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Beilstein J. Nanotechnol. 2016, 7, 1033–1043, doi:10.3762/bjnano.7.96
Figure 1: Simple model for two coupled harmonic oscillators, each represented by a mass (m1, m2), a sping (k1...
Figure 2: Calculated amplitude response for the cantilever (subsystem 1) with and without frequency matching ...
Figure 3: SEM images (a) of the fabricated sensor, (b) and (c) of the free end of the FeCNT before and after ...
Figure 4: Sketch of measurement positions which are reached by keeping the sensor position fixed and rotating...
Figure 5: Simulated magnetic field of the permanent magnet. The field dependence on the distance to the surfa...
Figure 6: Amplitude response curves of the cantilever measured at the field-free position (3) according to Figure 4 a...
Figure 7: Measured frequency shifts of both peaks (a) and (b) compared to the field free measurement for vari...
Figure 8: Dependence of the effective spring constant of each peak on the interaction spring constant k3. Th...