Third-order orbital angular momentum pulse generation from a passively Q-switched fiber laser

We propose and demonstrate an all-fiber passively Q-switched laser generating a third-order orbital angular momentum (OAM) pulse by introducing a few-mode long-period fiber grating (LPFG) into the laser cavity. The LPFG with asymmetric cross structure and strong refractive index modulation overcomes...

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Bibliographic Details
Main Authors: Du, C. (Author), Gao, S. (Author), Li, W. (Author), Li, Z. (Author), Liu, W. (Author), Tu, J. (Author), Wen, T. (Author), Xiao, R. (Author), Zhang, B. (Author), Zhou, J. (Author)
Format: Article
Language:English
Published: Optica Publishing Group (formerly OSA) 2022
Subjects:
Online Access:View Fulltext in Publisher
LEADER 02461nam a2200493Ia 4500
001 10.1364-OE.454147
008 220425s2022 CNT 000 0 und d
020 |a 10944087 (ISSN) 
245 1 0 |a Third-order orbital angular momentum pulse generation from a passively Q-switched fiber laser 
260 0 |b Optica Publishing Group (formerly OSA)  |c 2022 
300 |a 10 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1364/OE.454147 
520 3 |a We propose and demonstrate an all-fiber passively Q-switched laser generating a third-order orbital angular momentum (OAM) pulse by introducing a few-mode long-period fiber grating (LPFG) into the laser cavity. The LPFG with asymmetric cross structure and strong refractive index modulation overcomes the coupling issue between the fundamental and the third-azimuthal-order (LP31 or OAM3) modes and realizes their direct conversion. A homemade graphene-based saturable absorber is used to realize Q-switched operation. The laser operates at a center wavelength of 1548.2nm, with a 3 dB spectral bandwidth of 0.4nm, and the OAM+3 and OAM−3 beams can achieve the purity of 90.0% and 90.2%, respectively. This all-fiber Q-switched laser has simple and compact structure and high purity of OAM±3 beams, which has potential applications in the fields of optical tweezers and material processing. © 2022 Optica Publishing Group under the terms of the Optica Open Access Publishing Agreement Journal © 2022 
650 0 4 |a All fiber 
650 0 4 |a Angular momentum 
650 0 4 |a Cross structures 
650 0 4 |a Diffraction gratings 
650 0 4 |a Fiber lasers 
650 0 4 |a Fibers 
650 0 4 |a Graphene 
650 0 4 |a Long-period fibre gratings 
650 0 4 |a Optical tweezers 
650 0 4 |a Orbital angular momentum 
650 0 4 |a Passively Q-switched 
650 0 4 |a Passively Q-switched lasers 
650 0 4 |a Pulse generation 
650 0 4 |a Q switched lasers 
650 0 4 |a Q switching 
650 0 4 |a Q-switched fiber lasers 
650 0 4 |a Refractive index 
650 0 4 |a Refractive-index modulation 
650 0 4 |a Saturable absorbers 
650 0 4 |a Third order 
700 1 |a Du, C.  |e author 
700 1 |a Gao, S.  |e author 
700 1 |a Li, W.  |e author 
700 1 |a Li, Z.  |e author 
700 1 |a Liu, W.  |e author 
700 1 |a Tu, J.  |e author 
700 1 |a Wen, T.  |e author 
700 1 |a Xiao, R.  |e author 
700 1 |a Zhang, B.  |e author 
700 1 |a Zhou, J.  |e author 
773 |t Optics Express