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Finite element method calculations of ZnO nanowires for nanogenerators
The bending of a nonconducting piezoelectric ZnO nanowire is simulated by finite element method calculations. The top part is bent by a lateral force, which could be applied by an atomic force microscope tip. The generated electrical potential is ± 0.3 V . This relatively high signal is, however, di...
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| Published in: | Applied physics letters 2008-03, Vol.92 (12), p.122904-122904-3 |
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| Main Authors: | , , , , |
| Format: | Article |
| Language: | English |
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| cites | cdi_FETCH-LOGICAL-c284t-486e8d9396e51d61f8ed167f68d40713549ad5e6894303e9e905185a6d62c20d3 |
| container_end_page | 122904-3 |
| container_issue | 12 |
| container_start_page | 122904 |
| container_title | Applied physics letters |
| container_volume | 92 |
| creator | Schubert, M. A. Senz, S. Alexe, M. Hesse, D. Gösele, U. |
| description | The bending of a nonconducting piezoelectric ZnO nanowire is simulated by finite element method calculations. The top part is bent by a lateral force, which could be applied by an atomic force microscope tip. The generated electrical potential is
±
0.3
V
. This relatively high signal is, however, difficult to measure due to the low capacitance of the ZnO nanowire
(
∼
4
×
10
−
5
pF
)
as compared to the capacitance of most preamplifiers
(
∼
5
pF
)
. A further problem arises from the semiconducting properties of experimentally fabricated ZnO nanowires which causes the disappearance of the voltage signal within picoseconds. |
| doi_str_mv | 10.1063/1.2903114 |
| format | article |
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±
0.3
V
. This relatively high signal is, however, difficult to measure due to the low capacitance of the ZnO nanowire
(
∼
4
×
10
−
5
pF
)
as compared to the capacitance of most preamplifiers
(
∼
5
pF
)
. A further problem arises from the semiconducting properties of experimentally fabricated ZnO nanowires which causes the disappearance of the voltage signal within picoseconds.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.2903114</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>American Institute of Physics</publisher><ispartof>Applied physics letters, 2008-03, Vol.92 (12), p.122904-122904-3</ispartof><rights>2008 American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c284t-486e8d9396e51d61f8ed167f68d40713549ad5e6894303e9e905185a6d62c20d3</citedby><cites>FETCH-LOGICAL-c284t-486e8d9396e51d61f8ed167f68d40713549ad5e6894303e9e905185a6d62c20d3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/apl/article-lookup/doi/10.1063/1.2903114$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,782,784,795,27922,27923,76153</link.rule.ids></links><search><creatorcontrib>Schubert, M. A.</creatorcontrib><creatorcontrib>Senz, S.</creatorcontrib><creatorcontrib>Alexe, M.</creatorcontrib><creatorcontrib>Hesse, D.</creatorcontrib><creatorcontrib>Gösele, U.</creatorcontrib><title>Finite element method calculations of ZnO nanowires for nanogenerators</title><title>Applied physics letters</title><description>The bending of a nonconducting piezoelectric ZnO nanowire is simulated by finite element method calculations. The top part is bent by a lateral force, which could be applied by an atomic force microscope tip. The generated electrical potential is
±
0.3
V
. This relatively high signal is, however, difficult to measure due to the low capacitance of the ZnO nanowire
(
∼
4
×
10
−
5
pF
)
as compared to the capacitance of most preamplifiers
(
∼
5
pF
)
. A further problem arises from the semiconducting properties of experimentally fabricated ZnO nanowires which causes the disappearance of the voltage signal within picoseconds.</description><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNp1kMFKxDAURYMoWEcX_kG2LjrmNU2abAQZ7CgMzEY3bkJIXrXSSSSJiH_v2Jmtq_suHB7cQ8g1sCUwyW9h2WjGAdoTUgHrunp_q1NSMcZ4LbWAc3KR88e-iobzivT9GMaCFCfcYSh0h-U9eurs5L4mW8YYMo0DfQ1bGmyI32PCTIeY5vaGAZMtMeVLcjbYKePVMRfkpX94Xj3Wm-36aXW_qV2j2lK3SqLymmuJAryEQaEH2Q1S-ZZ1wEWrrRcolW4546hRMwFKWOll4xrm-YLcHP66FHNOOJjPNO5s-jHAzJ8AA-YoYM_eHdjsxjJP-R8-WDBHC2a2wH8BKWRiLg</recordid><startdate>20080324</startdate><enddate>20080324</enddate><creator>Schubert, M. A.</creator><creator>Senz, S.</creator><creator>Alexe, M.</creator><creator>Hesse, D.</creator><creator>Gösele, U.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20080324</creationdate><title>Finite element method calculations of ZnO nanowires for nanogenerators</title><author>Schubert, M. A. ; Senz, S. ; Alexe, M. ; Hesse, D. ; Gösele, U.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c284t-486e8d9396e51d61f8ed167f68d40713549ad5e6894303e9e905185a6d62c20d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Schubert, M. A.</creatorcontrib><creatorcontrib>Senz, S.</creatorcontrib><creatorcontrib>Alexe, M.</creatorcontrib><creatorcontrib>Hesse, D.</creatorcontrib><creatorcontrib>Gösele, U.</creatorcontrib><collection>CrossRef</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schubert, M. A.</au><au>Senz, S.</au><au>Alexe, M.</au><au>Hesse, D.</au><au>Gösele, U.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Finite element method calculations of ZnO nanowires for nanogenerators</atitle><jtitle>Applied physics letters</jtitle><date>2008-03-24</date><risdate>2008</risdate><volume>92</volume><issue>12</issue><spage>122904</spage><epage>122904-3</epage><pages>122904-122904-3</pages><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>The bending of a nonconducting piezoelectric ZnO nanowire is simulated by finite element method calculations. The top part is bent by a lateral force, which could be applied by an atomic force microscope tip. The generated electrical potential is
±
0.3
V
. This relatively high signal is, however, difficult to measure due to the low capacitance of the ZnO nanowire
(
∼
4
×
10
−
5
pF
)
as compared to the capacitance of most preamplifiers
(
∼
5
pF
)
. A further problem arises from the semiconducting properties of experimentally fabricated ZnO nanowires which causes the disappearance of the voltage signal within picoseconds.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.2903114</doi></addata></record> |
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| ispartof | Applied physics letters, 2008-03, Vol.92 (12), p.122904-122904-3 |
| issn | 0003-6951 1077-3118 |
| language | eng |
| recordid | cdi_crossref_primary_10_1063_1_2903114 |
| source | American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list); AIP - American Institute of Physics |
| title | Finite element method calculations of ZnO nanowires for nanogenerators |
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