Khalid Aloufi | Searcharxiv

arXiv2023

A revision of the forces exerted in the Rayleigh regime by a tighlty focused optical vortex tweezer

Optical tweezers use light from a tightly focused laser beam to manipulate the motion of tiny particles. When the laser light is strongly focused, but still paraxial, its e/m field is characterized by a longitudinal component which is of magnitude comparable to the transverse ones and which has been ignored in the theoretical analysis of the tweezing forces. In our work we revise the calculations of the various components of the radiation pressure force, within the limits of Rayleigh regime or dipole approximation, in the case where a tiny particle interacts, in free space, with a circularly polarized optical vortex beam, by taking into account this ignored field term. We show that this term is responsible for considerable modifications in the magnitude of the various components, moreover and also for the appearance of terms involving the coupling of the spin angular momentum (SAM) and the orbital angular momentum (OAM) of the photons of the vortex beam. We compare our findings with the ones taken ignoring the longitudinal field component.

physics.optics↗

arXiv2014

Dynamics of entangled states in squeezed reservoirs

Dynamics of entangled states of two independent single-mode cavities in squeezed reservoirs is investigated in the context of matching of the correlations contained in the entangled states to those contained in the squeezed reservoir. We illustrate our considerations by examining the time evolution of entanglement of single and double excitation NOON and EPR states. A comparison is made when each cavity is coupled to own reservoir or both cavities are coupled to a common reservoir. It is shown that the evolution of the initial entanglement and transfer of entanglement from the squeezed reservoir to the cavity modes depend crucially on the matching of the initial correlations to that contained in the squeezed reservoir. In particular, it is found that initially entangled modes with correlations different from the reservoir correlations prevent the transfer of the correlations from the squeezed field to the modes. In addition, we find that the transient entanglement exhibits several features unique to quantum nature of squeezing. In particular, we show that in the case of separate squeezed reservoirs a variation of the decay time of the initial entanglement with the squeezing phase is unique to quantum squeezing. In the case of a common reservoir a recurrence of entanglement occurs and we find that this feature also results from the reservoir correlations unique to quantum squeezing. There is no revival of entanglement when the modes interact with a classically squeezed field.

quant-ph↗