch4ioqspiANSK8o81mwJVdaBkNeWR8UYSBFSmiN1phsTjNRBtTKkwCFIPrsYv933TZvHcWNWzRd-7qrdJghWI1S_E9pi8DRoNhRfE99VDVt3bqtVr7dOgT3PZr7O5rL7wvFLfKdlO6lKm7o81fy7dJpI4xyz3e5KwQf3Y5HT06JL1ZIbDE</recordid><startdate>20150428</startdate><enddate>20150428</enddate><creator>Kawai, Kenji</creator><creator>Tsuchiya, Taku</creator><general>Blackwell Publishing Ltd</general><general>John Wiley & Sons, Inc</general><scope>BSCLL</scope><scope>7TG</scope><scope>7TN</scope><scope>8FD</scope><scope>F1W</scope><scope>FR3</scope><scope>H8D</scope><scope>H96</scope><scope>KL.</scope><scope>KR7</scope><scope>L.G</scope><scope>L7M</scope></search><sort><creationdate>20150428</creationdate><title>Small shear modulus of cubic CaSiO3 perovskite</title><author>Kawai, Kenji ; Tsuchiya, Taku</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4392-15e86ef4704a5e9a9f8c2564f7ea58af5e1fe5e536618779deb3cf165ae305103</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Anisotropy</topic><topic>Bearing</topic><topic>Boundary conditions</topic><topic>Ca-perovskite</topic><topic>Computer simulation</topic><topic>Density</topic><topic>Dynamics</topic><topic>Earth</topic><topic>Earth mantle</topic><topic>Elasticity</topic><topic>first principles</topic><topic>Functional anatomy</topic><topic>Iron</topic><topic>Lower mantle</topic><topic>Mantle</topic><topic>Mathematical models</topic><topic>Mean field theory</topic><topic>Methods</topic><topic>Minerals</topic><topic>Modulus of elasticity</topic><topic>Molecular dynamics</topic><topic>Movement</topic><topic>Shear</topic><topic>Shear modulus</topic><topic>Temperature</topic><topic>Temperature effects</topic><topic>Velocity</topic><topic>Wave velocity</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kawai, Kenji</creatorcontrib><creatorcontrib>Tsuchiya, Taku</creatorcontrib><collection>Istex</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Oceanic Abstracts</collection><collection>Technology Research Database</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Civil Engineering Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Geophysical research letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kawai, Kenji</au><au>Tsuchiya, Taku</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Small shear modulus of cubic CaSiO3 perovskite</atitle><jtitle>Geophysical research letters</jtitle><addtitle>Geophys. Res. Lett</addtitle><date>2015-04-28</date><risdate>2015</risdate><volume>42</volume><issue>8</issue><spage>2718</spage><epage>2726</epage><pages>2718-2726</pages><issn>0094-8276</issn><eissn>1944-8007</eissn><abstract>Ca‐perovskite (CaPv) is considered to be one of the most abundant minerals in the Earth's lower mantle (LM). Furthermore, previous static calculations and mean‐field theory suggest that it has a much larger shear modulus than bridgmanite (MgPv). In this study, the elasticity of cubic CaPv was reinvestigated using the density functional constant‐temperature first principles molecular dynamics method under the correct conditions to simulate its elasticity. Our new results clearly demonstrate that cubic CaPv has comparable bulk and slightly smaller shear moduli than Fe‐bearing MgPv. This is because the boundary condition for the supercell used in this study allows for the rotational phonon motion of SiO6 octahedra under strain, which predominantly affects the decrease in C11 and C44. Acoustic wave velocities determined from the elastic moduli indicate that cubic CaPv has slower velocities and larger densities than Fe‐bearing MgPv and preliminary reference Earth model in the LM. This suggests that if CaPv‐rich material exists, it can accumulate in the lowermost LM and produce a seismically low‐velocity anomaly.
Key Points
Smaller G of CaPv due to rotational relaxation of SiO6 octahedra for strain
Cubic CaPv has slower elastic velocities in the lower mantle
SiO6 framework controls elastic properties in the lower mantle</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1002/2015GL063446</doi><tpages>9</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Anisotropy Bearing Boundary conditions Ca-perovskite Computer simulation Density Dynamics Earth Earth mantle Elasticity first principles Functional anatomy Iron Lower mantle Mantle Mathematical models Mean field theory Methods Minerals Modulus of elasticity Molecular dynamics Movement Shear Shear modulus Temperature Temperature effects Velocity Wave velocity |
title | Small shear modulus of cubic CaSiO3 perovskite |
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