Circularly polarized light can induce additional mode conversion when it interacts with a material that rotates the orientation of the plane of polarization, which is known as “optical rotation” or “rotary polarization”. The effect of this additional mode conversion phenomenon is studied in the framework of the optical radiation force theory. The time-averaged force (per-length) acting on an infinitely long perfect electromagnetic conductor (PEMC) circular cylinder is considered. The multipole modal expansion method in cylindrical coordinates is utilized to derive exact series expansions for the components of the longitudinal radiation force per-length (i.e. acting along the direction of wave propagation) applicable to any range of frequencies. Numerical predictions for the radiation force function (which is the radiation force per unit energy density and cross-sectional surface) and its components clearly demonstrate the contribution of the co-polarized and cross-polarized waves. It is shown that the total radiation force is not the mere sum of the TM and TE mode components in a circularly polarized wave-field. There is an additional cross-interference term describing the contributions of TM ⇄ TE mode conversion to the total force that cannot be neglected. The computations show that the interference term can be positive, null or negative as the dimensionless size parameter ka and admittance M of the cylinder vary (where k is the wavenumber in the medium of wave propagation and a is the radius of the cylinder). The results show that the total force is always positive and acts in the direction of wave propagation (i.e., force of repulsion). The analysis is further extended to compute the energy efficiencies, demonstrating the validity of the results from the standpoint of energy conservation. This work generalizes the radiation force formalism for linearly polarized fields by introducing additional terms corresponding to TM ⇄ TE mode conversions in the series expansion for the longitudinal radiation force on cylindrical materials exhibiting rotary polarization in circularly polarized plane progressive waves.
Read full abstract