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Higher harmonic atomic force microscopy: Imaging of biological membranes in liquid Institute for Biophysics Johannes Kepler University of Linz Altenbergerstr. 69 A-4040 Linz, Austria Peter Hinterdorfer Johannes Preiner Agilent eSeminar, May 28 th , 2008 AFM – Group Institute of Biophysics J. Kepler University Linz

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  • Higher harmonic atomic force microscopy: Imaging of biological membranes in liquid

    Institute for Biophysics Johannes Kepler University of Linz Altenbergerstr. 69 A-4040 Linz, Austria

    Peter HinterdorferJohannes Preiner

    Agilent eSeminar, May 28th, 2008

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

  • Model: 1-DIM Harmonic Oscillator

    Equation of Motion (EQM):

    Hydrodynamic Damping:

    Contact Mechanics: Derjaguin-Muller-Toporov (DMT)-modelfor a sphere-flat geometry:

    Hamaker constant for silicon nitride/Water/Mica: H=3.1*10-21 J;f0=8.46 kHz; Q=2.078; m=35 ng; (obtained from thermal spectra),k=0.1 N/m; fd=7.184 kHz

    C. Rankl et al. Ultramicroscopy 2004

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    J.Preiner et al. Phys.Rev.Lett. 99 2007 (046102)

  • Simulation

    • Numerically solving EQM

    • Stepwise approach to the surface in 0.1 nm steps

    • FFT analysis of the solution (timetrace) at every step=> frequency spectra

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    J.Preiner et al. Phys.Rev.Lett. 99 2007 (046102)

  • Simulation of amplitude vs. distance curves

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    Simulation

    Reference

    Experimental Setup:

    Data Acquisition:NI PCI-6013200 kS/s, 16 bit

    1

    2

    J.Preiner et al. Phys.Rev.Lett. 99 2007 (046102)

  • Comparison between simulation and experimental data

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    Simulation Experiment

    J.Preiner et al. Phys.Rev.Lett. 99 2007 (046102)

    A0=4 nm;Asp=3.5 nm

  • Dependence of the 2nd harmonic amplitude on interaction parametersContact Mechanics (DMT-model):

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    J.Preiner et al. PRL 99 2007 (046102)

  • Dependence of the 2nd harmonic amplitude on interaction parameters

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    Music: different instruments can be distinguished even when they are playingthe same note

    Reason: it‘s not only the fundamental notewhat defines the timbre (color of sound) but the sum of the fundamental note and all the harmonics

    Analogy to AFM: recording harmonics in the cantilever movement (timbre) enablesto distinguish different interactions

  • Topography 2nd Harmonic Amplitude

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    Images of bacterial S-Layer(sbpA, Bacillus sphaericus CCM 2177)

    (A0=10 nm,Asp/A0=0.85,fd 7.3kHz, k=0.1 N/m,PBS Buffer)

    Periodicity~14 nm

    Amplitude

    color code: 0-5 nm

    J.Preiner et al. Phys.Rev.Lett. 99 2007 (046102)

    Phase

    12

  • Rhino Virus (HRV2)

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    Topography 2nd Harmonic Amplitude

    color code: 0-13 nm

    (A0=15 nm, Asp/A0=0.9, fd 7.9 kHz, k=0.1 N/m, Ni-Tris Buffer)

    J.Preiner et al. Phys.Rev.Lett. 99 2007 (046102)

  • Imaging Recognition using 2ndHarmonic

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    Simulation and experimental verification of dynamic approaching curves revealed characteristic signature of molecular recognition in 2nd harmonic amplitude

    Additional non-linear forcedue to PEG-linker stretching:

    NH2

    2HNNH2

    NH22HN2HN

    NH2

    N

    NH

    PEG

    O

    OO

    O

    O

    "NHS"

    N

    NH

    PEG

    O

    OO

    O

    O

    "NHS"

    SMCC

    PEGPEG

    S S

    COOH

    T EPC

    Strep-tactin

    NH C

    O N

    O

    O

    ( )( )[ ] ⎥⎥⎦

    ⎢⎢⎣

    ⎡+−

    −=

    02

    0 41

    /241

    Lz

    LzLTkzFP

    BWLC

  • AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

    Imaging Recognition using 2ndHarmonic

    Coparison of TREC and 2nd harmonic imaging of mol. recognition

    • Bacterial S-Layer SbpA

    • native:Strep tagged=7:1

    • Streptactin on tip

    NH2

    2HNNH2

    NH22HN2HN

    NH2

    N

    NH

    PEG

    O

    OO

    O

    O

    "NHS"

    N

    NH

    PEG

    O

    OO

    O

    O

    "NHS"

    SMCC

    PEGPEG

    S S

    COOH

    T EPC

    Strep-tactin

    NH C

    O N

    O

    O

    • Block with free Strep tag II

  • Summary• Simulations of dynamic AFM in liquid:

    Amplitudes of higher harmonics are sensitive to variations in the nonlinear tip-sample interactions

    • 2nd harmonic images of various samples in liquid (S-layer, HRV2,) showed detailed substructures not visible in topographical images

    • 2nd harmonic images of molecular recognition

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz

  • Acknowledgments

    JKU Linz:

    Johannes PreinerJilin TangVasilli PastushenkoAndreas Ebner

    BOKU Vienna:

    Uwe SleytrNicola Ilk

    Vienna Biocenter:

    Dieter Blaas

    Funding:European ComissionFORCETOOL, No. NMP3-CT-2004-013684

    AFM – GroupInstitute of BiophysicsJ. Kepler University Linz