• Infrared and Laser Engineering
  • Vol. 49, Issue 12, 20201061 (2020)
Sha Wang1, Zhicheng Zhang1, Guoliang Deng1、*, and Shouhuan Zhou2
Author Affiliations
  • 1College of Electronics and Information Engineering, Sichuan University, Chengdu 610064, China
  • 2College of Electronics and Information Engineering, Sichuan University, Chengdu 610064, China
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    DOI: 10.3788/IRLA20201061 Cite this Article
    Sha Wang, Zhicheng Zhang, Guoliang Deng, Shouhuan Zhou. Research progress on direct generation of ultrashort pulse OAM vortex beams (Invited)[J]. Infrared and Laser Engineering, 2020, 49(12): 20201061 Copy Citation Text show less

    Abstract

    Orbital angular momentum (OAM) vortex beam has a phase singularity with a twisted wave-front, whose complex amplitude comprises the helical term exp (ilθ). OAM vortex beam has been widely used in optical manipulation, imaging, optical communication, sensing and so on. Ultra-short pulse OAM vortex beams have the advantages of both vortex beams and ultra-short pulses, and can be applied to chiral material processing, long distance transmission, strong field physics and nonlinear frequency conversion. Direct generation of ultra-short OAM vortex beams has the advantages of compact and simple system and good beam quality. The research progress on direct generation of ultra-short OAM vortex beams was summarized. At present, the pulse width of the ultra-short OAM vortex beam generated by the active method is still limited to a few hundred femtoseconds. How to obtain the pulsed vortex beam output within 100 femtoseconds or even with a few cycles through the direct output method will be an important future development direction.
    $\begin{split} \left\{ {\begin{array}{*{20}{c}} {\hat x{L_{ \pm l,m}}} \\ {\hat y{L_{ \pm l,m}}} \end{array}} \right\} =& \left\{ {\begin{array}{*{20}{c}} {LP_{l,m}^{c,x} \pm iLP_{l,m}^{s,x}} \\ {LP_{l,m}^{c,y} \pm iLP_{l,m}^{s,y}} \end{array}} \right\} = {F_{l,m}}(r)\left\{ {\begin{array}{*{20}{c}} {\hat x\exp ( \pm il\varphi )} \\ {\hat y\exp ( \pm il\varphi )} \end{array}} \right\},\\ &(l \geqslant 1)\\ \end{split} $(1)

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    $\begin{split} \left\{ {\begin{array}{*{20}{c}} {V_{ \pm l,m}^ \pm } \\ {V_{ \pm l,m}^ \mp } \end{array}} \right\} =& \left\{ {\begin{array}{*{20}{c}} {HE_{l + 1,m}^e \pm iHE_{l + 1,m}^o} \\ {EH_{l - 1}^e \pm iEH_{l - 1,m}^o} \end{array}} \right\} =\\ &{F_{l,m}}(r)\left\{ {\begin{array}{*{20}{c}} {{{\hat \sigma }^ \pm }\exp ( \pm il\varphi ),(l \geqslant 1)} \\ {{{\hat \sigma }^ \mp }\exp ( \pm il\varphi ),(l > 1)} \end{array}} \right\} \end{split}$(2)

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    Sha Wang, Zhicheng Zhang, Guoliang Deng, Shouhuan Zhou. Research progress on direct generation of ultrashort pulse OAM vortex beams (Invited)[J]. Infrared and Laser Engineering, 2020, 49(12): 20201061
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