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1 article(s) from Cappella, Brunero

Application of contact-resonance AFM methods to polymer samples

Sebastian Friedrich and
Brunero Cappella

Beilstein J. Nanotechnol. 2020, 11, 1714–1727, doi:10.3762/bjnano.11.154

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Figure 1: The function D without approximations (Equation 2) and with both approximations (Equation 4 and Equation 5) for γ = 0.97. The top...

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Figure 2: The function α without approximations (Equation 1) and its three approximations α_c (Equation 8), α_t (Equation 10), and α_ξ (Equation 12). The ...

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Figure 3: Error ΔE_tot engendered by an uncertainty Δf_n/f_n⁰ = 1%, calculated from Equation 20 with γ = 0.97, F = 100 nN, R...

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Figure 4: Tapping-mode topography image of a 100 nm thick PnBMA film after a smaller area (15 µm)² was scanne...

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Figure 5: CR frequency f(t) in the first mode as a function of the measuring time on three PnBMA films with t...

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Figure 6: CR frequencies as a function of the force F on glass (diamonds), bulk PMMA (triangles), and bulk PS...

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Figure 7: CR frequency as a function of the force F on glass (diamonds), bulk PMMA (white triangles), and bul...

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Figure 8: Normalized contact stiffness α on glass (white diamonds, calculated with γ = 0.982, and grey diamon...

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Figure 9: CR frequency as a function of the normalized contact stiffness α_H = k_s,H/k_c on glass (open and full...

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Published 12 Nov 2020

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