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Noise in NC-AFM measurements with significant tip–sample interaction
The frequency shift noise in non-contact atomic force microscopy (NC-AFM) imaging and spectroscopy consists of thermal noise and detection system noise with an additional contribution from amplitude noise if there are significant tip–sample interactions. The total noise power spectral density D(Δ)(f...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Beilstein-Institut
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5238627/ https://www.ncbi.nlm.nih.gov/pubmed/28144538 http://dx.doi.org/10.3762/bjnano.7.181 |
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author | Lübbe, Jannis Temmen, Matthias Rahe, Philipp Reichling, Michael |
author_facet | Lübbe, Jannis Temmen, Matthias Rahe, Philipp Reichling, Michael |
author_sort | Lübbe, Jannis |
collection | PubMed |
description | The frequency shift noise in non-contact atomic force microscopy (NC-AFM) imaging and spectroscopy consists of thermal noise and detection system noise with an additional contribution from amplitude noise if there are significant tip–sample interactions. The total noise power spectral density D(Δ)(f)(f(m)) is, however, not just the sum of these noise contributions. Instead its magnitude and spectral characteristics are determined by the strongly non-linear tip–sample interaction, by the coupling between the amplitude and tip–sample distance control loops of the NC-AFM system as well as by the characteristics of the phase locked loop (PLL) detector used for frequency demodulation. Here, we measure D(Δ)(f)(f(m)) for various NC-AFM parameter settings representing realistic measurement conditions and compare experimental data to simulations based on a model of the NC-AFM system that includes the tip–sample interaction. The good agreement between predicted and measured noise spectra confirms that the model covers the relevant noise contributions and interactions. Results yield a general understanding of noise generation and propagation in the NC-AFM and provide a quantitative prediction of noise for given experimental parameters. We derive strategies for noise-optimised imaging and spectroscopy and outline a full optimisation procedure for the instrumentation and control loops. |
format | Online Article Text |
id | pubmed-5238627 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | Beilstein-Institut |
record_format | MEDLINE/PubMed |
spelling | pubmed-52386272017-01-31 Noise in NC-AFM measurements with significant tip–sample interaction Lübbe, Jannis Temmen, Matthias Rahe, Philipp Reichling, Michael Beilstein J Nanotechnol Full Research Paper The frequency shift noise in non-contact atomic force microscopy (NC-AFM) imaging and spectroscopy consists of thermal noise and detection system noise with an additional contribution from amplitude noise if there are significant tip–sample interactions. The total noise power spectral density D(Δ)(f)(f(m)) is, however, not just the sum of these noise contributions. Instead its magnitude and spectral characteristics are determined by the strongly non-linear tip–sample interaction, by the coupling between the amplitude and tip–sample distance control loops of the NC-AFM system as well as by the characteristics of the phase locked loop (PLL) detector used for frequency demodulation. Here, we measure D(Δ)(f)(f(m)) for various NC-AFM parameter settings representing realistic measurement conditions and compare experimental data to simulations based on a model of the NC-AFM system that includes the tip–sample interaction. The good agreement between predicted and measured noise spectra confirms that the model covers the relevant noise contributions and interactions. Results yield a general understanding of noise generation and propagation in the NC-AFM and provide a quantitative prediction of noise for given experimental parameters. We derive strategies for noise-optimised imaging and spectroscopy and outline a full optimisation procedure for the instrumentation and control loops. Beilstein-Institut 2016-12-01 /pmc/articles/PMC5238627/ /pubmed/28144538 http://dx.doi.org/10.3762/bjnano.7.181 Text en Copyright © 2016, Lübbe et al. https://creativecommons.org/licenses/by/4.0https://www.beilstein-journals.org/bjnano/termsThis is an Open Access article under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. The license is subject to the Beilstein Journal of Nanotechnology terms and conditions: (https://www.beilstein-journals.org/bjnano/terms) |
spellingShingle | Full Research Paper Lübbe, Jannis Temmen, Matthias Rahe, Philipp Reichling, Michael Noise in NC-AFM measurements with significant tip–sample interaction |
title | Noise in NC-AFM measurements with significant tip–sample interaction |
title_full | Noise in NC-AFM measurements with significant tip–sample interaction |
title_fullStr | Noise in NC-AFM measurements with significant tip–sample interaction |
title_full_unstemmed | Noise in NC-AFM measurements with significant tip–sample interaction |
title_short | Noise in NC-AFM measurements with significant tip–sample interaction |
title_sort | noise in nc-afm measurements with significant tip–sample interaction |
topic | Full Research Paper |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5238627/ https://www.ncbi.nlm.nih.gov/pubmed/28144538 http://dx.doi.org/10.3762/bjnano.7.181 |
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