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 DΔf(fm...

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Main Authors: Jannis Lübbe, Matthias Temmen, Philipp Rahe, Michael Reichling
Format: Article
Language:English
Published: Beilstein-Institut 2016-12-01
Series:Beilstein Journal of Nanotechnology
Subjects:
Online Access:https://doi.org/10.3762/bjnano.7.181
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spelling doaj-d618699f2a8a4122bf057c0d4419c0132020-11-24T21:55:58ZengBeilstein-InstitutBeilstein Journal of Nanotechnology2190-42862016-12-01711885190410.3762/bjnano.7.1812190-4286-7-181Noise in NC-AFM measurements with significant tip–sample interactionJannis Lübbe0Matthias Temmen1Philipp Rahe2Michael Reichling3Fachbereich Physik, Universität Osnabrück, Barbarastraße 7, 49076 Osnabrück, GermanyFachbereich Physik, Universität Osnabrück, Barbarastraße 7, 49076 Osnabrück, GermanyDepartment of Physics and Astronomy, The University of Utah, 115 South 1400 East, Salt Lake City, UT 84112-0830, USAFachbereich Physik, Universität Osnabrück, Barbarastraße 7, 49076 Osnabrück, GermanyThe 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 DΔf(fm) 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 DΔf(fm) 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.https://doi.org/10.3762/bjnano.7.181amplitude noisecantilever stiffnessclosed loopdetection system noisefrequency shift noisenon-contact atomic force microscopy (NC-AFM)Q-factorspectral analysisthermal noisetip–sample interaction
collection DOAJ
language English
format Article
sources DOAJ
author Jannis Lübbe
Matthias Temmen
Philipp Rahe
Michael Reichling
spellingShingle Jannis Lübbe
Matthias Temmen
Philipp Rahe
Michael Reichling
Noise in NC-AFM measurements with significant tip–sample interaction
Beilstein Journal of Nanotechnology
amplitude noise
cantilever stiffness
closed loop
detection system noise
frequency shift noise
non-contact atomic force microscopy (NC-AFM)
Q-factor
spectral analysis
thermal noise
tip–sample interaction
author_facet Jannis Lübbe
Matthias Temmen
Philipp Rahe
Michael Reichling
author_sort Jannis Lübbe
title Noise in NC-AFM measurements with significant tip–sample interaction
title_short 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_sort noise in nc-afm measurements with significant tip–sample interaction
publisher Beilstein-Institut
series Beilstein Journal of Nanotechnology
issn 2190-4286
publishDate 2016-12-01
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 DΔf(fm) 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 DΔf(fm) 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.
topic amplitude noise
cantilever stiffness
closed loop
detection system noise
frequency shift noise
non-contact atomic force microscopy (NC-AFM)
Q-factor
spectral analysis
thermal noise
tip–sample interaction
url https://doi.org/10.3762/bjnano.7.181
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AT matthiastemmen noiseinncafmmeasurementswithsignificanttipsampleinteraction
AT philipprahe noiseinncafmmeasurementswithsignificanttipsampleinteraction
AT michaelreichling noiseinncafmmeasurementswithsignificanttipsampleinteraction
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