We calculate the Casimir force between parallel plates for a discrete
massless scalar field. The scalar field forms a periodic lattice in continuous
spacetime. The dispersion relation for both the square and triangular lattices
allows for the accurate reproduction of the subtle Casimir effect without
encountering infinite quantities. Our findings demonstrate that the Casimir
force is independent of the type of periodic lattice used. At low frequencies,
we observe a high level of rotational symmetry in both lattices. However, at
high frequencies, both lattices lose their rotational symmetry, although the
propagation of high-frequency waves becomes significantly limited as their
group velocity approaches zero. We claim that the behavior of physics in
discrete fields becomes similar to that in the continuous case, with the
exception that we now have a natural and smooth cutoff mechanism that proves
useful in cases requiring regularization. It appears that we have found an
alternative approach to regularization using lattices with different symmetries
in the background of continuous spacetime.Comment: 10 pages, 9 figure