Electron holography in a transmission electron microscope was applied to measure the phase shift ∆ϕ induced by Au clusters as a function of the cluster size. Large ∆ϕ observed for small Au clusters cannot be described by the well-known equation ∆ϕ = CEV0t (CE: interaction constant, V0: mean inner Coulomb potential (MIP) of bulk gold, t: cluster thickness). The rapid increase of the Au MIP with decreasing cluster size derived from ∆ϕ, can be explained by the compressive strain of surface atoms in the cluster.PACS numbers: 61.14. Nm, 81.07.Bc, 68.37.Lp Au clusters are considered as prototype material for nano-scaled electronic devices and biosensors [1]. Moreover, Au clusters exhibit an exceptional catalytic activity [2]. All these potential applications have motivated numerous studies regarding the properties of Au nano-clusters. One fundamental material property is the mean inner Coulomb potential (MIP), which plays an important role for the quantitative evaluation of experimental data obtained from electron scattering techniques, e.g. transmission electron microscopy (TEM) and electron holography (EH). The MIP is the volume-averaged electrostatic part of the crystal potential, which can be expressed [3,4] bywith Planck's constant h, the electron mass and charge m and e, the unit cell volume Ω and the occupation number n i for the atomic species i within the unit cell. The important property in Eq. (1) is the atomic scattering factor f el i (0) [5] which correlates the MIP with the amplitude of the electron wave scattered in forward direction. The MIP can be determined by off-axis EH under kinematical diffraction conditions according to the relation ∆ϕ = C E V 0 t (C E : interaction constant) by measuring the phase shift ∆ϕ between the electron wave passing through the sample with a known thickness t and a vacuum reference wave [6]. On the other hand, local TEM sample thicknesses can be determined by EH, if precise values of the MIP are known, but thus far only MIP values for few materials with limited accuracy are available [7,8,9,10,11]. For instance, experimental values for the MIP of Au between 16.8 and 30.2 V were reported [8], whereas calculations yield values of 25.0 to 35.9 V [7,8,11]. Moreover, a strong increase of the Au MIP up to 45 V was reported for Au clusters deposited on T iO 2 powder with decreasing cluster size [12]. Recently, effective carbon MIP values up to 65 V were reported for ultra-thin amorphous carbon (a-C) films compared to a bulk value of 9 V [13]. This indicates that the MIP increase for nano-scaled objects could be a general phenomenon. In this study, we applied EH to determine 1) the MIP of bulk Au, which corresponds to the MIP of Au atoms in the cluster core and 2) the contribution of surface atoms to the overall MIP of Au clusters to elucidate the physical origin of its increase.Samples were prepared by low-energy-beam cluster deposition of Au n clusters with 10≤n≤20 atoms on commercial a-C substrates, ≈10 nm thick. Due to the storage of the sample, a coarsening of the partic...