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Mechanical Polishing Effects Toward Surface Domain Evolution in Pb(Zn^sub 1/3^Nb^sub 2/3^)O^sub 3^-PbTiO^sub 3^ Single Crystals
This paper presents the mechanical polishing effects on the surface domains and crystal structures of relaxor-based Pb(Zn1/3Nb2/3)O3-PbTiO3 (PZN-PT) single crystals. In normal sample preparation processes, a "surface deformed layer" composed of distorted crystal structures is produced due...
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Published in: | Journal of the American Ceramic Society 2011-04, Vol.94 (4), p.1079 |
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description | This paper presents the mechanical polishing effects on the surface domains and crystal structures of relaxor-based Pb(Zn1/3Nb2/3)O3-PbTiO3 (PZN-PT) single crystals. In normal sample preparation processes, a "surface deformed layer" composed of distorted crystal structures is produced due to intense compression caused by several polishing steps using a series of lapping films down to 1 ...m in particle size. This "surface deformed layer" may contribute to dissimilar properties compared with those of the interior, and also result in pop-in events in the load-displacement curve (P - h curve) during nanoindentation. An anomaly in the X-ray diffraction (XRD) profiles is also found, demonstrating a broad minor peak besides the major peak in the intensity. In addition, Piezoresponse Force Microscopy reveals that the domain structures on the crystal surface appear to be distorted and aligned along the polishing direction. Therefore, a controlled fine polishing procedure using ... slurry of 0.3 ...m particle size is adopted to remove this "surface deformed layer." After polishing to mirror finish, the macroscopic orientations of the domain walls agree well with the permissible domain wall directions. The topography is also altered analogous with the polarization direction. More specifically, the upward domains constitute a depression of ~10 nm compared with the downward domains, suggesting a different hardness for the head and tail domain sections. Furthermore, the minor peak in the XRD and the pop-in event in the nanoindentation P - h curve are successfully eliminated after this fine polishing procedure. The removal of the surface layer may also lower the coercive field of the crystals, thus enabling ferroelectric control with a smaller voltage. (ProQuest: ... denotes formulae/symbols omitted.) |
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In normal sample preparation processes, a "surface deformed layer" composed of distorted crystal structures is produced due to intense compression caused by several polishing steps using a series of lapping films down to 1 ...m in particle size. This "surface deformed layer" may contribute to dissimilar properties compared with those of the interior, and also result in pop-in events in the load-displacement curve (P - h curve) during nanoindentation. An anomaly in the X-ray diffraction (XRD) profiles is also found, demonstrating a broad minor peak besides the major peak in the intensity. In addition, Piezoresponse Force Microscopy reveals that the domain structures on the crystal surface appear to be distorted and aligned along the polishing direction. Therefore, a controlled fine polishing procedure using ... slurry of 0.3 ...m particle size is adopted to remove this "surface deformed layer." After polishing to mirror finish, the macroscopic orientations of the domain walls agree well with the permissible domain wall directions. The topography is also altered analogous with the polarization direction. More specifically, the upward domains constitute a depression of ~10 nm compared with the downward domains, suggesting a different hardness for the head and tail domain sections. Furthermore, the minor peak in the XRD and the pop-in event in the nanoindentation P - h curve are successfully eliminated after this fine polishing procedure. The removal of the surface layer may also lower the coercive field of the crystals, thus enabling ferroelectric control with a smaller voltage. 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In normal sample preparation processes, a "surface deformed layer" composed of distorted crystal structures is produced due to intense compression caused by several polishing steps using a series of lapping films down to 1 ...m in particle size. This "surface deformed layer" may contribute to dissimilar properties compared with those of the interior, and also result in pop-in events in the load-displacement curve (P - h curve) during nanoindentation. An anomaly in the X-ray diffraction (XRD) profiles is also found, demonstrating a broad minor peak besides the major peak in the intensity. In addition, Piezoresponse Force Microscopy reveals that the domain structures on the crystal surface appear to be distorted and aligned along the polishing direction. Therefore, a controlled fine polishing procedure using ... slurry of 0.3 ...m particle size is adopted to remove this "surface deformed layer." After polishing to mirror finish, the macroscopic orientations of the domain walls agree well with the permissible domain wall directions. The topography is also altered analogous with the polarization direction. More specifically, the upward domains constitute a depression of ~10 nm compared with the downward domains, suggesting a different hardness for the head and tail domain sections. Furthermore, the minor peak in the XRD and the pop-in event in the nanoindentation P - h curve are successfully eliminated after this fine polishing procedure. The removal of the surface layer may also lower the coercive field of the crystals, thus enabling ferroelectric control with a smaller voltage. (ProQuest: ... denotes formulae/symbols omitted.)</description><subject>Ceramics</subject><subject>Crystals</subject><subject>Diffraction</subject><subject>Effects</subject><subject>Ferroelectrics</subject><subject>Materials science</subject><issn>0002-7820</issn><issn>1551-2916</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNqNjL1uwjAYRS1EJULLO3xigiEidn4IM6RiASKRqUOQExwwMja1YyqmvjoWgp3pnqN7dTvIw3GMfTLDSRd5QRAQf5qSoIf6xpyc4lkaeeh_xeojlbymAnIluDlyeYCsaVjdGijUH9V72Frd0JrBQp0pl5BdlbAtVxKc5NXoR5bGVoAnYbmuHkgcjjcPDEs_rwr-Eti6f8Fgrm-mpcJ8oY_GBRs88xMNv7NivvQvWv1aZtrdSVktXbVLkyQiOI6i8K3RHfrhTno</recordid><startdate>20110401</startdate><enddate>20110401</enddate><creator>Wong, Meng Fei</creator><creator>Zeng, Kaiyang</creator><general>Wiley Subscription Services, Inc</general><scope>7QQ</scope><scope>7SR</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20110401</creationdate><title>Mechanical Polishing Effects Toward Surface Domain Evolution in Pb(Zn^sub 1/3^Nb^sub 2/3^)O^sub 3^-PbTiO^sub 3^ Single Crystals</title><author>Wong, Meng Fei ; Zeng, Kaiyang</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_8664215443</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Ceramics</topic><topic>Crystals</topic><topic>Diffraction</topic><topic>Effects</topic><topic>Ferroelectrics</topic><topic>Materials science</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wong, Meng Fei</creatorcontrib><creatorcontrib>Zeng, Kaiyang</creatorcontrib><collection>Ceramic Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of the American Ceramic Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wong, Meng Fei</au><au>Zeng, Kaiyang</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Mechanical Polishing Effects Toward Surface Domain Evolution in Pb(Zn^sub 1/3^Nb^sub 2/3^)O^sub 3^-PbTiO^sub 3^ Single Crystals</atitle><jtitle>Journal of the American Ceramic Society</jtitle><date>2011-04-01</date><risdate>2011</risdate><volume>94</volume><issue>4</issue><spage>1079</spage><pages>1079-</pages><issn>0002-7820</issn><eissn>1551-2916</eissn><coden>JACTAW</coden><abstract>This paper presents the mechanical polishing effects on the surface domains and crystal structures of relaxor-based Pb(Zn1/3Nb2/3)O3-PbTiO3 (PZN-PT) single crystals. In normal sample preparation processes, a "surface deformed layer" composed of distorted crystal structures is produced due to intense compression caused by several polishing steps using a series of lapping films down to 1 ...m in particle size. This "surface deformed layer" may contribute to dissimilar properties compared with those of the interior, and also result in pop-in events in the load-displacement curve (P - h curve) during nanoindentation. An anomaly in the X-ray diffraction (XRD) profiles is also found, demonstrating a broad minor peak besides the major peak in the intensity. In addition, Piezoresponse Force Microscopy reveals that the domain structures on the crystal surface appear to be distorted and aligned along the polishing direction. Therefore, a controlled fine polishing procedure using ... slurry of 0.3 ...m particle size is adopted to remove this "surface deformed layer." After polishing to mirror finish, the macroscopic orientations of the domain walls agree well with the permissible domain wall directions. The topography is also altered analogous with the polarization direction. More specifically, the upward domains constitute a depression of ~10 nm compared with the downward domains, suggesting a different hardness for the head and tail domain sections. Furthermore, the minor peak in the XRD and the pop-in event in the nanoindentation P - h curve are successfully eliminated after this fine polishing procedure. The removal of the surface layer may also lower the coercive field of the crystals, thus enabling ferroelectric control with a smaller voltage. (ProQuest: ... denotes formulae/symbols omitted.)</abstract><cop>Columbus</cop><pub>Wiley Subscription Services, Inc</pub></addata></record> |
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subjects | Ceramics Crystals Diffraction Effects Ferroelectrics Materials science |
title | Mechanical Polishing Effects Toward Surface Domain Evolution in Pb(Zn^sub 1/3^Nb^sub 2/3^)O^sub 3^-PbTiO^sub 3^ Single Crystals |
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