“…The three-nucleon force is acknowledged since many decades as an important component of the nuclear interaction. This has been firmly established at the beginning of the current century, when very accurate models of the two-nucleon component of the nuclear interaction, describing thousands of scattering data with a 2 close to 1, became available, either in the form of phenomenological potentials, such as the AV18 [1] or the CD-Bonn [2], or derived within the chiral effective field theory (ChEFT) [3][4][5]. At the same time, accurate numerical methods were developed, which enabled the computation of light-nuclei binding energies from first principles, i.e.…”