High resolution laser Stark excitation of np (60 < n < 85) Rydberg states of ultra-cold cesium atoms shows an efficient blockade of the excitation attributed to long-range dipole-dipole interaction. The dipole blockade effect is observed as a quenching of the Rydberg excitation depending on the value of the dipole moment induced by the external electric field. Effects of eventual ions which could match the dipole blockade effect are discussed in detail but are ruled out for our experimental conditions. Analytic and Monte-Carlo simulations of the excitation of an ensemble of interacting Rydberg atoms agree with the experiments indicates a major role of the nearest neighboring Rydberg atom.PACS numbers: 32.80. Rm; 32.80.Pj; 34.20.Cf; 34.60.+z Long-range dipole-dipole interactions often play an important role in the properties of an assembly of cold atoms. One example is the efficiency of photoassociation of cold atoms and the formation of cold molecules [1]. In the case of a Rydberg atomic ensemble, the range of the dipole-dipole interactions can exceed several micrometers, leading to many-body effects [2,3,4]. An interesting application of the dipole-dipole interaction is the dipole blockade (DB) in Rydberg excitation. This effect offers exciting possibilities for quantum information [5] with the fascinating possibilities for manipulating quantum bits stored in a single collective excitation in mesoscopic ensembles, or for realizing scalable quantum logic gates [6]. The DB process for an ensemble of atoms is the result of shifting the Rydberg energy from its isolated atomic value due to the dipole-dipole interaction with the surrounding atoms. In a large volume, a partial or local blockade, corresponding to a limitation of the excitation is expected when the dipole-dipole energy shift exceeds the resolution of the laser excitation. In a zero electric field, Rydberg atoms present no permanent dipole and usually no DB is expected. Nevertheless, a van der Waals blockade, corresponding to a second order dipole-dipole interaction, has been observed through a limitation of the excitation of high Rydberg states np (n ∼ 70 − 80) of rubidium, using a pulsed amplified single mode laser [7]. CW excitations have also been performed [8,9] showing the suppression of the excitation and affecting the atom counting statistics [8]. The DB phenomenon itself has been observed for the first time, in the case of cesium Rydberg atoms, for a so called Förster Resonance Energy Transfer (FRET) reaction, np + np −→ ns + (n + 1)s [10]. The FRET configuration has several advantages: the dipole-dipole interaction can be tuned on and off by the Stark effect, the dipole-dipole interaction having its * Laboratoire Aimé Cotton is associated to Université ParisSud and belongs to Fédération de Recherche Lumière Matière (LUMAT). maximum effect at the resonant field. Its main drawback comes from the fact that the resonance exists only for n ≤ 41 in the cesium case, which limited the observed DB to an efficiency of ∼ 30%.In this letter, we report t...