Cantilever contribution to the total electrostatic force measured with the atomic force microscope
The atomic force microscope (AFM) is a powerful tool for surface imaging at the nanometer scale and surface force measurements in the piconewton range. Among long-range surface forces, the electrostatic forces play a predominant role. They originate if the electric potentials of the substrate and of...
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Veröffentlicht in: | Measurement science & technology 2010-02, Vol.21 (2), p.025502-025502 |
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creator | Guriyanova, Svetlana Golovko, Dmytro S Bonaccurso, Elmar |
description | The atomic force microscope (AFM) is a powerful tool for surface imaging at the nanometer scale and surface force measurements in the piconewton range. Among long-range surface forces, the electrostatic forces play a predominant role. They originate if the electric potentials of the substrate and of the tip of the AFM cantilever are different. A quantitative interpretation of the AFM signal is often difficult because it depends in a complicated fashion on the cantilever--tip--surface geometry. Since the electrostatic interaction is a long-range interaction, the cantilever, which is many microns from the surface, contributes to the total electrostatic force along with the tip. Here we present results of the electrostatic interaction between a conducting flat surface and horizontal or tilted cantilevers, with and without tips, at various distances from the surface. As addressed in a previous work, we show that the contribution of the cantilever to the overall force cannot be neglected. Based on a predictive model and on 3D confocal measurements, we discuss the influence of the tilting angle of the cantilever. |
doi_str_mv | 10.1088/0957-0233/21/2/025502 |
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Among long-range surface forces, the electrostatic forces play a predominant role. They originate if the electric potentials of the substrate and of the tip of the AFM cantilever are different. A quantitative interpretation of the AFM signal is often difficult because it depends in a complicated fashion on the cantilever--tip--surface geometry. Since the electrostatic interaction is a long-range interaction, the cantilever, which is many microns from the surface, contributes to the total electrostatic force along with the tip. Here we present results of the electrostatic interaction between a conducting flat surface and horizontal or tilted cantilevers, with and without tips, at various distances from the surface. As addressed in a previous work, we show that the contribution of the cantilever to the overall force cannot be neglected. 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Among long-range surface forces, the electrostatic forces play a predominant role. They originate if the electric potentials of the substrate and of the tip of the AFM cantilever are different. A quantitative interpretation of the AFM signal is often difficult because it depends in a complicated fashion on the cantilever--tip--surface geometry. Since the electrostatic interaction is a long-range interaction, the cantilever, which is many microns from the surface, contributes to the total electrostatic force along with the tip. Here we present results of the electrostatic interaction between a conducting flat surface and horizontal or tilted cantilevers, with and without tips, at various distances from the surface. As addressed in a previous work, we show that the contribution of the cantilever to the overall force cannot be neglected. Based on a predictive model and on 3D confocal measurements, we discuss the influence of the tilting angle of the cantilever.</description><subject>Atomic force microscopes</subject><subject>Atomic force microscopy</subject><subject>Confocal</subject><subject>Electric potential</subject><subject>Electrostatics</subject><subject>Force measurement</subject><subject>Three dimensional</subject><issn>0957-0233</issn><issn>1361-6501</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNqNkE1LxDAQhoMouK7-BKE3L9ZOkibbHGXxCwQveg5pkrKRtqlJqvjvba3oQQ-eXoZ5nmF4ETrFcIGhqgoQbJMDobQguCAFEMaA7KEVphznnAHeR6tv5hAdxfgMABsQYoXqreqTa-2rDZn2fQquHpPzfZZ8lnZ2iqTazLZWp-BjUsnprPFB26yzKo7BmuzNpd0nq5LvftZOT4L2gz1GB41qoz35yjV6ur563N7m9w83d9vL-1xTTlPORWN4LUxpiIFaqarGpaKVLakpOTTTRATnFQhOa6WnvSgN46oxpKkoqw1do7Pl7hD8y2hjkp2L2rat6q0fo6wY45MkyolkCzm_GINt5BBcp8K7xCDnSuVcl5zrkgRLIpdKJw8Wz_nh38r5b-VPVA6moR-eU4do</recordid><startdate>20100201</startdate><enddate>20100201</enddate><creator>Guriyanova, Svetlana</creator><creator>Golovko, Dmytro S</creator><creator>Bonaccurso, Elmar</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope></search><sort><creationdate>20100201</creationdate><title>Cantilever contribution to the total electrostatic force measured with the atomic force microscope</title><author>Guriyanova, Svetlana ; Golovko, Dmytro S ; Bonaccurso, Elmar</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c363t-69fd6b9d4d2d0baa8b14a38e43d460fb14296680963bacaa894d56afd2f835bd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>Atomic force microscopes</topic><topic>Atomic force microscopy</topic><topic>Confocal</topic><topic>Electric potential</topic><topic>Electrostatics</topic><topic>Force measurement</topic><topic>Three dimensional</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Guriyanova, Svetlana</creatorcontrib><creatorcontrib>Golovko, Dmytro S</creatorcontrib><creatorcontrib>Bonaccurso, Elmar</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><jtitle>Measurement science & technology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Guriyanova, Svetlana</au><au>Golovko, Dmytro S</au><au>Bonaccurso, Elmar</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Cantilever contribution to the total electrostatic force measured with the atomic force microscope</atitle><jtitle>Measurement science & technology</jtitle><date>2010-02-01</date><risdate>2010</risdate><volume>21</volume><issue>2</issue><spage>025502</spage><epage>025502</epage><pages>025502-025502</pages><issn>0957-0233</issn><eissn>1361-6501</eissn><abstract>The atomic force microscope (AFM) is a powerful tool for surface imaging at the nanometer scale and surface force measurements in the piconewton range. Among long-range surface forces, the electrostatic forces play a predominant role. They originate if the electric potentials of the substrate and of the tip of the AFM cantilever are different. A quantitative interpretation of the AFM signal is often difficult because it depends in a complicated fashion on the cantilever--tip--surface geometry. Since the electrostatic interaction is a long-range interaction, the cantilever, which is many microns from the surface, contributes to the total electrostatic force along with the tip. Here we present results of the electrostatic interaction between a conducting flat surface and horizontal or tilted cantilevers, with and without tips, at various distances from the surface. As addressed in a previous work, we show that the contribution of the cantilever to the overall force cannot be neglected. Based on a predictive model and on 3D confocal measurements, we discuss the influence of the tilting angle of the cantilever.</abstract><pub>IOP Publishing</pub><doi>10.1088/0957-0233/21/2/025502</doi><tpages>1</tpages></addata></record> |
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source | IOP Publishing Journals; Institute of Physics (IOP) Journals - HEAL-Link |
subjects | Atomic force microscopes Atomic force microscopy Confocal Electric potential Electrostatics Force measurement Three dimensional |
title | Cantilever contribution to the total electrostatic force measured with the atomic force microscope |
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