“…This is achieved by transverse collimation of the beam of metastable atoms using two-dimensional (2D) transverse radiative pressure forces (Aspect et al, 1990;Hoogerland et al, 1996b;Metcalf and van der Straten, 1999;Morita and Kumakura, 1991;Partlow et al, 2004;Rasel et al, 1999;Rooijakkers et al, 1996;Shimizu et al, 1987Shimizu et al, , 1990Vansteenkiste et al, 1991), focussing in a hexapole (Woestenenk et al, 2001) or 2D magneto-optical compression (Labeyrie et al, 1999;Schiffer et al, 1997;Scholz et al, 1994). For maximum efficiency, the collimation zone, which has a typical length of several to a few tens of cm, has to be implemented as close as possible to the source, typically directly after the skimmer.…”