We have measured the non-local resistance of aluminum-iron spin-valve structures fabricated by e-beam lithography and shadow evaporation. The sample geometry consists of an aluminum bar with two or more ferromagnetic wires forming point contacts to the aluminum at varying distances from each other. In the normal state of aluminum, we observe a spin-valve signal which allows us to control the relative orientation of the magnetizations of the ferromagnetic contacts. In the superconducting state, at low temperatures and excitation voltages well below the gap, we observe a spin-dependent non-local resistance which decays on a smaller length scale than the normal-state spin-valve signal. The sign, magnitude and decay length of this signal is consistent with predictions made for crossed Andreev reflection (CAR).Singlet superconductivity and ferromagnetism are competing long-range orders which favor a different alignment of electron spins, antiparallel and parallel, respectively. Therefore, they generally exclude each other in homogenous bulk materials. In mesoscopic hybrid structures, the interplay of superconductivity and ferromagnetism leads to rich novel physics. Recent experimental studies on equilibrium properties of superconductorferromagnet (SF) interfaces have shown that the local density of states (LDOS) on the superconducting side is strongly affected by the pair breaking effect of the ferromagnetic exchange field [1], and on the ferromagnetic side an oscillatory behavior of the LDOS due to the exchange splitting of the spin sub-bands has been observed [2]. Transport properties of SF point contacts [3,4,5] and FSF planar junctions [6] show a suppression of spin-polarized current injection into the superconductor, and in SFS Josephson junctions [7,8,9], a π-state with a spontaneous equilibrium Josephson current is observed. In this work, we report on spin-dependent transport properties of the superconducting condensate on length scales comparable to the coherence length. We have combined ferromagnet-superconductor point contacts with a non-local spin-valve geometry, and find evidence for crossed Andreev reflection (CAR), i.e. the splitting of a Cooper pair into two spatially separated leads. Figure 1 shows an SEM image of one of our samples, together with a schematic view of the experiment. The samples were fabricated by e-beam lithography and shadow evaporation techniques. First, 20 nm of iron is evaporated onto an oxidized silicon substrate to form a series of wires (vertical), with varying width (50-120 nm) and a small tip at the end. Their elongated shape creates a magnetic shape anisotropy which confines their magne- tizations to be aligned along the wires, pointing either upwards or downwards, with different coercive fields due to the width variation. In a second evaporation step under a different angle, and without breaking the vacuum, an aluminum bar of 80 nm height and 250 nm width (horizontal), is created. It slightly touches the iron wires, forming metallic contacts of about 20 × 50 nm, much smalle...