In monolayer Transition Metal Dichalcogenides (TMDs) the valence and conduction bands are spin split because of the strong spin-orbit interaction. In tungsten-based TMDs the spin-ordering of the conduction band is such that the so-called dark exciton, consisting of an electron and a hole with opposite spin orientation, has lower energy than the A exciton. A possible mechanism leading to the transition from bright to dark excitons involves the scattering of the electrons from the upper to the lower conduction band state in K. Here we exploit the valley selective optical selection rules and use two-color helicity-resolved pump-probe spectroscopy to directly measure the intravalley spin-flip relaxation dynamics of electrons in the conduction band of single-layer WS2. This process occurs on a sub-ps time scale and it is significantly dependent on the temperature, indicative of a phonon-assisted relaxation. These experimental results are supported by time-dependent ab-initio calculations which show that the intra-valley spin-flip scattering occurs on significantly longer time scales only exactly at the K point. In a realistic situation the occupation of states away from the minimum of the conduction band leads to a dramatic reduction of the scattering time.Transition metal dichalcogenides (TMDs) are promising for opto-electronics[1-4], valleytronics[5-9] and quantum information processing [10]. Monolayers (1L) of TMDs are direct bandgap semiconductors[11] whose optical properties are dominated by excitons with binding energies of up to several hundred meVs [12][13][14][15][16][17][18]. The valence/conduction (VB/CB) band extrema lie at the non-equivalent K and K' points on the edge of the Brillouin zone [19,20]. Their spin-degeneracy is lifted by strong spin-orbit (SO) interaction [21]. For the VB the energy splitting ∆ v ranges between 150 and 400meV [22], while for the CB ∆ c it is one/two orders of magnitude lower (∼1-30meV) [23,24]. Together with a broken inversion symmetry, this results in spin-polarized bands and valley-dependent dipole-allowed interband optical transitions, as first detected by helicity resolved photoluminescence (PL) measurements [25][26][27].The large VB splitting gives rise to two distinct interband transitions (called A and B) strongly renormalized by excitonic effects [16], dominating the optical response in the visible range [22]. Recent theoretical calculations predicted that, while the spin orientation of the upper and lower CB states is antiparallel in K/K', in W-based 1L-TMDs, the upper CB state has the same spin orientation as the upper VB. A direct consequence of this spin-ordering is the formation of an intravalley (i.e. zero momentum) dark exciton with a lower energy than the bright exciton [28][29][30][31][32][33]. The bright to dark exciton transition reduces the PL quantum yield in W-based 1L-TMDs for decreasing temperatures, as recently shown [33]. The formation of dark excitons requires scattering processes such as intravalley relaxation. We stress that other excitonic comple...