Optical Vortex Laser

A special issue of Photonics (ISSN 2304-6732). This special issue belongs to the section "Lasers, Light Sources and Sensors".

Deadline for manuscript submissions: 31 August 2024 | Viewed by 822

Special Issue Editor

Research Center for Physics of 2D Opto-Electronic Materials and Devices, School of Physics and Electronics, Henan University, Kaifeng 475004, China
Interests: light field manipulation and nonlinear optics; laser technology and application

Special Issue Information

Dear Colleagues,

Optical vortex beams bearing phase singularities and carrying orbital angular momentum are attracting more people to study from fundamental and applied perspectives, with investigations into optical microscopy, hyper-entanglement, strong coupling between light and matter, optical trapping and optical spanners, classical and quantum communications, etc. On the basis of the number of phase singularities in optical vortex beams, they can mainly be divided into two categories: on-axis single singularity optical vortex beams and multi-singularity optical vortex beam. The multi-singularity optical vortex beam can be further subdivided into two types: optical vortex arrays and optical vortex lattices.

At present, optical vortex beams are mainly generated through passive and active methods. Compared to the passive method of external cavity mode transformation, the active method has significant advantages in conversion, beam quality (mode purity), and power improvement. This Special Issue aims to present original state-of-the-art research articles dealing with vortex laser generated with active method, including off-axis pumping method, annular pumping method, intracavity spherical aberration method, etc. Specifically, papers are also solicited that deal with vortex lasers coupled to various kinds of nonlinear frequency conversion, such as second harmonic generation, sum-frequency generation, optical parametric oscillation, and Raman processes, and so on. Researchers are invited to submit their contributions to this Special Issue. Topics include, but are not limited to:

  • Scalar vortex laser;
  • Vector vortex laser;
  • Vortex arrays laser;
  • Vortex lattices laser;
  • Raman vortex laser;
  • Intra-cavity frequency-doubled/sum-frequency generation vortex laser;
  • Intra-cavity optical parametric vortex laser;
  • Cascaded-pumped vortex laser;
  • Vortex random fiber laser;
  • Kaleidoscope vortex laser.

Dr. Peng Li
Guest Editor

Manuscript Submission Information

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Keywords

  • scalar vortex laser
  • vector vortex laser
  • vortex arrays laser
  • vortex lattices laser
  • raman vortex laser
  • intra-cavity frequency-doubled/sum-frequency generation vortex laser
  • intra-cavity optical parametric vortex laser
  • cascaded-pumped vortex laser
  • vortex random fiber laser
  • kaleidoscope vortex laser

Published Papers (1 paper)

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Research

10 pages, 2466 KiB  
Communication
Study on the Generation of 1.9 μm Mode Superposition Conversion Laser by Double-End Off-Axis Pumping
by Chao Li, Xinyu Chen, Ye Sun, Jingliang Liu and Guangyong Jin
Photonics 2024, 11(3), 210; https://doi.org/10.3390/photonics11030210 - 26 Feb 2024
Viewed by 613
Abstract
In this paper, the Laguerre–Gaussian (LG) mode superposition is obtained by using the technology of double-end off-axis pumping Tm:YLF crystal, and the LG mode superposition is achieved by combining the extra-cavity conversion method. The impact of changing the off-axis distance on the order [...] Read more.
In this paper, the Laguerre–Gaussian (LG) mode superposition is obtained by using the technology of double-end off-axis pumping Tm:YLF crystal, and the LG mode superposition is achieved by combining the extra-cavity conversion method. The impact of changing the off-axis distance on the order of Hermite–Gaussian (HG) mode and the topological charge of LG mode is studied. The results show that when the off-axis distance of the pump source at both ends is tuned, when the off-axis distance is in the range of 260 μm~845 μm, the single-ended 0~10 order HG mode can be obtained. Subsequently, the mode converter is placed to obtain the LG mode beam, and the double-end simultaneously pumps the crystal to obtain the superimposed LG mode. The tuning off-axis quantity changes the topological charge number. When P = 0, l1=l2, the superimposed LG mode is a single-ring spot, and the vortex beam center’s dark hollow area increases with the topological charge number. When P = 0, l1=l2, the superimposed LG mode is a petal-like spot. The number of petals differs from the topological charges of two opposite numbers. Finally, in the case of changing the topological charge number of the double-ended LG mode, the output of the vortex array structured beams of the tuning mode order 1.9 μm Tm:YLF is completed in the case of conversion and superposition. Full article
(This article belongs to the Special Issue Optical Vortex Laser)
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Planned Papers

The below list represents only planned manuscripts. Some of these manuscripts have not been received by the Editorial Office yet. Papers submitted to MDPI journals are subject to peer-review.

Planned Paper

Tentative Title: Generating Optical Vortex Array Laser Beams with a Dual-Phase Modulation Digital Laser System

Authorship: Ly Ly Nguyen Thi, Ko-Fan Tsai, and Shu-Chun Chu*

Affiliations: Department of Physics, National Cheng Kung University, No. 1, University Road, Tainan City 701, Taiwan; *[email protected]

Abstract:

This study presents an efficient and practical intra-cavity approach for selectively generating vortex array laser beams using a dual-phase modulation digital laser system. The stable optical vortex array laser beams are formed by superimposing cavity Hermite-Gaussian (HG) eigenmodes. In particular, when the selected cavity HG modes share the same Gouy phase, the resulting optical vortex beam can preserve its light field pattern, thereby maintaining the optical vortex properties in both the near and far fields. Numerical results demonstrate that employing dual-phase modulation establishes optimal boundary conditions for selecting HG modes within the cavity, leading to successful generation of various vortex array laser beams, such as 1D vortex array laser and checkerboard-distributed vortex array laser. Experimental validation of the proposed method confirms the ability to select optical vortex array lasers solely through the control of the loaded phase of the dual-phase modulation digital laser. The results demonstrate the ability of digital lasers for dynamically controlling and generating optical vortex array lasers.

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