Focal Pattern of Hyperbolic-Cosine-Gaussian Beam with Optical Vortex

Author(s):  
Xiumin Gao ◽  
Qiufang Zhan ◽  
Jinsong Li ◽  
Jian Wang ◽  
Songlin Zhuang
2011 ◽  
Vol 42 (6-7) ◽  
pp. 367-380 ◽  
Author(s):  
Xiumin Gao ◽  
Qi Wang ◽  
Qiufang Zhan ◽  
Maojin Yun ◽  
Hanming Guo ◽  
...  

2011 ◽  
Author(s):  
Ireneusz Augustyniak ◽  
Agnieszka Popiolek-Masajada ◽  
Jan Masajada

2011 ◽  
Vol 13 (3) ◽  
pp. 035714 ◽  
Author(s):  
J Masajada ◽  
M Leniec ◽  
I Augustyniak
Keyword(s):  

Nanoscale ◽  
2020 ◽  
Vol 12 (12) ◽  
pp. 6673-6690 ◽  
Author(s):  
Tetsuro Tsuji ◽  
Ryoji Nakatsuka ◽  
Kichitaro Nakajima ◽  
Kentaro Doi ◽  
Satoyuki Kawano

We experimentally and theoretically characterize dielectric nano- and microparticle orbital motion induced by an optical vortex of the Laguerre–Gaussian beam and investigate the role of hydrodynamic inter-particle interaction.


2010 ◽  
Vol 48 (7-8) ◽  
pp. 766-773 ◽  
Author(s):  
Xiumin Gao ◽  
Zhuo Li ◽  
Jian Wang ◽  
Lingling Sun ◽  
Songlin Zhuang

2019 ◽  
Vol 43 (3) ◽  
pp. 356-367
Author(s):  
V.V. Kotlyar ◽  
A.A. Kovalev ◽  
A.P. Porfirev

Here we study three different types of astigmatic Gaussian beams, whose complex amplitude in the Fresnel diffraction zone is described by the complex argument Hermite polynomial of the order (n, 0). The first type is a circularly symmetric Gaussian optical vortex with and a topological charge n after passing through a cylindrical lens. On propagation, the optical vortex "splits" into n first-order optical vortices. Its orbital angular momentum per photon is equal to n. The second type is an elliptical Gaussian optical vortex with a topological charge n after passing through a cylindrical lens. With a special choice of the ellipticity degree (1: 3), such a beam retains its structure upon propagation and the degenerate intensity null on the optical axis does not “split” into n optical vortices. Such a beam has fractional orbital angular momentum not equal to n. The third type is the astigmatic Hermite-Gaussian beam (HG) of order (n, 0), which is generated when a HG beam passes through a cylindrical lens. The cylindrical lens brings the orbital angular momentum into the original HG beam. The orbital angular momentum of such a beam is the sum of the vortex and astigmatic components, and can reach large values (tens and hundreds of thousands per photon). Under certain conditions, the zero intensity lines of the HG beam "merge" into an n-fold degenerate intensity null on the optical axis, and the orbital angular momentum of such a beam is equal to n. Using intensity distributions of the astigmatic HG beam in foci of two cylindrical lenses, we calculate the normalized orbital angular momentum which differs only by 7 % from its theoretical orbital angular momentum value (experimental orbital angular momentum is –13,62, theoretical OAM is –14.76).


Sign in / Sign up

Export Citation Format

Share Document