We describe an ultracold fermionic set-up where it is possible to synthesize a superfluid phase with symmetry obtained by locking independent invariance groups of the normal state. In this phase, named two-flavors symmetry-locking phase (TFSL), non-Abelian fractional vortices with semi-integer flux and gapless non-Abelian Goldstone modes localized on them appear. Considerations on the possible experimental realization of the TFSL are also provided. [3]. The possibility to synthesize Abelian and non-Abelian gauge fields, also in the presence of optical lattices [4][5][6][7][8][9], promises a better understanding of an increasing number of relevant physical systems and new phases of gauge field theories. In the non-Abelian case, hyperfine levels of suitable atoms are typically used as internal degrees of freedom where the gauge potential is defined: an advantageous proposal is given by earth-alkaline atoms [10]. To date, only static gauge fields have been experimentally simulated, but proposals for dynamical fields recently appeared in literature [11][12][13][14][15]. A further promising and challenging application of ultracold atoms and synthetic gauge fields is the emulation of relativistic models relevant to high energy physics: recent proposals focused on 2D [16][17][18][19][20][21][22][23] These intensive efforts are also expected to progress towards a better understanding of strongly coupled nonAbelian gauge theories, like quantum chromodynamics (QCD), and potentially to give new insights on the QCD phase diagram. Indeed in QCD various problems stay unsolved, like the origin of color confinement [32], chiral symmetry breaking (CSB), as well as the dynamics of nucleons, nuclear matter or quarks under extreme conditions [33,34]. In the light of the developments mentioned above, ultracold atoms can become a precious tool in the investigation of these important topics.