Minimization of internal degrees of freedom is an important step in the cooling of atomic species to degeneracy temperature. Here, we report on the loading of 5 6 10 thulium atoms optically polarized at maximum possible magnetic quantum number 4 F m state into dipole trap operating at 532 nm. The purity of polarizations of the atoms was experimentally verified using a Stern-Gerlach-type experiment. Experimental measured polarization of the state is 3.91 0.26 F m .
II. INTRODUCTIONCold atoms with temperatures equal or close to the temperature of degenerate gas [1] have attracted a lot of attention in recent years due to their potential in various applications ranging from frequency standards and metrology [2,3] to quantum simulation of electro-magnetic properties of solid state materials [4][5][6], turbulence [7] or even the formation of stars [8].Lanthanides have a special place in the field of quantum simulations due to their unique properties, such as large orbital momentum [9,10] and large magnetic momentum in the ground state [11,12]. Large orbital momentum in the ground state leads to easily tunable interactions between cold atoms via lowfield Feshbach resonances [13], while large magnetic momentum leads to relatively strong dipole-dipole interactions [10]. In particular, the thulium atom has an orbital angular momentum of 3 and magnetic moment of 4 Bohr magnetons in the ground state. In addition, it has a relatively simple level structure, thus combining the strength of more developed Er and Dy [9,14] with the advantage of a clearer system.Cooling of the thulium atom to the Bose-Einstein condensation (BEC) has not been achieved yet.Traditionally, the last step in cooling to BEC temperatures is done via evaporative cooling, either in a magnetic or in an optical dipole trap (ODT). In the case of the thulium atom, inelastic collisions in a magnetic trap were measured and found to be quite substantial [15]; therefore, we selected the optical