Neutron spin echo has revealed the single chain dynamic structure factor of entangled polymer chains confined in cylindrical nanopores with chain dimensions either much larger or smaller than the lateral pore sizes. In both situations, a slowing down of the dynamics with respect to the bulk behavior is only observed at intermediate times. The results at long times provide a direct microscopic measurement of the entanglement distance under confinement. They constitute the first experimental microscopic evidence of the dilution of the total entanglement density in a polymer melt under strong confinement, a phenomenon that so far was hypothesized on the basis of various macroscopic observations. DOI: 10.1103/PhysRevLett.104.197801 PACS numbers: 61.41.+e, 62.25.Àg, 78.70.Nx, 82.35.Lr Confinement effects in polymer melts may lead to unusual properties. This concerns both the chain conformation, which may be distorted, as well as chain dynamics, which may be altered due to surface interactions and changes of topology and chain self-density [1][2][3][4]. The understanding of such behavior is not only a scientific challenge but is also important for knowledge-based applications in nanotechnology, such as nanocomposites, coatings, adhesives, etc. [5]. Today, microscopic studies on the chain dynamics under confinement are mainly available through simulations. Only a few experiments have addressed this problem, e.g., the flow of polymers through nanopores, the extensional rheology of nanosized polymer films, the observation of dewetting kinetics of thin films or NMR relaxometry. Chain dynamics is commonly described in terms of the Rouse and the reptation model. The relaxation of the Rouse modes, determined by a balance of viscous and entropic forces, only depends on the chain length and the monomeric friction. In addition, long polymers heavily interpenetrate each other and mutually restrict their motions at long times in forming topological constraints (''entanglements''). In the reptation model the entanglement effect is modeled by a tube of diameter d $ ' ffiffiffiffiffiffi N e p along the coarse grained chain profile confining the chain motion (', monomer length; N e , number of monomers between the entanglements). The dominant motional mechanisms in this model are (i) a curvilinear version of the Rouse motion (local reptation) followed by (ii) the escape of the whole molecule from the tube at long times, the reptation process (see, e.g., [6,7]). The important question that is addressed now both by simulations [2,3,8,9] as well as by a variety of experiments on a macroscopic level [4,[10][11][12] is how these dynamics change under confinement.Basically all simulations available indicate that confinement reduces chain mobility independent of the adhesive potential of the wall. An analysis of the Rouse modes of unentangled chains under confinement reveals a uniform slowing down of all modes which was interpreted by an effective increase of monomeric friction [8]. The consequences for the entanglement density are less...