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<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1021/acs.nanolett.9b02351</dc:identifier><dc:language>eng</dc:language><dc:creator>Gruber, G.</dc:creator><dc:creator>Urgell, C.</dc:creator><dc:creator>Tavernarakis, A.</dc:creator><dc:creator>Stavrinadis, A.: Tepsic, S.</dc:creator><dc:creator>Magén, C.</dc:creator><dc:creator>Sangiao, S.</dc:creator><dc:creator>De Teresa, J.M.</dc:creator><dc:creator>Verlot, P.</dc:creator><dc:creator>Bachtold, A.</dc:creator><dc:title>Mass Sensing for the Advanced Fabrication of Nanomechanical Resonators</dc:title><dc:identifier>ART-2019-114526</dc:identifier><dc:description>We report on a nanomechanical engineering method to monitor matter growth in real time via e-beam electromechanical coupling. This method relies on the exceptional mass sensing capabilities of nanomechanical resonators. Focused electron beam-induced deposition (FEBID) is employed to selectively grow platinum particles at the free end of singly clamped nanotube cantilevers. The electron beam has two functions: it allows both to grow material on the nanotube and to track in real time the deposited mass by probing the noise-driven mechanical resonance of the nanotube. On the one hand, this detection method is highly effective as it can resolve mass deposition with a resolution in the zeptogram range; on the other hand, this method is simple to use and readily available to a wide range of potential users because it can be operated in existing commercial FEBID systems without making any modification. The presented method allows one to engineer hybrid nanomechanical resonators with precisely tailored functionalities. It also appears as a new tool for studying the growth dynamics of ultrathin nanostructures, opening new opportunities for investigating so far out-of-reach physics of FEBID and related methods.</dc:description><dc:date>2019</dc:date><dc:source>http://zaguan.unizar.es/record/85461</dc:source><dc:doi>10.1021/acs.nanolett.9b02351</dc:doi><dc:identifier>http://zaguan.unizar.es/record/85461</dc:identifier><dc:identifier>oai:zaguan.unizar.es:85461</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/DGA/E13-17R</dc:relation><dc:relation>info:eu-repo/grantAgreement/EC/H2020/692876/EU/Nanotube Mechanical Resonator, Spin, and Superfluidity/NaTuRe</dc:relation><dc:relation>This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No H2020 692876-NaTuRe</dc:relation><dc:relation>info:eu-repo/grantAgreement/EC/H2020/758794/EU/Quantum optomechanics at ROOm Temperature/Q-ROOT</dc:relation><dc:relation>This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No H2020 758794-Q-ROOT</dc:relation><dc:relation>info:eu-repo/grantAgreement/EC/H2020/862149/EU/Room Temperature Magnetic Resonance Force Microscopy/RTMFRM</dc:relation><dc:relation>This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No H2020 862149-RTMFRM</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/FIS2015-69831-P</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/MAT2017-82970-C2-1-R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/MAT2017-82970-C2-2-R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/RTI2018-097953-B-I00</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MINECO/SEV-2015-0522</dc:relation><dc:identifier.citation>Nano Letters 19, 10 (2019), 6987-6992</dc:identifier.citation><dc:rights>by-nc</dc:rights><dc:rights>http://creativecommons.org/licenses/by-nc/3.0/es/</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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