Structure of light antikaon-nuclear quasi-bound states, which consist of an antikaon (K = K − ,K 0 ) and a few nucleons (N = p, n) such asKN N ,KN N N ,KN N N N andKN N N N N N systems, is studied with full three-to seven-body calculations. Employing a realisticKN potential based on the chiral SU(3) effective field theory with the SIDDHARTA constraint, we show that the central nucleon densities of these systems increases when the antikaon is injected, by about factor of two at maximum. TheKN N N N system shows the largest central density, about 0.74 fm −3 even with the phenomenologicalKN potential, which are not as high as those suggested in previous studies with approximate treatments of the few-body systems. We find the spin of the ground state of theKN N N N N N system depends on the strength of theKN attraction. Thus, the quantum number of the ground state can be another constraint on theKN interaction.