The magnetic penetration depth λ has been measured in MgCNi3 single crystals using both a high precision Tunnel Diode Oscillator technique (TDO) and Hall probe magnetization (HPM). In striking contrast to previous measurements in powders, δλ(T) deduced from TDO measurements increases exponentially at low temperature, clearly showing that the superconducting gap is fully open over the whole Fermi surface. An absolute value at zero temperature λ(0) =230 nm is found from the lower critical field measured by HPM. We also discuss the observed difference of the superfluid density deduced from both techniques. A possible explanation could be due to a systematic decrease of the critical temperature at the sample surface.PACS numbers: 74.25. Nf, 74.25.Op, 74.70.Dd The interplay between magnetism and superconductivity is currently a subject of great interest. In the UGe 2 and URhGe uranium compounds, for instance, a long range ferromagnetic ordered phase coexists with the superconducting phase and a mechanism of spin fluctuations (SF) could be at the origin of the Cooper pair formation [1, 2]. The recent discovery of high temperature superconductivity in oxypnictides also rapidly became the topic of a tremendous number of both experimental and theoretical works. The parent undoped LnOFeAs (where Ln=La,Sm,...) compound is here close to itinerant magnetism due to the presence of a high density of Fe d states at the Fermi level [3], leading to competing ferromagnetic and antiferromagnetic fluctuations. Similarly in the cubic (anti-)perovskite MgCNi 3 compound [4], the presence of a strong Van Hove singularity in the density of Ni states slightly below the Fermi level also leads to strong ferromagnetic fluctuations [5][6][7][8][9]. These two systems have also a Fermi surface composed of both electron and hole pockets (3D sheets in MgCNi 3 as compared to quasi-cylindrical sheets in oxypnictides).Despite these striking similarities in their electronic and magnetic properties, spin fluctuations lead to very different effects in those systems. On the one hand, ab-initio calculations rapidly showed that the electronphonon coupling constant (λ e−ph ∼ 0.2) is far too low to account for the high critical temperatures observed in oxypnictides (up to ∼ 55 K) and an unconventional mechanism mediated by the SF associated with a sign reversal of the (s-wave) order parameter between electrons and holes sheets of the Fermi surface has been proposed [10]. On the other hand, it has been suggested that the narrow van Hove singularity could be responsible for a nearly unstable phonon mode in MgCNi 3 inducing a large, although reduced by SF, λ e−ph [11,12] in agreement with experiments which yield an average electronphonon coupling constant in the order of 1.7 [11,13,14]. The interplay between electron-phonon coupling and SF is further emphasized in this system by the existence of a large isotopic effect [15] which has been suggested to be enhanced by the strong SF [16].In this context, the nature of the superconducting order parameter rapidl...