adolescence of force feedback microscopy · system analysis of force feedback microscopy, journal...
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17/03/2014 Luca Costa 1
Adolescence of Force Feedback Microscopy
L. Costa1,2, M. S. Rodrigues3, S. Carpentier4, M. Vitorino1,3, J.
Chevrier2,4,1, F. Comin1
1) European Synchrotron Radiation Facility, 6 rue Jules Horowitz BP 220, 38043 Grenoble
Cedex, France 2) UniversitéJoseph Fourier BP 53, 38041 Grenoble Cedex 9, France 3) CFMC/Dep. Fisica, Faculdade de Ciencias, Universidade de Lisboa, Campo Grande, 1749-
016 Lisboa,Portugal 4) Institut Néel CNRS BP 166, 38042 Grenoble Cedex 9, France
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OUTLINE • Force Feedback Microscope
• Interactions at the nanoscale
• Biomolecules
• Spectroscopy on living cells
• Optical beam deflection operational schemes
• Conclusions
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Introduction
Imaging modes
Optical beam deflection
Force Feedback Microscope:
an AFM where the total force acting on the tip is zero: Σi F
i = 0
An additional force Ffeedback
has to be applied
Ffeedback
= - Finteraction
Xt is kept constant
by a feedback loop
Force Feedback Microscope
Interaction curves
Elastic and inelastic interactions
Ffeedback
Finteraction
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AFM cantilever
Introduction
Imaging modes
Optical beam deflection
Force Feedback Microscope
Interaction curves
Elastic and inelastic interactions
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Ffeedback
Finteraction
Introduction
Imaging modes
Optical beam deflection
Force Feedback Microscope
Interaction curves
Elastic and inelastic interactions
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Approach – Retract force curves between a silicon nitride
probe and mica in deionized water
M. S. Rodrigues, L. Costa, J. Chevrier, and F. Comin, Applied Physics Letters 101, 203105 (2012)
Approach – Retract force curves between a silicon probe
and hydrophilic silicon native oxide surface in air
Introduction
Imaging modes
Optical beam deflection
Force Feedback Microscope
Interaction curves
Elastic and inelastic interactions
Solid/liquid interface
Solid/air interface
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Introduction
Imaging modes
Optical beam deflection
Force Feedback Microscope
Interaction curves
Elastic and inelastic interactions
Approach – Retract force curve between a silicon nitride probe and
mica in deionized water sample
M. S. Rodrigues, L. Costa, J. Chevrier, and F. Comin, Journal of Applied Physics 115, 054309(2014)
Force gradient & Dissipation
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Introduction
Imaging modes
Optical beam deflection
Force Feedback Microscope
Interaction curves
Elastic and inelastic interactions
“Take-home” message - Σ
i F
i = 0 on the tip
- linear regime AFM with small oscillation amplitudes,
typically 1 – 2 Ångström → ɣ(d) and ∂zF(z)
- the frequency is arbitrarily chosen
- no jump to contact
M. S. Rodrigues, L. Costa, J. Chevrier, and F. Comin, Journal of Applied Physics 115, 054309(2014)
M. S. Rodrigues, L. Costa, J. Chevrier, and F. Comin, Applied Physics Letters 101, 203105 (2012)
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Introduction
Imaging modes
Optical beam deflection
Lipids
Living cells
(a) Topography
(b) Force
(c) Stiffness
(d) Dissipation
L. Costa, M. S. Rodrigues, E. Newman, C. Zubieta, J. Chevrier, and F. Comin, Journal of Molecular Recognition, 26: 689-693 (2013)
Phospholipids DSPE
Excitation frequency of the tip not linked
to resonance
Young modulus E ≈ 7 MPa
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Introduction
Imaging modes
Optical beam deflection
Lipids
Living cells
Static indentation on living cells Quasi-static conditions: Young modulus ≈ 1 kPa
L. Costa, M. S. Rodrigues, N. Benseny-Cases, V. Mayeux, J. Chevrier, and F. Comin, in revision in PlosOne (2014)
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Introduction
Imaging modes
Optical beam deflection
Lipids
Living cells
FFM indentation Quasi-static conditions: Young modulus ≈ 1 kPa
Blue = 1.13 kHz
Red = 5.13 kHz
Green = 7.13 kHz
Black = 11.13 kHz
L. Costa, M. S. Rodrigues, N. Benseny-Cases, V. Mayeux, J. Chevrier, and F. Comin, in revision in PlosOne (2014)
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Introduction
Imaging modes
Optical beam deflection
Principle
Preliminary results
Black = No interaction
Red = cantilever base
inclined with interaction
Red dotted = cantilever
base inclined without
interaction
M. V. Vitorino, S. Carpentier, L. Costa, M. S. Rodrigues, in preparation (2014)
lf = illuminated cantilever length
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Introduction
Imaging modes
Optical beam deflection
Principle
Preliminary results
Capillary condensation
M. V. Vitorino, S. Carpentier, L. Costa, M. S. Rodrigues, in preparation (2014)
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Introduction
Imaging modes
Optical beam deflection
Conclusions
- F, ɣ(d) and ∂zF(z)
simultaneously
- the frequency is
arbitrarily chosen
- no jump to contact
Interferometric operational
schemes
Optical beam deflection
operational schemes
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Surface Science Lab. Team
Fabio Comin
Joel Chevrier
Mario S. Rodrigues
..... and you for your kind attention
Introduction
Imaging modes
Living cells
Viscoelasticity vs frequency
Viscoelasticity: a local information
Conclusions
Simon Carpentier
Miguel V. Vitorino
Why do atomic force microscopy force curves still exhibit jump to contact? , Applied Physics Letters 101, 203105 (2012)
System analysis of force feedback microscopy, Journal of Applied Physics 115, 054309 (2014)
Imaging material properties of biological samples with a force feedback microscope, Journal of Molecular Recognition, 26: 689-693 (2013)
Spectroscopic investigation of local mechanical impedance of living cells, in revision in PlosOne (2014), arXiv:1310.6201
Force feedback Microscopy on a laser beam deflection scheme, Brownian motion and capillary bridges, in preparation (2014)
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Additional Slides
Images with a commercial AFM (Asylum Cypher)
Mica in water
Bacteriorhodopsin
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DMASP
Additional Slides
Digital Instruments Dimension 3100
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Additional Slides
Biomolecules images with a commercial AFM (Asylum MFP3D)
LIPIDS DNA Proteins
TBK1 OPTN
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Additional Slides
Tip power spectral density in air and liquid as a function of the tip-
fiber distance
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Additional Slides
The Force Feedback Microscope
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Additional Slides
Another FFM image on PC12 living cells