Transverse energy redistribution upon edge diffraction of a paraxial laser beam with optical vortex

Author(s):  
Aleksandr Bekshaev ◽  
Kadhim Ameen Mohammed
2014 ◽  
Vol 53 (10) ◽  
pp. B27 ◽  
Author(s):  
Aleksandr Ya. Bekshaev ◽  
Kadhim A. Mohammed ◽  
Ivan A. Kurka

1999 ◽  
Author(s):  
Lyubov V. Kreminskaya ◽  
R. Amezquita ◽  
Vladimir B. Markov ◽  
Freddy A. Monroy ◽  
G. Arenas ◽  
...  
Keyword(s):  

2021 ◽  
Vol 11 (16) ◽  
pp. 7677
Author(s):  
Ewa Frączek ◽  
Wojciech Frączek ◽  
Agnieszka Popiołek-Masajada

We propose the use of high-order optical vortices as markers in the positioning of a laser beam. The broken optical vortices are arranged in constellations. The center of gravity of these constellations makes it possible to position the beam carrying information encoded in the optical vortices. This paper describes three positioning methods using both intensity and phase maps. The methods described were tested in experiments performed in a laboratory and an open space.


2000 ◽  
Vol 123 (4) ◽  
pp. 609-614 ◽  
Author(s):  
A. F. H. Kaplan ◽  
G. Groboth

The technology of laser beam cladding of metals by single-step powder delivery is analyzed with a process model which is based on balance equations of energy and mass. Effects like powder heating, clad layer formation, substrate dilution and overlapping of tracks are discussed in dependence of the process parameters. In particular, the powder catchment efficiency and the beam energy redistribution in the material can be optimized by the powder mass flow rate and by the geometrical properties of the beam and of the powder jet.


2015 ◽  
Author(s):  
Aleksey Chernykh ◽  
Aleksandr Bekshaev ◽  
Anna Khoroshun ◽  
Lidiya Mikhaylovskaya ◽  
Aleksandr Akhmerov ◽  
...  

2015 ◽  
Vol 63 (2) ◽  
pp. 164-176 ◽  
Author(s):  
Ljiljana Janicijevic ◽  
Suzana Topuzoski

2021 ◽  
Vol 45 (1) ◽  
pp. 13-18
Author(s):  
A.G. Nalimov ◽  
S.S. Stafeev

We have shown that when sharply focusing a linearly polarized optical vortex with topological charge 2, in the near-axis region of the focal plane, not only does a reverse energy flow (the negative on-axis projection of the Poynting vector) occur, but also the right-handed circular polariza-tion of light. Moreover, due to spin-orbital angular momentum conversion, the on-axis polarization vector and the transverse energy flow rotate around the optical axis in the same direction (counter-clockwise). If an absorbing spherical microparticle is put in the focus on the optical axis, it will rotate around the axis and around its center of mass counterclockwise. Numerical simulation results confirms the theoretical predictions.


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