Tapping Mode

Tapping mode is a type of an amplitude modulation (AM) technique, in which relatively large-amplitude vibrations of the AFM probe are applied for imaging. It allows for measurements to be made at ambient conditions. When the oscillating AFM probe hits the sample, its short-time interactions with minimal shear are less destructive than the tip-sample forces in contact mode.

Fig. 1. Tapping mode topography image of self-assembled structures of semifluorinated alkanes on silicon (Agilent 5500 AFM, standard tapping mode AFM probe). Scan size 350x350nm. Scan height 5nm. Image courtesy of S. Magonov, Agilent Technologies.
Tapping mode, semifluorinated alkanes self-assembled structures on Si, 350x350nm, height 5nm, p.c. S.Magonov, Agilent

 

For identifying a type of tip-sample force, e.g. attractive or repulsive, recording of the phase behavior of the AFM probe (for example, as phase shift dependence on tip-sample separation) can be used. Actually, at small amplitudes the operation in tapping mode is characterized by attractive tip-sample forces and overlaps with the operation in non-contact mode. The latter mode is characterized by small probe oscillations and net attractive interactions which does not necessary mean true non-contact regime.

Tapping mode AFM in air

Stable oscillations of the tapping AFM probe are possible when the AFM cantilever has enough energy to overcome the adhesive and capillary forces of the samples in air. Traditionally, silicon AFM probes with stiffness in the 30-50N/m range, such as the HQ:NSC15, are used for tapping mode experiments. Depending on the type of the sample and problem to solve, AFM probes with stiffness ranging from 0.3N/m to 400N/m may be required. AFM probes with low stiffness should be applied to soft materials or particles with low adhesion to the surface. Stiff AFM probes are used for imaging at the elevated forces needed for the visualization of mechanically-different components of multicomponent samples.

The stiffness of the AFM probe is only one of the parameters that influence tip-sample forces in tapping mode. The other parameters are two amplitudes: the amplitude of the free oscillating probe and the set-point amplitude used for the feedback. The difference between the set-point and free amplitude determines the tip-sample force level, which controls the image contrast.

Between two AFM cantilevers with a given spring constant, the one with the higher resonance frequency is preferable because it allows for a faster scan rate. AFM cantilevers with a high resonance frequency of 300kHz and above provide the fastest possible scan rates. It should also be taken into account that polymer surfaces become stiffer at higher frequencies. This property further reduces the possibility of sample damage when using a high resonance frequency AFM cantilever.

High Q-factor is desirable in tapping mode to optimize the sensitivity. For a given resonance frequency and spring constant, a rectangular AFM cantilever generally has the higher Q-factor in comparison to its triangular analog.

Important: If an AFM study involves heating the AFM probe, silicon AFM cantilevers without any coating are preferred. Coated AFM cantilevers can bend and/or twist at elevated temperatures.

Hi'Res-C AFM tips provide extremely high resolution when used in light tapping mode on smooth surfaces. See the application note on high resolution imaging for details.

Tapping mode in liquids

If a particular sample seems to be having problems with adhesive capillary tip-sample forces, these forces can be substantially reduced by immersing the AFM tip and the sample in a liquid, which generally requires the use of a liquid cell accessory. Further reduction of the attractive forces is possible by operating in appropriate solvents, especially ethanol. The liquid cell is also used for in-situ electrochemical and biological experiments.

Conventional liquid cells have a drive frequency of about 10kHz. This matches the resonance frequency of AFM cantilevers that vibrate in air at about 50-70kHz. Typical values of the Q-factor in liquids are 1-3 due to increased hydrodynamic damping. Rectangular AFM cantilevers suffer less damping in liquids than triangular AFM cantilevers.

Important: The aluminum reflective coating is usually stable in water and ethanol. However, certain experimental conditions may cause corrosion of the coating. For example, Al dissolves readily in caustic alkali solutions and forms aluminum hydroxide. It's generally recommended to use uncoated cantilevers or cantilevers with Cr-Au back side coating in liquids.


Further reading

Lift mode

 

Tapping Mode

Robust samples in air
HQ:NSC AFM probes with high force constant
HQ:NSC15/Al BS

Soft, weakly-adhering, or fragile, samples in air
HQ:NSC AFM probes with medium force constant
HQ:NSC14/Al BS

Near-liquid samples in air
HQ:NSC AFM probes with medium force constant
HQ:NSC19/Al BS

High-resolution in air
Hi'Res-C AFM probes with medium force constant
Hi'Res-C14/Cr-Au

In liquid (water)
AFM probes with resonance frequency 50-70 kHz
HQ:NSC18/Cr-Au BS

In aggressive liquid medium
AFM probes with resonance frequency 50-70 kHz having chemically inert coating
HQ:NSC18/Cr-Au