Use policyThe full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-pro t purposes provided that:• a full bibliographic reference is made to the original source • a link is made to the metadata record in DRO • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders.Please consult the full DRO policy for further details. Atomic force microscopy's 7 (AFM) ability of visualizing the topography and the property of surfaces and interfaces at a molecular level 8 has enabled a rapid development in the understanding of surface phenomena. Its versatility allows the exploration of hard and soft materials in vacuum 9-12 , in air 13 , but also in complex liquids 14,15 , often allowing imaging at sub-nanometre and sometimes atomic resolution 16 . In dynamic mode 17 (vibrating cantilever), AFM has proven sensitive to the interfacial compliance of viscous liquids and provided quantitative information about the structure of liquid layers between the AFM tip and the solid surface 18 , with, in some cases, atomic resolution 15 . However, specialized instruments were used and the nature of the tip-sample interaction remains an issue of debate. Dynamic AFM has the ability to probe the solid-liquid interface [18][19][20][21] , but an interpretation of experimental results remains difficult 22,23 . Traditionally, interfaces are characterized by an interfacial energy, IE, the sum of the two surface energies in vacuum minus the work of adhesion (W SL ) necessary to separate the surfaces (Dupré Equation 24 ). The latter is de facto the energy spent to restructure the interface due to the atomistic interaction between the two materials (Fig. 1c). In practice at a solid-liquid interface this is the energy that generates density variations and structuring of the liquid close to the interface. Hereafter we will call this layer of liquid which differs from the bulk