Generation of vortex beams with nonuniform phase jumps in azimuthal locations

The phase angle of the vortex beam along a closed loop centered on the optical singularity changes by 2 pi l, where l is the number of phase jumps (PJs) from 0 to 2 pi and indicates the topological charge of the vortex beam. In this paper, the generation and specification of a new type of vortex beam, in which their PJs are asymmetrically embedded in the phase pattern, are reported. In contrast to Laguerre-Gaussian vortex beams, where PJs are equally spaced azimuthally around the optical singularity, the presented vortex beams have PJs embedded at arbitrary azimuthal angles. By designing a particular forked grating and displaying it on a spatial light modulator, this type of vortex beam is experimentally generated. As with conventional forked grating, the designed grating produces vortex beams with the opposite orbital angular momentum (OAM) sign in the first diffraction order. By measuring the relative orientation of the intensity profile of these OAM beams in the first diffraction order, the position of the PJs on the wavefront of a vortex beam with l = 2 can be determined. This type of vortex beam could have potential applications in various fields of photonics, especially in optical communications based on optical vortices.

Automated summary

In this paper, a new type of vortex beam with asymmetrically embedded phase jumps is reported. By designing a specific forked grating and displaying it on a spatial light modulator, this type of vortex beam is experimentally generated. The position of the phase jumps on the wavefront of the vortex beam can be determined by measuring the relative orientation of the intensity profile of the opposite orbital angular momentum (OAM) beams in the first diffraction order.