Comparison of noise floor and sensitivity for different magnetoelectric laminates
We present a comparison of the magnetoelectric (ME) response and magnetic-field sensitivities of engineered laminate sensors comprised of magnetostrictive and piezoelectric phases. The ME voltage coefficients for Metglas and single crystal fibers of Pb ( Mg 1 / 3 Nb 2 / 3 ) O 3 - PbTiO 3 (PMN-PT) or...
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Veröffentlicht in: | Journal of applied physics 2010-10, Vol.108 (8), p.084509-084509-3 |
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container_issue | 8 |
container_start_page | 084509 |
container_title | Journal of applied physics |
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creator | Gao, Junqi Das, Jaydip Xing, Zengping Li, Jiefang Viehland, D. |
description | We present a comparison of the magnetoelectric (ME) response and magnetic-field sensitivities of engineered laminate sensors comprised of magnetostrictive and piezoelectric phases. The ME voltage coefficients for Metglas and single crystal fibers of
Pb
(
Mg
1
/
3
Nb
2
/
3
)
O
3
-
PbTiO
3
(PMN-PT) or
Pb
(
Zn
1
/
3
Nb
2
/
3
)
O
3
-
PbTiO
3
(PZN-PT) are about 2.8 times larger than those with Metglas-
Pb
(
Zr
,
Ti
)
O
3
(PZT) ceramic ones. This results in a 1.7 times enhancement in the magnetic-field sensitivity for the structures with single crystals. Accordingly, the noise floors are about three to four times lower for composites with PMN-PT or PZN-PT fibers than those with PZT. |
doi_str_mv | 10.1063/1.3486483 |
format | Article |
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Pb
(
Mg
1
/
3
Nb
2
/
3
)
O
3
-
PbTiO
3
(PMN-PT) or
Pb
(
Zn
1
/
3
Nb
2
/
3
)
O
3
-
PbTiO
3
(PZN-PT) are about 2.8 times larger than those with Metglas-
Pb
(
Zr
,
Ti
)
O
3
(PZT) ceramic ones. This results in a 1.7 times enhancement in the magnetic-field sensitivity for the structures with single crystals. Accordingly, the noise floors are about three to four times lower for composites with PMN-PT or PZN-PT fibers than those with PZT.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.3486483</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>American Institute of Physics</publisher><ispartof>Journal of applied physics, 2010-10, Vol.108 (8), p.084509-084509-3</ispartof><rights>2010 American Institute of Physics</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c384t-24742221a36add4465cc1a0e1a4b2f59cf52a267820b778ec3d4a712a36183ba3</citedby><cites>FETCH-LOGICAL-c384t-24742221a36add4465cc1a0e1a4b2f59cf52a267820b778ec3d4a712a36183ba3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jap/article-lookup/doi/10.1063/1.3486483$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,1558,4502,27915,27916,76145,76151</link.rule.ids></links><search><creatorcontrib>Gao, Junqi</creatorcontrib><creatorcontrib>Das, Jaydip</creatorcontrib><creatorcontrib>Xing, Zengping</creatorcontrib><creatorcontrib>Li, Jiefang</creatorcontrib><creatorcontrib>Viehland, D.</creatorcontrib><title>Comparison of noise floor and sensitivity for different magnetoelectric laminates</title><title>Journal of applied physics</title><description>We present a comparison of the magnetoelectric (ME) response and magnetic-field sensitivities of engineered laminate sensors comprised of magnetostrictive and piezoelectric phases. The ME voltage coefficients for Metglas and single crystal fibers of
Pb
(
Mg
1
/
3
Nb
2
/
3
)
O
3
-
PbTiO
3
(PMN-PT) or
Pb
(
Zn
1
/
3
Nb
2
/
3
)
O
3
-
PbTiO
3
(PZN-PT) are about 2.8 times larger than those with Metglas-
Pb
(
Zr
,
Ti
)
O
3
(PZT) ceramic ones. This results in a 1.7 times enhancement in the magnetic-field sensitivity for the structures with single crystals. Accordingly, the noise floors are about three to four times lower for composites with PMN-PT or PZN-PT fibers than those with PZT.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNp1kE1LAzEURYMoWKsL_0G2Lkbzkswks3AhxS8oiKDr8JpJJDKTlCQI_feOtuDK1YXL4XI5hFwCuwbWiRu4FlJ3UosjsgCm-0a1LTsmC8Y4NLpX_Sk5K-WTMQAt-gV5XaVpizmUFGnyNKZQHPVjSpliHGhxsYQavkLdUT93Q_DeZRcrnfAjuprc6GzNwdIRpxCxunJOTjyOxV0cckneH-7fVk_N-uXxeXW3bqzQsjZcKsk5BxQdDoOUXWstIHOAcsN921vfcuSd0pxtlNLOikGiAj7z8_MNiiW52u_anErJzpttDhPmnQFmflwYMAcXM3u7Z4sNFWtI8X_4T4hJ3vwKEd_Aomcn</recordid><startdate>20101015</startdate><enddate>20101015</enddate><creator>Gao, Junqi</creator><creator>Das, Jaydip</creator><creator>Xing, Zengping</creator><creator>Li, Jiefang</creator><creator>Viehland, D.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20101015</creationdate><title>Comparison of noise floor and sensitivity for different magnetoelectric laminates</title><author>Gao, Junqi ; Das, Jaydip ; Xing, Zengping ; Li, Jiefang ; Viehland, D.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c384t-24742221a36add4465cc1a0e1a4b2f59cf52a267820b778ec3d4a712a36183ba3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Gao, Junqi</creatorcontrib><creatorcontrib>Das, Jaydip</creatorcontrib><creatorcontrib>Xing, Zengping</creatorcontrib><creatorcontrib>Li, Jiefang</creatorcontrib><creatorcontrib>Viehland, D.</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gao, Junqi</au><au>Das, Jaydip</au><au>Xing, Zengping</au><au>Li, Jiefang</au><au>Viehland, D.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Comparison of noise floor and sensitivity for different magnetoelectric laminates</atitle><jtitle>Journal of applied physics</jtitle><date>2010-10-15</date><risdate>2010</risdate><volume>108</volume><issue>8</issue><spage>084509</spage><epage>084509-3</epage><pages>084509-084509-3</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>We present a comparison of the magnetoelectric (ME) response and magnetic-field sensitivities of engineered laminate sensors comprised of magnetostrictive and piezoelectric phases. The ME voltage coefficients for Metglas and single crystal fibers of
Pb
(
Mg
1
/
3
Nb
2
/
3
)
O
3
-
PbTiO
3
(PMN-PT) or
Pb
(
Zn
1
/
3
Nb
2
/
3
)
O
3
-
PbTiO
3
(PZN-PT) are about 2.8 times larger than those with Metglas-
Pb
(
Zr
,
Ti
)
O
3
(PZT) ceramic ones. This results in a 1.7 times enhancement in the magnetic-field sensitivity for the structures with single crystals. Accordingly, the noise floors are about three to four times lower for composites with PMN-PT or PZN-PT fibers than those with PZT.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.3486483</doi><oa>free_for_read</oa></addata></record> |
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identifier | ISSN: 0021-8979 |
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issn | 0021-8979 1089-7550 |
language | eng |
recordid | cdi_crossref_primary_10_1063_1_3486483 |
source | AIP Journals Complete; AIP Digital Archive; Alma/SFX Local Collection |
title | Comparison of noise floor and sensitivity for different magnetoelectric laminates |
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