The Peak Force Tapping and QNM modes allow the simultaneous acquisition of 3D topography and mechanical parameters. The force applied on the tip is controlled in order to preserve the integrity of the sample and the AFM tip. The approach-retraction curves (2 kHz) are obtained (force spectroscopy) and analyzed in real time in order to extract the mechanical parameters (Young's modulus, tip-surface adhesion, deformation...). In QNM mode, the measurements become quantitative after calibration of the tip.
A pulsed source of mono or multi-atomic primary ions (Ga+, Bin+, Au+, C60+, ...) with an energy of a few keV bombards the sample surface. The secondary ions resulting from the interaction between the primary ions and the sample are then focused and accelerated with the same kinetic energy towards the time-of-flight analyzer which separates them according to their m/z ratio with a very good mass resolution (ΔM/M > 10 000 at mass 28).
The adhesion of the different layers is an essential property for the good combustion of solid propellant in rocket engines. When a macroscopic adhesion defect is observed, an investigation of the mechanical properties at the micrometer scale can provide solutions. Figure 1 shows the presence of an interphase at the interface binder (right)/thermal protection (left) which displays a smooth topography and a high Young's modulus. It can be schematized as a dotted cut along the two assembled layers. This defect weakens the adhesion between the bonder and the thermal protection, making the assembly unusable. A comparison of the results obtained via the Peak Force QNM mode of AFM and by nanoindentation was carried out on different propellant formulations (Table 1). The measurements acquired by the two techniques correspond, the AFM can thus be used in replacement of a nanoindenter on isotropic materials. A complementary analysis of the linker/thermal protection interface using ToF-SIMS (Figure 2) showed the increased presence of the cross-linking agent used in the linker formulation. This migration at the interface with the thermal protection is accompanied by a local over-crosslinking of the linker and explains the higher Young's modulus measured by AFM. A modification of the linker formulation allowed to correct the adhesion defect and to obtain an interface as in figure 3.