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Experimental deformation of olivine single crystals at mantle pressures and temperatures
Deformation experiments were carried out in a deformation-DIA high-pressure apparatus (D-DIA) on oriented San Carlos olivine single crystals, at pressure ( P) ranging from 3.5 to 8.5 GPa, temperature ( T) from 1373 to 1673 K, and in poor water condition. Oxygen fugacity ( fO 2) was maintained within...
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Published in: | Physics of the earth and planetary interiors 2009-01, Vol.172 (1), p.74-83 |
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description | Deformation experiments were carried out in a deformation-DIA high-pressure apparatus (D-DIA) on oriented San Carlos olivine single crystals, at pressure (
P) ranging from 3.5 to 8.5
GPa, temperature (
T) from 1373 to 1673
K, and in poor water condition. Oxygen fugacity (
fO
2) was maintained within the olivine stability field and contact with enstatite powder ensured an orthopyroxene activity
a
opx
=
1. Two compression directions were tested, promoting either [1
0
0] slip alone or [0
0
1] slip alone in (0
1
0) crystallographic plane, here called, respectively, a-slip and c-slip. Constant applied stress (
σ) and specimen strain rates (
ε
˙
) were monitored
in situ using time-resolved X-ray synchrotron diffraction and radiography, respectively. Transmission electron microscopy (TEM) investigation of run products revealed that dislocation creep was responsible for sample deformation. Comparison of the obtained high-
P deformation data with the data obtained at room-
P by Bai et al. [Bai, Q., Mackwell, S.L., Kohlstedt D.L., 1991, High-temperature creep of olivine single crystals. 1. Mechanical results for buffered samples, Journal of Geophysical Research, 96, 2441–2463] – on identical materials deformed at comparable
T–
σ–
fO
2–
a
opx conditions – allowed quantifying the
P effect on a-slip and c-slip rheological laws. A slip transition with increasing pressure, from dominant a-slip to dominant c-slip, is documented. a-slip appears sensitive to pressure, which translates into the high activation volume
V
a
*
=
12
±
4
c
m
3
/mol
in the corresponding rheological law, while pressure has little effect on c-slip with
V
c
*
=
3
±
4
c
m
3
/mol
. These results may explain the discrepancy between olivine low-
P and high-
P deformation data which has been debated in the literature for more than a decade. |
doi_str_mv | 10.1016/j.pepi.2008.07.026 |
format | article |
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P) ranging from 3.5 to 8.5
GPa, temperature (
T) from 1373 to 1673
K, and in poor water condition. Oxygen fugacity (
fO
2) was maintained within the olivine stability field and contact with enstatite powder ensured an orthopyroxene activity
a
opx
=
1. Two compression directions were tested, promoting either [1
0
0] slip alone or [0
0
1] slip alone in (0
1
0) crystallographic plane, here called, respectively, a-slip and c-slip. Constant applied stress (
σ) and specimen strain rates (
ε
˙
) were monitored
in situ using time-resolved X-ray synchrotron diffraction and radiography, respectively. Transmission electron microscopy (TEM) investigation of run products revealed that dislocation creep was responsible for sample deformation. Comparison of the obtained high-
P deformation data with the data obtained at room-
P by Bai et al. [Bai, Q., Mackwell, S.L., Kohlstedt D.L., 1991, High-temperature creep of olivine single crystals. 1. Mechanical results for buffered samples, Journal of Geophysical Research, 96, 2441–2463] – on identical materials deformed at comparable
T–
σ–
fO
2–
a
opx conditions – allowed quantifying the
P effect on a-slip and c-slip rheological laws. A slip transition with increasing pressure, from dominant a-slip to dominant c-slip, is documented. a-slip appears sensitive to pressure, which translates into the high activation volume
V
a
*
=
12
±
4
c
m
3
/mol
in the corresponding rheological law, while pressure has little effect on c-slip with
V
c
*
=
3
±
4
c
m
3
/mol
. These results may explain the discrepancy between olivine low-
P and high-
P deformation data which has been debated in the literature for more than a decade.</description><identifier>ISSN: 0031-9201</identifier><identifier>EISSN: 1872-7395</identifier><identifier>EISSN: 0031-9201</identifier><identifier>DOI: 10.1016/j.pepi.2008.07.026</identifier><language>eng</language><publisher>United States: Elsevier B.V</publisher><subject>Activation volume ; COMPRESSION ; CREEP ; DEFORMATION ; DIFFRACTION ; Dislocation creep ; DISLOCATIONS ; ENSTATITE ; High pressure ; MONOCRYSTALS ; national synchrotron light source ; OLIVINE ; OXYGEN ; PARTICLE ACCELERATORS ; Rheological law ; San Carlos olivine ; SLIP ; Slip systems ; STABILITY ; STRAIN RATE ; SYNCHROTRONS ; TRANSMISSION ELECTRON MICROSCOPY ; Upper mantle ; WATER</subject><ispartof>Physics of the earth and planetary interiors, 2009-01, Vol.172 (1), p.74-83</ispartof><rights>2008 Elsevier B.V.</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a493t-72083846c34502ab401ac8494bc9fc042b3d39d80b82c9873f3a35a0a156a1133</citedby><cites>FETCH-LOGICAL-a493t-72083846c34502ab401ac8494bc9fc042b3d39d80b82c9873f3a35a0a156a1133</cites><orcidid>0000-0002-7163-6263 ; 0000-0002-1883-2994 ; 0000-0001-6256-1944</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27915,27916</link.rule.ids><backlink>$$Uhttps://hal.science/hal-00532169$$DView record in HAL$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/biblio/980204$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Raterron, Paul</creatorcontrib><creatorcontrib>Amiguet, Elodie</creatorcontrib><creatorcontrib>Chen, Jiuhua</creatorcontrib><creatorcontrib>Li, Li</creatorcontrib><creatorcontrib>Cordier, Patrick</creatorcontrib><creatorcontrib>Brookhaven National Laboratory (BNL) National Synchrotron Light Source</creatorcontrib><title>Experimental deformation of olivine single crystals at mantle pressures and temperatures</title><title>Physics of the earth and planetary interiors</title><description>Deformation experiments were carried out in a deformation-DIA high-pressure apparatus (D-DIA) on oriented San Carlos olivine single crystals, at pressure (
P) ranging from 3.5 to 8.5
GPa, temperature (
T) from 1373 to 1673
K, and in poor water condition. Oxygen fugacity (
fO
2) was maintained within the olivine stability field and contact with enstatite powder ensured an orthopyroxene activity
a
opx
=
1. Two compression directions were tested, promoting either [1
0
0] slip alone or [0
0
1] slip alone in (0
1
0) crystallographic plane, here called, respectively, a-slip and c-slip. Constant applied stress (
σ) and specimen strain rates (
ε
˙
) were monitored
in situ using time-resolved X-ray synchrotron diffraction and radiography, respectively. Transmission electron microscopy (TEM) investigation of run products revealed that dislocation creep was responsible for sample deformation. Comparison of the obtained high-
P deformation data with the data obtained at room-
P by Bai et al. [Bai, Q., Mackwell, S.L., Kohlstedt D.L., 1991, High-temperature creep of olivine single crystals. 1. Mechanical results for buffered samples, Journal of Geophysical Research, 96, 2441–2463] – on identical materials deformed at comparable
T–
σ–
fO
2–
a
opx conditions – allowed quantifying the
P effect on a-slip and c-slip rheological laws. A slip transition with increasing pressure, from dominant a-slip to dominant c-slip, is documented. a-slip appears sensitive to pressure, which translates into the high activation volume
V
a
*
=
12
±
4
c
m
3
/mol
in the corresponding rheological law, while pressure has little effect on c-slip with
V
c
*
=
3
±
4
c
m
3
/mol
. These results may explain the discrepancy between olivine low-
P and high-
P deformation data which has been debated in the literature for more than a decade.</description><subject>Activation volume</subject><subject>COMPRESSION</subject><subject>CREEP</subject><subject>DEFORMATION</subject><subject>DIFFRACTION</subject><subject>Dislocation creep</subject><subject>DISLOCATIONS</subject><subject>ENSTATITE</subject><subject>High pressure</subject><subject>MONOCRYSTALS</subject><subject>national synchrotron light source</subject><subject>OLIVINE</subject><subject>OXYGEN</subject><subject>PARTICLE ACCELERATORS</subject><subject>Rheological law</subject><subject>San Carlos olivine</subject><subject>SLIP</subject><subject>Slip systems</subject><subject>STABILITY</subject><subject>STRAIN RATE</subject><subject>SYNCHROTRONS</subject><subject>TRANSMISSION ELECTRON MICROSCOPY</subject><subject>Upper mantle</subject><subject>WATER</subject><issn>0031-9201</issn><issn>1872-7395</issn><issn>0031-9201</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><recordid>eNp9kE9LAzEQxYMoWKtfwFM8eth1kuyfBLyUUq1Q8KLgLaTZrE1pkyWJxX57s1Q8epmBx-8N8x5CtwRKAqR52JaDGWxJAXgJbQm0OUMTwltatEzU52gCwEghKJBLdBXjFgAIo2yCPhbfgwl2b1xSO9yZ3oe9StY77Hvsd_ZgncHRus-dwTocY6YiVgnvlUtZGoKJ8SsPrFyHk9nnYyqNwjW66DNrbn73FL0_Ld7my2L1-vwyn60KVQmWipYCZ7xqNKtqoGpdAVGaV6Jaa9FrqOiadUx0HNacasFb1jPFagWK1I0ihLEpujvd9TFZGbVNRm-0d87oJAUHClVm7k_MRu3kkNOqcJReWbmcreSoAdSMkkYcSGbpidXBxxhM_2cgIMeu5VaOXcuxawmtzF1n0-PJZHLSgzVhfMQ4bTobxj86b_-z_wAFboeq</recordid><startdate>20090101</startdate><enddate>20090101</enddate><creator>Raterron, Paul</creator><creator>Amiguet, Elodie</creator><creator>Chen, Jiuhua</creator><creator>Li, Li</creator><creator>Cordier, Patrick</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><scope>VOOES</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0002-7163-6263</orcidid><orcidid>https://orcid.org/0000-0002-1883-2994</orcidid><orcidid>https://orcid.org/0000-0001-6256-1944</orcidid></search><sort><creationdate>20090101</creationdate><title>Experimental deformation of olivine single crystals at mantle pressures and temperatures</title><author>Raterron, Paul ; Amiguet, Elodie ; Chen, Jiuhua ; Li, Li ; Cordier, Patrick</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a493t-72083846c34502ab401ac8494bc9fc042b3d39d80b82c9873f3a35a0a156a1133</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2009</creationdate><topic>Activation volume</topic><topic>COMPRESSION</topic><topic>CREEP</topic><topic>DEFORMATION</topic><topic>DIFFRACTION</topic><topic>Dislocation creep</topic><topic>DISLOCATIONS</topic><topic>ENSTATITE</topic><topic>High pressure</topic><topic>MONOCRYSTALS</topic><topic>national synchrotron light source</topic><topic>OLIVINE</topic><topic>OXYGEN</topic><topic>PARTICLE ACCELERATORS</topic><topic>Rheological law</topic><topic>San Carlos olivine</topic><topic>SLIP</topic><topic>Slip systems</topic><topic>STABILITY</topic><topic>STRAIN RATE</topic><topic>SYNCHROTRONS</topic><topic>TRANSMISSION ELECTRON MICROSCOPY</topic><topic>Upper mantle</topic><topic>WATER</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Raterron, Paul</creatorcontrib><creatorcontrib>Amiguet, Elodie</creatorcontrib><creatorcontrib>Chen, Jiuhua</creatorcontrib><creatorcontrib>Li, Li</creatorcontrib><creatorcontrib>Cordier, Patrick</creatorcontrib><creatorcontrib>Brookhaven National Laboratory (BNL) National Synchrotron Light Source</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><collection>OSTI.GOV</collection><jtitle>Physics of the earth and planetary interiors</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Raterron, Paul</au><au>Amiguet, Elodie</au><au>Chen, Jiuhua</au><au>Li, Li</au><au>Cordier, Patrick</au><aucorp>Brookhaven National Laboratory (BNL) National Synchrotron Light Source</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Experimental deformation of olivine single crystals at mantle pressures and temperatures</atitle><jtitle>Physics of the earth and planetary interiors</jtitle><date>2009-01-01</date><risdate>2009</risdate><volume>172</volume><issue>1</issue><spage>74</spage><epage>83</epage><pages>74-83</pages><issn>0031-9201</issn><eissn>1872-7395</eissn><eissn>0031-9201</eissn><abstract>Deformation experiments were carried out in a deformation-DIA high-pressure apparatus (D-DIA) on oriented San Carlos olivine single crystals, at pressure (
P) ranging from 3.5 to 8.5
GPa, temperature (
T) from 1373 to 1673
K, and in poor water condition. Oxygen fugacity (
fO
2) was maintained within the olivine stability field and contact with enstatite powder ensured an orthopyroxene activity
a
opx
=
1. Two compression directions were tested, promoting either [1
0
0] slip alone or [0
0
1] slip alone in (0
1
0) crystallographic plane, here called, respectively, a-slip and c-slip. Constant applied stress (
σ) and specimen strain rates (
ε
˙
) were monitored
in situ using time-resolved X-ray synchrotron diffraction and radiography, respectively. Transmission electron microscopy (TEM) investigation of run products revealed that dislocation creep was responsible for sample deformation. Comparison of the obtained high-
P deformation data with the data obtained at room-
P by Bai et al. [Bai, Q., Mackwell, S.L., Kohlstedt D.L., 1991, High-temperature creep of olivine single crystals. 1. Mechanical results for buffered samples, Journal of Geophysical Research, 96, 2441–2463] – on identical materials deformed at comparable
T–
σ–
fO
2–
a
opx conditions – allowed quantifying the
P effect on a-slip and c-slip rheological laws. A slip transition with increasing pressure, from dominant a-slip to dominant c-slip, is documented. a-slip appears sensitive to pressure, which translates into the high activation volume
V
a
*
=
12
±
4
c
m
3
/mol
in the corresponding rheological law, while pressure has little effect on c-slip with
V
c
*
=
3
±
4
c
m
3
/mol
. These results may explain the discrepancy between olivine low-
P and high-
P deformation data which has been debated in the literature for more than a decade.</abstract><cop>United States</cop><pub>Elsevier B.V</pub><doi>10.1016/j.pepi.2008.07.026</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0002-7163-6263</orcidid><orcidid>https://orcid.org/0000-0002-1883-2994</orcidid><orcidid>https://orcid.org/0000-0001-6256-1944</orcidid><oa>free_for_read</oa></addata></record> |
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ispartof | Physics of the earth and planetary interiors, 2009-01, Vol.172 (1), p.74-83 |
issn | 0031-9201 1872-7395 0031-9201 |
language | eng |
recordid | cdi_osti_scitechconnect_980204 |
source | ScienceDirect Journals |
subjects | Activation volume COMPRESSION CREEP DEFORMATION DIFFRACTION Dislocation creep DISLOCATIONS ENSTATITE High pressure MONOCRYSTALS national synchrotron light source OLIVINE OXYGEN PARTICLE ACCELERATORS Rheological law San Carlos olivine SLIP Slip systems STABILITY STRAIN RATE SYNCHROTRONS TRANSMISSION ELECTRON MICROSCOPY Upper mantle WATER |
title | Experimental deformation of olivine single crystals at mantle pressures and temperatures |
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