scholarly journals Fourier-Bessel beams of finite energy

2021 ◽  
Vol 45 (4) ◽  
pp. 506-511
Author(s):  
V.V. Kotlyar ◽  
A.A. Kovalev ◽  
D.S. Kalinkina ◽  
E.S. Kozlova

In this paper, we consider a new type of Bessel beams having Fourier-invariance property and, therefore, called Fourier-Bessel beams. In contrast to the known Bessel beams, these beams have weak side lobes. Analytical expressions for the complex amplitude of the proposed field in the initial plane of the source and in the far field region have been obtained. It is shown that the proposed Fourier-Bessel beams have a finite energy, although they do not have a Gaussian envelope. Their complex amplitude is proportional to a fractional-order Bessel function (an odd integer divided by 6) in the initial plane and in the Fraunhofer zone. The Fourier-Bessel modes have a smaller internal dark spot compared to the Laguerre-Gauss modes with a zero radial index. The proposed beams can be generated with a spatial light modulator and may find uses in telecommunications, interferometry, and the capture of metal microparticles.

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Lyubomir Stoyanov ◽  
Maya Zhekova ◽  
Aleksander Stefanov ◽  
Ivan Stefanov ◽  
Gerhard G. Paulus ◽  
...  

AbstractWe demonstrate an alternative approach for generating zeroth- and first-order long range non-diffracting Gauss–Bessel beams (GBBs). Starting from a Gaussian beam, the key point is the creation of a bright ring-shaped beam with a large radius-to-width ratio, which is subsequently Fourier-transformed by a thin lens. The phase profile required for creating zeroth-order GBBs is flat and helical for first-order GBBs with unit topological charge (TC). Both the ring-shaped beam and the required phase profile can be realized by creating highly charged optical vortices by a spatial light modulator and annihilating them by using a second modulator of the same type. The generated long-range GBBs are proven to have negligible transverse evolution up to 2 m and can be regarded as non-diffracting. The influences of the charge state of the TCs, the propagation distance behind the focusing lens, and the GBB profiles on the relative intensities of the peak/rings are discussed. The method is much more efficient as compared to this using annular slits in the back focal plane of lenses. Moreover, at large propagation distances the quality of the generated GBBs significantly surpasses this of GBBs created by low angle axicons. The developed analytical model reproduces the experimental data. The presented method is flexible, easily realizable by using a spatial light modulator, does not require any special optical elements and, thus, is accessible in many laboratories.


1994 ◽  
Vol 19 (16) ◽  
pp. 1228 ◽  
Author(s):  
Gary D. Sharp ◽  
Kristina M. Johnson

CLEO: 2014 ◽  
2014 ◽  
Author(s):  
G. A. Hine ◽  
A. J. Goers ◽  
S. J. Yoon ◽  
J. A. Elle ◽  
H. M. Milchberg

2006 ◽  
Vol 14 (12) ◽  
pp. 5581 ◽  
Author(s):  
Jonathan Leach ◽  
Graham M. Gibson ◽  
Miles J. Padgett ◽  
Elric Esposito ◽  
Gail McConnell ◽  
...  

2012 ◽  
Vol 285 (1) ◽  
pp. 5-12 ◽  
Author(s):  
Angela Dudley ◽  
Ruslan Vasilyeu ◽  
Vladimir Belyi ◽  
Nikolai Khilo ◽  
Piotr Ropot ◽  
...  

2012 ◽  
Author(s):  
Adriaan Hendriks ◽  
Darryl Naidoo ◽  
Filippus S. Roux ◽  
Carlos López-Mariscal ◽  
Andrew Forbes

Sensors ◽  
2020 ◽  
Vol 20 (14) ◽  
pp. 3850 ◽  
Author(s):  
Svetlana N. Khonina ◽  
Sergey V. Karpeev ◽  
Alexey P. Porfirev

We propose a new type of a wavefront aberration sensor, that is, a Zernike matched multichannel diffractive optical filter, which performs consistent filtering of phase distributions corresponding to Zernike polynomials. The sensitivity of the new sensor is theoretically estimated. Based on the theory, we develop recommendations for its application. Test wavefronts formed using a spatial light modulator are experimentally investigated. The applicability of the new sensor for the fine-tuning of a laser collimator is assessed.


2011 ◽  
Vol 31 (s1) ◽  
pp. s100205
Author(s):  
陈君 Chen Jun ◽  
赵星 Zhao Xing ◽  
方志良 Fang Zhiliang

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