scholarly journals Deformation of Optical Vortex Beam by Displacement of Incident-Beam Optical Axis from Spiral Phase Plate Center

2021 ◽  
pp. 100076
Author(s):  
Miki Kitazawa ◽  
Kyoko Kitamura ◽  
Shogo Ura
2016 ◽  
Vol 53 (9) ◽  
pp. 092602
Author(s):  
郭苗军 Guo Miaojun ◽  
曾军 Zeng Jun ◽  
李晋红 Li Jinhong

2013 ◽  
Vol 19 (S2) ◽  
pp. 1168-1169
Author(s):  
A.M. Blackburn ◽  
J.C. Loudon

Extended abstract of a paper presented at Microscopy and Microanalysis 2013 in Indianapolis, Indiana, USA, August 4 – August 8, 2013.


Photonics ◽  
2020 ◽  
Vol 7 (3) ◽  
pp. 60
Author(s):  
Ireneusz Augustyniak ◽  
Weronika Lamperska ◽  
Jan Masajada ◽  
Łukasz Płociniczak ◽  
Agnieszka Popiołek-Masajada

The analytical solution for the propagation of the laser beam with optical vortex through the system of lenses is presented. The optical vortex is introduced into the laser beam (described as Gaussian beam) by spiral phase plate. The solution is general as it holds for the optical vortex of any integer topological charge, the off-axis position of the spiral phase plate and any number of lenses. Some intriguing conclusions are discussed. The higher order vortices are unstable and split under small phase or amplitude disturbance. Nevertheless, we have shown that off-axis higher order vortices are stable during the propagation through the set of lenses described in paraxial approximation, which is untypical behavior. The vortex trajectory registered at image plane due to spiral phase plate shift behaves like a rigid body. We have introduced a new factor which in our beam plays the same role as Gouy phase in pure Gaussian beam.


2018 ◽  
Vol 42 (2) ◽  
pp. 212-218
Author(s):  
V. V. Kotlyar ◽  
A. A. Kovalev

We obtain a simple formula for the relative total orbital angular momentum (OAM) of a paraxial light beam with arbitrary rotationally symmetric complex amplitude passed through a spiral phase plate (SPP) whose center is shifted from the optical axis. The formula shows that the OAM equals zero if the incident beam is bounded by an aperture and the SPP center is outside this aperture. For the incident beam bounded by an annular aperture, there is another interesting consequence of the obtained expression. The total OAM of such a beam is the same regardless of the position of the SPP center within the shaded circle of the aperture. Thus, it would be appropriate to illuminate the SPP by beams with an annular intensity distribution, since in this case an inaccurate alignment of the SPP center and the center of the annular intensity distribution does not affect the total OAM of the beam. We also obtain an expression for the OAM density of such a beam in the initial plane.


Sign in / Sign up

Export Citation Format

Share Document