“…Thus, through this procedure, the particle is subjected to the so called geometric potential [10]. Recently, the da Costa proposition appeared in various physical contexts as, for instance, in the derivation of the Pauli equation for a charged spin particle confined to move on a spatially curved surface in the presence of an electromagnetic field [11], in the study of curvature effects in thin magnetic shells [12], in effects of non-zero curvature in a waveguide to investigate the appearance of an attractive quantum potential which crucially affects the dynamics in matter-wave circuits [13], in the quantum mechanics of a single particle constrained to move along an arbitrary smooth reference curve by a confinement that is allowed to vary along the waveguide [14], to derive the exact Hamiltonians for Rashba and cubic Dresselhaus spin-orbit couplings on a curved surface with an arbitrary shape [15], in the study of highorder-harmonic generation in dimensionally reduced systems [16], to explore the effects arising due to the coupling of the center of mass and relative motion of two charged particles confined on an inhomogeneous helix with a locally modified radius [17], to study the dynamics of shape-preserving accelerating electromagnetic wave packets in curved space [18], in the derivation of the Schrö dinger equation for a spinless charged particle constrained to move on a curved surface in the presence of an electric and magnetic field [19], etc.…”